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		<id>https://chemwiki.ch.ic.ac.uk/index.php?title=MO_hyc116&amp;diff=732672</id>
		<title>MO hyc116</title>
		<link rel="alternate" type="text/html" href="https://chemwiki.ch.ic.ac.uk/index.php?title=MO_hyc116&amp;diff=732672"/>
		<updated>2018-05-25T15:45:19Z</updated>

		<summary type="html">&lt;p&gt;Hyc116: /* Aromaticity: discussion */&lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;==BH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;==&lt;br /&gt;
&lt;br /&gt;
===standard information===&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;Calculation type&amp;lt;/b&amp;gt;: Optimisation&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;Calculation Method&amp;lt;/b&amp;gt;: B3LYP&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;Basis set&amp;lt;/b&amp;gt;: 6-31G(d,p) &lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Summary table&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
[[file:Hyc116_bh3_631g_opt_summarytable.png]]&lt;br /&gt;
&lt;br /&gt;
The above summary table was obtained after the 2nd optimisation of BH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt; (after the initial optimisation using the 3-21G basis set). Notice how the symmetry is incorrect and shown as Cs. This is because the symmetry was manually broken at the beginning by changing the bond length of B-H bonds. The point group was manually adjusted and the molecule was optimised again before the frequency analysis and the new summary table is attached below.&lt;br /&gt;
&lt;br /&gt;
[[file:Hyc116_bh3_correctsummarytable.png]]&lt;br /&gt;
&lt;br /&gt;
The above summary table was obtained from the optimisation after adjusting the symmetry. The point shown in this summary table is D&amp;lt;sub&amp;gt;3h&amp;lt;/sub&amp;gt;, which is the correct for BH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;. &lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Items table&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
Below is the items table taken from the optimisation with the correct point group.&lt;br /&gt;
&lt;br /&gt;
&amp;lt;pre&amp;gt;&lt;br /&gt;
Item               Value     Threshold  Converged?&lt;br /&gt;
 Maximum Force            0.000015     0.000450     YES&lt;br /&gt;
 RMS     Force            0.000010     0.000300     YES&lt;br /&gt;
 Maximum Displacement     0.000058     0.001800     YES&lt;br /&gt;
 RMS     Displacement     0.000038     0.001200     YES&lt;br /&gt;
&amp;lt;/pre&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Frequency log file&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
[[Media:HYC116 BH3 FREQ.LOG]] &lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Frequencies&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;pre&amp;gt;&lt;br /&gt;
Low frequencies ---  -10.3498   -3.4492   -1.2454   -0.0055    0.4779    3.2165&lt;br /&gt;
Low frequencies --- 1162.9519 1213.1527 1213.1554&lt;br /&gt;
&amp;lt;/pre&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;jmol of BH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;&#039;&#039;&#039;&lt;br /&gt;
&amp;lt;jmol&amp;gt;&amp;lt;jmolApplet&amp;gt;&lt;br /&gt;
  &amp;lt;title&amp;gt;optimised BH3&amp;lt;/title&amp;gt;&lt;br /&gt;
  &amp;lt;color&amp;gt;black&amp;lt;/color&amp;gt;&lt;br /&gt;
  &amp;lt;size&amp;gt;200&amp;lt;/size&amp;gt;&lt;br /&gt;
  &amp;lt;uploadedFileContents&amp;gt;HYC116_BH3_FREQ.LOG&amp;lt;/uploadedFileContents&amp;gt;&lt;br /&gt;
&amp;lt;/jmolApplet&amp;gt;&amp;lt;/jmol&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
===Vibrational spectrum===&lt;br /&gt;
&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot;&lt;br /&gt;
!wavenumber (cm&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;)&lt;br /&gt;
!Intensity (arbitrary units)&lt;br /&gt;
!symmetry&lt;br /&gt;
!IR active?&lt;br /&gt;
!type&lt;br /&gt;
|-&lt;br /&gt;
|1163&lt;br /&gt;
|93&lt;br /&gt;
|A&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;&#039; &#039;&lt;br /&gt;
|Yes&lt;br /&gt;
|Out of plane bend&lt;br /&gt;
|-&lt;br /&gt;
|1213&lt;br /&gt;
|14&lt;br /&gt;
|E&#039;&lt;br /&gt;
|Very slight&lt;br /&gt;
|Bend&lt;br /&gt;
|-&lt;br /&gt;
|1213&lt;br /&gt;
|14&lt;br /&gt;
|E&#039;&lt;br /&gt;
|Very slight&lt;br /&gt;
|Bend&lt;br /&gt;
|-&lt;br /&gt;
|2582&lt;br /&gt;
|0&lt;br /&gt;
|A&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;&#039;&lt;br /&gt;
|No&lt;br /&gt;
|Symmetric stretch&lt;br /&gt;
|-&lt;br /&gt;
|2716&lt;br /&gt;
|126&lt;br /&gt;
|E&#039;&lt;br /&gt;
|Yes&lt;br /&gt;
|Asymmetric stretch&lt;br /&gt;
|-&lt;br /&gt;
|2716&lt;br /&gt;
|126&lt;br /&gt;
|E&#039;&lt;br /&gt;
|Yes&lt;br /&gt;
|Asymmetric stretch&lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;IR spectrum&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
[[file:Hyc116_ir_bh3.png|400*600]]&lt;br /&gt;
&lt;br /&gt;
There are only three peaks on the IR spectrum of BH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;, despite that there are 6 vibrational modes for the molecule. As shown in the table above, the symmetric stretching mode with A1 symmetry at 2582 cm&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt; is not IR active; naturally, that vibrational mode doesn’t give a peak on the IR spectrum. As shown from the table, two pairs of vibrational modes, the bond angle deformation/bend at 1213 cm&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt; and the asymmetric bond stretch at 2716 cm&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;, are degenerate with the symmetry label E. This means that they have the same energy, and hence give the same wavenumber on the IR spectrum. Each pair of degenerate vibrational modes give rise to one peak. This leaves three peaks, as confirmed by the IR spectrum above.&lt;br /&gt;
&lt;br /&gt;
===Molecular orbitals of BH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;===&lt;br /&gt;
&lt;br /&gt;
[[file:hyc116_bh3_MO_diagram.png]]&lt;br /&gt;
&lt;br /&gt;
The above molecular orbital diagram was taken from Dr Patricia Hunt&#039;s &amp;lt;i&amp;gt;Lecture 4 Tutorial Problem Model Answers&amp;lt;/i&amp;gt;.&amp;lt;ref&amp;gt;P. Hunt, &amp;quot;Lecture 4 Tutorial Problem Model Answers&amp;quot;, 2 (2018)&amp;lt;/ref&amp;gt; Diagrams of the &amp;quot;real&amp;quot; MOs were obtained from Gaussian.&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
There is no significant difference between the LCAO MOs and the real ones. Features such as orbital phases are shown clearly on both the LCAO MOs and the real MOs, illustrating the bonding/anti-bonding characters of the molecular orbitals. This suggests that the the qualitative MO theory is highly accurate and useful when studying the molecular orbitals of molecules.&lt;br /&gt;
&lt;br /&gt;
==Associated energies: ammonium borane==&lt;br /&gt;
&lt;br /&gt;
===NH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;===&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;Calculation type&amp;lt;/b&amp;gt;: Optimisation&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;Calculation Method&amp;lt;/b&amp;gt;: B3LYP&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;Basis set&amp;lt;/b&amp;gt;: 6-31G(d,p) &lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Summary table&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
[[file:Hyc116_nh3_631g_summarytable.png]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Items table&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;pre&amp;gt;&lt;br /&gt;
Item               Value     Threshold  Converged?&lt;br /&gt;
 Maximum Force            0.000006     0.000450     YES&lt;br /&gt;
 RMS     Force            0.000004     0.000300     YES&lt;br /&gt;
 Maximum Displacement     0.000012     0.001800     YES&lt;br /&gt;
 RMS     Displacement     0.000008     0.001200     YES&lt;br /&gt;
&amp;lt;/pre&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Frequency log file&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
[[Media:HYC116_NH3_FREQ.LOG]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Frequencies&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;pre&amp;gt;&lt;br /&gt;
Low frequencies ---   -8.5646   -8.5588   -0.0047    0.0454    0.1784   26.4183&lt;br /&gt;
Low frequencies --- 1089.7603 1694.1865 1694.1865&lt;br /&gt;
&amp;lt;/pre&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;jmol of NH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;&#039;&#039;&#039;&lt;br /&gt;
&amp;lt;jmol&amp;gt;&amp;lt;jmolApplet&amp;gt;&lt;br /&gt;
  &amp;lt;title&amp;gt;optimised NH3&amp;lt;/title&amp;gt;&lt;br /&gt;
  &amp;lt;color&amp;gt;black&amp;lt;/color&amp;gt;&lt;br /&gt;
  &amp;lt;size&amp;gt;200&amp;lt;/size&amp;gt;&lt;br /&gt;
  &amp;lt;uploadedFileContents&amp;gt;HYC116_NH3_FREQ.LOG&amp;lt;/uploadedFileContents&amp;gt;&lt;br /&gt;
&amp;lt;/jmolApplet&amp;gt;&amp;lt;/jmol&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
===NH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;BH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;===&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;Calculation type&amp;lt;/b&amp;gt;: Optimisation&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;Calculation Method&amp;lt;/b&amp;gt;: B3LYP&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;Basis set&amp;lt;/b&amp;gt;: 6-31G(d,p) &lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Summary table&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
[[file:Hyc116_nh3bh3_631g_summarytable1.png]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Items table&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;pre&amp;gt;&lt;br /&gt;
Item               Value     Threshold  Converged?&lt;br /&gt;
 Maximum Force            0.000121     0.000450     YES&lt;br /&gt;
 RMS     Force            0.000057     0.000300     YES&lt;br /&gt;
 Maximum Displacement     0.000501     0.001800     YES&lt;br /&gt;
 RMS     Displacement     0.000293     0.001200     YES&lt;br /&gt;
&amp;lt;/pre&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Frequency log file&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
[[Media:HYC116_NH3BH3_FREQ1.LOG]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Frequencies&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;pre&amp;gt;&lt;br /&gt;
Low frequencies ---   -0.0574   -0.0501   -0.0074   21.6276   21.6377   40.3839&lt;br /&gt;
Low frequencies ---  265.9973  632.3725  640.1275&lt;br /&gt;
&amp;lt;/pre&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;jmol of NH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;BH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;&#039;&#039;&#039;&lt;br /&gt;
&amp;lt;jmol&amp;gt;&amp;lt;jmolApplet&amp;gt;&lt;br /&gt;
  &amp;lt;title&amp;gt;optimised NH3BH3&amp;lt;/title&amp;gt;&lt;br /&gt;
  &amp;lt;color&amp;gt;black&amp;lt;/color&amp;gt;&lt;br /&gt;
  &amp;lt;size&amp;gt;200&amp;lt;/size&amp;gt;&lt;br /&gt;
  &amp;lt;uploadedFileContents&amp;gt;HYC116_NH3BH3_FREQ.LOG&amp;lt;/uploadedFileContents&amp;gt;&lt;br /&gt;
&amp;lt;/jmolApplet&amp;gt;&amp;lt;/jmol&amp;gt;&lt;br /&gt;
&lt;br /&gt;
===Association energy===&lt;br /&gt;
&lt;br /&gt;
E(BH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;) (using the optimisation with the correct symmetry) = -26.61532363 a.u. = &amp;lt;b&amp;gt;-26.61532 a.u. (5 d.p.)&amp;lt;/b&amp;gt;&lt;br /&gt;
&lt;br /&gt;
E(NH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;) = -56.55776873 a.u. = &amp;lt;b&amp;gt;-56.55777 a.u. (5 d.p.)&amp;lt;/b&amp;gt;&lt;br /&gt;
&lt;br /&gt;
E(NH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;BH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;) = -83.22468892 a.u. = &amp;lt;b&amp;gt;-83.22469 a.u. (5 d.p.)&amp;lt;/b&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
Carrying out calculations using numbers which has already been rounded up can possibly result in errors in the last digit. Hence, here the calculations were carried out using the numbers provided from the optimisations (i.e. with more decimal places than necessary); the answer was then rounded up to the desired accuracy. &lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
ΔE = E(NH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;BH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;)-[E(NH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;)+E(BH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;)]&lt;br /&gt;
&lt;br /&gt;
ΔE = -83.22468892 - (-56.55776873 + -26.61532363) = -0.05159656 a.u. &lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;ΔE = -0.05160 a.u. (5 d.p.)&amp;lt;/b&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Converting energy from a.u. to kJ/mol&#039;&#039;&#039;&lt;br /&gt;
An atomic unit for energy is Hartree, which is equal to 2625.5 kJ/mol.&lt;br /&gt;
&amp;lt;ref&amp;gt;https://cccbdb.nist.gov/hartree.asp (Accessed: 22.05.2018)&amp;lt;/ref&amp;gt;&lt;br /&gt;
 &lt;br /&gt;
&lt;br /&gt;
So ΔE in kJ/mol = -0.05159657 * 2625.5 = -135.46676828 kJ/mol&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;ΔE = -135 kJ/mol (nearest integer)&amp;lt;/b&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
The energy difference calculated above comes from the formation of the B-N dative bond. It is a relatively weak bond. According to a bond energy data sheet provided by the University of California,&amp;lt;ref&amp;gt;https://labs.chem.ucsb.edu/zakarian/armen/11---bonddissociationenergy.pdf (Accessed: 24.05.2018)&amp;lt;/ref&amp;gt;  the bond energy of the C-C bond of an ethane molecule is 368 kJ/mol. This is a fair comparison to the NH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;BH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt; molecule as the two molecules have the same structure, only with the carbon atoms on ethane swapped for Boron and Nitrogen in NH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;BH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;&lt;br /&gt;
&lt;br /&gt;
==Using a mixture of basis-sets and pseudo-potentials==&lt;br /&gt;
&lt;br /&gt;
===BBr&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;===&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;Calculation type&amp;lt;/b&amp;gt;: Optimisation&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;Calculation Method&amp;lt;/b&amp;gt;: B3LYP&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;Basis set&amp;lt;/b&amp;gt;: Boron: 6-31G(d,p) ; Br: LANL2DZ&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
Larger calculations are often sent to a web-server to run on a high-performance computer instead of a desktop. In order to experience and learn to use a web-server, the optimisation and the frequency analysis for BBr&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt; were both sent and done on a server instead of the desktop. The calculation results were downloaded from the web-server once they were finished.   &lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Summary table&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
[[file:Hyc116_bbr3_opt_summarytable.png]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Items table&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;pre&amp;gt;&lt;br /&gt;
Item               Value     Threshold  Converged?&lt;br /&gt;
 Maximum Force            0.000008     0.000450     YES&lt;br /&gt;
 RMS     Force            0.000005     0.000300     YES&lt;br /&gt;
 Maximum Displacement     0.000036     0.001800     YES&lt;br /&gt;
 RMS     Displacement     0.000023     0.001200     YES&lt;br /&gt;
&amp;lt;/pre&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Frequency log file&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
[[Media:Hyc116_bbr3_freq.log]]&lt;br /&gt;
&lt;br /&gt;
Attached above is the frequency file saved onto the computer from the SCAN server portal. The frequency file was also published on the chemistry database DSpace. {{DOI|10042/202442}}&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Frequencies&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;pre&amp;gt;&lt;br /&gt;
Low frequencies ---   -0.0137   -0.0064   -0.0046    2.4315    2.4315    4.8421&lt;br /&gt;
Low frequencies ---  155.9631  155.9651  267.7052&lt;br /&gt;
&amp;lt;/pre&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;jmol of BBr&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;&#039;&#039;&#039;&lt;br /&gt;
&amp;lt;jmol&amp;gt;&amp;lt;jmolApplet&amp;gt;&lt;br /&gt;
  &amp;lt;title&amp;gt;optimised BBr3&amp;lt;/title&amp;gt;&lt;br /&gt;
  &amp;lt;color&amp;gt;black&amp;lt;/color&amp;gt;&lt;br /&gt;
  &amp;lt;size&amp;gt;200&amp;lt;/size&amp;gt;&lt;br /&gt;
  &amp;lt;uploadedFileContents&amp;gt;Hyc116_bbr3_freq.log&amp;lt;/uploadedFileContents&amp;gt;&lt;br /&gt;
&amp;lt;/jmolApplet&amp;gt;&amp;lt;/jmol&amp;gt;&lt;br /&gt;
&lt;br /&gt;
==Mini project: Aromaticity==&lt;br /&gt;
&lt;br /&gt;
===Benzene===&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;Calculation type&amp;lt;/b&amp;gt;: Optimisation&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;Calculation Method&amp;lt;/b&amp;gt;: B3LYP&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;Basis set&amp;lt;/b&amp;gt;: 6-31G(d,p) &lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Summary table&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
[[file:Hyc116_c6h6_summarytable.png]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Items table&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;pre&amp;gt;&lt;br /&gt;
Item               Value     Threshold  Converged?&lt;br /&gt;
 Maximum Force            0.000193     0.000450     YES&lt;br /&gt;
 RMS     Force            0.000079     0.000300     YES&lt;br /&gt;
 Maximum Displacement     0.000830     0.001800     YES&lt;br /&gt;
 RMS     Displacement     0.000294     0.001200     YES&lt;br /&gt;
&amp;lt;/pre&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Frequency log file&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
[[Media:HYC116_C6H6_FREQ.LOG]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Frequencies&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;pre&amp;gt;&lt;br /&gt;
Low frequencies ---   -3.5606   -3.5606   -0.0089   -0.0043   -0.0043   10.0905&lt;br /&gt;
Low frequencies ---  413.9582  413.9582  621.1416&lt;br /&gt;
&amp;lt;/pre&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;jmol of C&amp;lt;sub&amp;gt;6&amp;lt;/sub&amp;gt;H&amp;lt;sub&amp;gt;6&amp;lt;/sub&amp;gt;&#039;&#039;&#039;&lt;br /&gt;
&amp;lt;jmol&amp;gt;&amp;lt;jmolApplet&amp;gt;&lt;br /&gt;
  &amp;lt;title&amp;gt;optimised Benzene&amp;lt;/title&amp;gt;&lt;br /&gt;
  &amp;lt;color&amp;gt;black&amp;lt;/color&amp;gt;&lt;br /&gt;
  &amp;lt;size&amp;gt;200&amp;lt;/size&amp;gt;&lt;br /&gt;
  &amp;lt;uploadedFileContents&amp;gt;HYC116_C6H6_FREQ.LOG&amp;lt;/uploadedFileContents&amp;gt;&lt;br /&gt;
&amp;lt;/jmolApplet&amp;gt;&amp;lt;/jmol&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
===Borazine===&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;Calculation type&amp;lt;/b&amp;gt;: Optimisation&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;Calculation Method&amp;lt;/b&amp;gt;: B3LYP&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;Basis set&amp;lt;/b&amp;gt;: 6-31G(d,p) &lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Summary table&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
[[file:Hyc116_borazine_summarytable.png]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Items table&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;pre&amp;gt;&lt;br /&gt;
Item               Value     Threshold  Converged?&lt;br /&gt;
 Maximum Force            0.000085     0.000450     YES&lt;br /&gt;
 RMS     Force            0.000033     0.000300     YES&lt;br /&gt;
 Maximum Displacement     0.000250     0.001800     YES&lt;br /&gt;
 RMS     Displacement     0.000074     0.001200     YES&lt;br /&gt;
&amp;lt;/pre&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Frequency log file&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
[[Media:HYC116_BORAZINE_FREQ.LOG]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Frequencies&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;pre&amp;gt;&lt;br /&gt;
Low frequencies ---  -12.6626  -12.6626   -8.9272   -0.0211   -0.0104   -0.0104&lt;br /&gt;
Low frequencies ---  289.1112  289.1112  403.8613&lt;br /&gt;
&amp;lt;/pre&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;jmol of Borazine&#039;&#039;&#039;&lt;br /&gt;
&amp;lt;jmol&amp;gt;&amp;lt;jmolApplet&amp;gt;&lt;br /&gt;
  &amp;lt;title&amp;gt;optimised Borazine&amp;lt;/title&amp;gt;&lt;br /&gt;
  &amp;lt;color&amp;gt;black&amp;lt;/color&amp;gt;&lt;br /&gt;
  &amp;lt;size&amp;gt;200&amp;lt;/size&amp;gt;&lt;br /&gt;
  &amp;lt;uploadedFileContents&amp;gt;HYC116_BORAZINE_FREQ.LOG&amp;lt;/uploadedFileContents&amp;gt;&lt;br /&gt;
&amp;lt;/jmolApplet&amp;gt;&amp;lt;/jmol&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
===Charge distribution===&lt;br /&gt;
&lt;br /&gt;
An NBO charge analysis was carried out on both the optimised benzene and borazine. Visualisations of the charge distribution are shown in the table below, with the colour range going from -1.102 to 1.102 for both molecule. This large scale was chosen as it allows direct comparison of the charge on any atoms in these two molecules and shows the relative magnitude of charges on all these atoms. Negative charges are shown in red, and positive charges are shown in green. A neutral charge is displayed in black, so the smaller a charge is (positive or negative), the darker its colour representation is. Larger charges are shown in brighter colours. The charges are also displayed on the atoms as numbers with a neutral charge being zero. Negative charges are shown as negative number and positive charges are shown as positive numbers. &lt;br /&gt;
&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot;&lt;br /&gt;
!&lt;br /&gt;
!Benzene&lt;br /&gt;
!Borazine&lt;br /&gt;
|-&lt;br /&gt;
!Visualisation of charge distribution&lt;br /&gt;
|[[File:Hyc116_benzene_charge_distribution1.png|500x500px|thumb|centre|Charge distribution of Benzene visualisation]]&lt;br /&gt;
|[[File:Hyc116_borazine_charge_distribution1.png|500x500px|thumb|centre|Charge distribution of Borazine visualisation]]&lt;br /&gt;
|-&lt;br /&gt;
!Charge &lt;br /&gt;
|Carbon: -0.239&lt;br /&gt;
&lt;br /&gt;
Hydrogen: 0.239&lt;br /&gt;
|Nitrogen: -1.102 &lt;br /&gt;
&lt;br /&gt;
Boron: 0.747&lt;br /&gt;
&lt;br /&gt;
Hydrogen (bonded to N): 0.432&lt;br /&gt;
&lt;br /&gt;
Hydrogen (bonded to B): -0.077&lt;br /&gt;
|-&lt;br /&gt;
!Discussion&lt;br /&gt;
|From the visualisation, it is shown that there is a slightly negative charge on the carbon atoms, and a positive charge of the same magnitude on the hydrogen atoms. All the carbon atoms have the same charge as they are in identical environments. The same applies to all the hydrogen atoms. This is due to the highly symmetrical structure of benzene. Since the same colour scale was used for both benzene and borazine, and the charges are much smaller in magnitude on atoms in benzene than atoms on borazine, the colours on the charge distribution visualisation is much darker. &lt;br /&gt;
|Polar bonds between nitrogen and boron are demonstration from the above visualisation. From the colours displayed on the charge distribution visualisation as well as the charge values, it is shown that nitrogen has a relatively large negative charge, while boron has a positive charge. This is due to the difference in electrogenativity between these atoms: nitrogen atoms are more electronegative than boron and tends to attract electrons towards themselves. It is worth noting that the hydrogen atoms do not all have the same charge. The hydrogen atoms bonded to boron have a slightly negative charge, and the ones bonded to nitrogen have a small positive charge. &lt;br /&gt;
&lt;br /&gt;
The fact that the same colour scale was used for both molecules comes in helpful here. It allows the charges on atoms to be compared directly. For example, just from looking at the colours, one can tell that or example, even though both carbon and nitrogen are electronegative, nitrogen is much more electronegative, which is quantitatively shown by Pauling&#039;s electronegativity scale.&amp;lt;ref&amp;gt;http://www.tutor-homework.com/Chemistry_Help/electronegativity_table/electronegativity.html (Accessed: 24.05.2018)&amp;lt;/ref&amp;gt;&lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
===Comparative MOs of Benzene and Borazine===&lt;br /&gt;
&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot;&lt;br /&gt;
!&lt;br /&gt;
!Benzene&lt;br /&gt;
!Borazine&lt;br /&gt;
!Comparison and Discussion&lt;br /&gt;
|-&lt;br /&gt;
!1st comparative pair&lt;br /&gt;
|[[File:Hyc116_benzene_1st_MO_pair_7.png|200x200px|centre]]&lt;br /&gt;
|[[File:Hyc116_borazine_1st_MO_pair_level9.png|200x200px|centre]]&lt;br /&gt;
|MO 9 of both benzene and borazine are comparable. They both show delocalised molecular orbital with an overall bonding character. There is a nodal plane across the molecular orbitals for both benzene and borazine. For benzene, there is contribution from all the carbon and hydrogen s orbitals. Moreover, the molecular orbitals are symmetric to their counterpart of opposite phase, giving an E&amp;lt;sub&amp;gt;1g&amp;lt;/sub&amp;gt; MO. That is not the case for borazine; they are less symmetric in borazine. This MO of borazine has an E&#039; symmetry. Nitrogen atoms are more electronegative than boron atoms and pull electron density towards themselves, resulting in a larger lobe. There is contribution from all the boron and nitrogen s orbitals, and three of the hydrogen s orbitals, though not all of them. &lt;br /&gt;
|-&lt;br /&gt;
!2nd comparative pair&lt;br /&gt;
|[[File:Hyc116_benzene_2nd_MO_pair_10.png|200x200px|centre]]&lt;br /&gt;
|[[File:Hyc116_borazine_2nd_MO_pair_level11.png|200x200px|centre]]&lt;br /&gt;
|MO 10 of benzene and MO 11 of borazine are comparable. Here shows a pair of rather delocalised molecular orbitals with slightly more antibonding character than the first pair shown above. On both MOs, there is no contribution from one pair of opposite hydrogen atoms, but contribution from s orbitals of all other atoms on both molecule. The benzene MO has an E&amp;lt;sub&amp;gt;2g&amp;lt;/sub&amp;gt; symmetry. In borazine, the lobes are in different sizes due to the higher electronegativity of nitrogen. The lobes at the nitrogen atoms are larger as they attract electrons towards themselves more so than boron atoms do. This borazine MO has an E&#039; symmetry. &lt;br /&gt;
|-&lt;br /&gt;
!3rd comparative pair&lt;br /&gt;
|[[File:Hyc116_benzene_3rd_MO_pair_21.png|200x200px|centre]]&lt;br /&gt;
|[[File:Hyc116_borazine_3rd_MO_pair_level21.png|200x200px|centre]]&lt;br /&gt;
|The HOMO (MO 21) of benzene and the HOMO (MO 21) of borazine are comparable. They are both made of p orbitals of all carbon atoms (or all boron and nitrogen atoms in the case of borazine); there is no contribution from hydrogen atoms as they do not have p orbitals. There is a nodal plan perpendicular to the z axis (highest rotational axis) and one parallel to the z axis. On benzene, the MO is very symmetric and has an E&amp;lt;sub&amp;gt;1g&amp;lt;/sub&amp;gt; symmetry; the lobes of the MO are the same in size. On borazine, the lobe where there are two nitrogen atoms is bigger in size, again due to the higher electronegtivity of nitrogen compared to boron. The borazine MO has an E&#039; &#039; symmetry.&lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
===Aromaticity: discussion===&lt;br /&gt;
&lt;br /&gt;
Aromatic compounds display properties such as their high stability and bond lengths between typical single and double bonds. A simple understanding of aromaticity involves the overlap of p orbitals perpendicular to the cyclic plane; the delocalisation of electrons on the pi system is identified to be responsible of the stability of aromatic systems. Aromatic compounds can be identified by the Huckel’s rule, which states that conjugated planar cyclic molecules with (4n +2) π electrons are aromatic. Both benzene and borazine obey the Huckel’s rule and fit the conventional description of aromaticity. &amp;lt;ref&amp;gt;Clayden, J., Greeves, N. &amp;amp; Warren, S. G. Organic chemistry. (Oxford University Press, 2012)&amp;lt;/ref&amp;gt;&lt;br /&gt;
&lt;br /&gt;
However, it is proved in recent years that the conventional criteria do not necessarily have to be obeyed for a compound to be aromatic. For instance, it has been shown that some non-planar compounds, for example, meta- and para- cyclophanes, display aromaticity. This suggests that the criteria for aromaticity is not simply structural, and these advances give rise to concepts such as quasiaromaticity and pseudoaromaticity. Recent advances show that there are quantum mechanics basis on the idea of aromaticity.&amp;lt;ref&amp;gt;Palusiak, M. &amp;amp; Krygowski, T. M. Application of AIM Parameters at Ring Critical Points for Estimation of π-Electron Delocalization in Six-Membered Aromatic and Quasi-Aromatic Rings. Chemistry - A European Journal 13, 7996–8006 (2007).&amp;lt;/ref&amp;gt; &lt;br /&gt;
&lt;br /&gt;
In conclusion, while the overlap of pi orbitals provides a simple understanding for aromaticity, it is not a sufficient description for aromaticity. There is also sigma orbital and quantum mechanics contribution to aromaticity.&lt;br /&gt;
&lt;br /&gt;
==References==&lt;/div&gt;</summary>
		<author><name>Hyc116</name></author>
	</entry>
	<entry>
		<id>https://chemwiki.ch.ic.ac.uk/index.php?title=MO_hyc116&amp;diff=732651</id>
		<title>MO hyc116</title>
		<link rel="alternate" type="text/html" href="https://chemwiki.ch.ic.ac.uk/index.php?title=MO_hyc116&amp;diff=732651"/>
		<updated>2018-05-25T15:40:33Z</updated>

		<summary type="html">&lt;p&gt;Hyc116: /* Associated energies: ammonium borane */&lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;==BH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;==&lt;br /&gt;
&lt;br /&gt;
===standard information===&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;Calculation type&amp;lt;/b&amp;gt;: Optimisation&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;Calculation Method&amp;lt;/b&amp;gt;: B3LYP&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;Basis set&amp;lt;/b&amp;gt;: 6-31G(d,p) &lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Summary table&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
[[file:Hyc116_bh3_631g_opt_summarytable.png]]&lt;br /&gt;
&lt;br /&gt;
The above summary table was obtained after the 2nd optimisation of BH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt; (after the initial optimisation using the 3-21G basis set). Notice how the symmetry is incorrect and shown as Cs. This is because the symmetry was manually broken at the beginning by changing the bond length of B-H bonds. The point group was manually adjusted and the molecule was optimised again before the frequency analysis and the new summary table is attached below.&lt;br /&gt;
&lt;br /&gt;
[[file:Hyc116_bh3_correctsummarytable.png]]&lt;br /&gt;
&lt;br /&gt;
The above summary table was obtained from the optimisation after adjusting the symmetry. The point shown in this summary table is D&amp;lt;sub&amp;gt;3h&amp;lt;/sub&amp;gt;, which is the correct for BH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;. &lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Items table&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
Below is the items table taken from the optimisation with the correct point group.&lt;br /&gt;
&lt;br /&gt;
&amp;lt;pre&amp;gt;&lt;br /&gt;
Item               Value     Threshold  Converged?&lt;br /&gt;
 Maximum Force            0.000015     0.000450     YES&lt;br /&gt;
 RMS     Force            0.000010     0.000300     YES&lt;br /&gt;
 Maximum Displacement     0.000058     0.001800     YES&lt;br /&gt;
 RMS     Displacement     0.000038     0.001200     YES&lt;br /&gt;
&amp;lt;/pre&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Frequency log file&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
[[Media:HYC116 BH3 FREQ.LOG]] &lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Frequencies&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;pre&amp;gt;&lt;br /&gt;
Low frequencies ---  -10.3498   -3.4492   -1.2454   -0.0055    0.4779    3.2165&lt;br /&gt;
Low frequencies --- 1162.9519 1213.1527 1213.1554&lt;br /&gt;
&amp;lt;/pre&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;jmol of BH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;&#039;&#039;&#039;&lt;br /&gt;
&amp;lt;jmol&amp;gt;&amp;lt;jmolApplet&amp;gt;&lt;br /&gt;
  &amp;lt;title&amp;gt;optimised BH3&amp;lt;/title&amp;gt;&lt;br /&gt;
  &amp;lt;color&amp;gt;black&amp;lt;/color&amp;gt;&lt;br /&gt;
  &amp;lt;size&amp;gt;200&amp;lt;/size&amp;gt;&lt;br /&gt;
  &amp;lt;uploadedFileContents&amp;gt;HYC116_BH3_FREQ.LOG&amp;lt;/uploadedFileContents&amp;gt;&lt;br /&gt;
&amp;lt;/jmolApplet&amp;gt;&amp;lt;/jmol&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
===Vibrational spectrum===&lt;br /&gt;
&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot;&lt;br /&gt;
!wavenumber (cm&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;)&lt;br /&gt;
!Intensity (arbitrary units)&lt;br /&gt;
!symmetry&lt;br /&gt;
!IR active?&lt;br /&gt;
!type&lt;br /&gt;
|-&lt;br /&gt;
|1163&lt;br /&gt;
|93&lt;br /&gt;
|A&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;&#039; &#039;&lt;br /&gt;
|Yes&lt;br /&gt;
|Out of plane bend&lt;br /&gt;
|-&lt;br /&gt;
|1213&lt;br /&gt;
|14&lt;br /&gt;
|E&#039;&lt;br /&gt;
|Very slight&lt;br /&gt;
|Bend&lt;br /&gt;
|-&lt;br /&gt;
|1213&lt;br /&gt;
|14&lt;br /&gt;
|E&#039;&lt;br /&gt;
|Very slight&lt;br /&gt;
|Bend&lt;br /&gt;
|-&lt;br /&gt;
|2582&lt;br /&gt;
|0&lt;br /&gt;
|A&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;&#039;&lt;br /&gt;
|No&lt;br /&gt;
|Symmetric stretch&lt;br /&gt;
|-&lt;br /&gt;
|2716&lt;br /&gt;
|126&lt;br /&gt;
|E&#039;&lt;br /&gt;
|Yes&lt;br /&gt;
|Asymmetric stretch&lt;br /&gt;
|-&lt;br /&gt;
|2716&lt;br /&gt;
|126&lt;br /&gt;
|E&#039;&lt;br /&gt;
|Yes&lt;br /&gt;
|Asymmetric stretch&lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;IR spectrum&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
[[file:Hyc116_ir_bh3.png|400*600]]&lt;br /&gt;
&lt;br /&gt;
There are only three peaks on the IR spectrum of BH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;, despite that there are 6 vibrational modes for the molecule. As shown in the table above, the symmetric stretching mode with A1 symmetry at 2582 cm&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt; is not IR active; naturally, that vibrational mode doesn’t give a peak on the IR spectrum. As shown from the table, two pairs of vibrational modes, the bond angle deformation/bend at 1213 cm&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt; and the asymmetric bond stretch at 2716 cm&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;, are degenerate with the symmetry label E. This means that they have the same energy, and hence give the same wavenumber on the IR spectrum. Each pair of degenerate vibrational modes give rise to one peak. This leaves three peaks, as confirmed by the IR spectrum above.&lt;br /&gt;
&lt;br /&gt;
===Molecular orbitals of BH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;===&lt;br /&gt;
&lt;br /&gt;
[[file:hyc116_bh3_MO_diagram.png]]&lt;br /&gt;
&lt;br /&gt;
The above molecular orbital diagram was taken from Dr Patricia Hunt&#039;s &amp;lt;i&amp;gt;Lecture 4 Tutorial Problem Model Answers&amp;lt;/i&amp;gt;.&amp;lt;ref&amp;gt;P. Hunt, &amp;quot;Lecture 4 Tutorial Problem Model Answers&amp;quot;, 2 (2018)&amp;lt;/ref&amp;gt; Diagrams of the &amp;quot;real&amp;quot; MOs were obtained from Gaussian.&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
There is no significant difference between the LCAO MOs and the real ones. Features such as orbital phases are shown clearly on both the LCAO MOs and the real MOs, illustrating the bonding/anti-bonding characters of the molecular orbitals. This suggests that the the qualitative MO theory is highly accurate and useful when studying the molecular orbitals of molecules.&lt;br /&gt;
&lt;br /&gt;
==Associated energies: ammonium borane==&lt;br /&gt;
&lt;br /&gt;
===NH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;===&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;Calculation type&amp;lt;/b&amp;gt;: Optimisation&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;Calculation Method&amp;lt;/b&amp;gt;: B3LYP&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;Basis set&amp;lt;/b&amp;gt;: 6-31G(d,p) &lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Summary table&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
[[file:Hyc116_nh3_631g_summarytable.png]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Items table&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;pre&amp;gt;&lt;br /&gt;
Item               Value     Threshold  Converged?&lt;br /&gt;
 Maximum Force            0.000006     0.000450     YES&lt;br /&gt;
 RMS     Force            0.000004     0.000300     YES&lt;br /&gt;
 Maximum Displacement     0.000012     0.001800     YES&lt;br /&gt;
 RMS     Displacement     0.000008     0.001200     YES&lt;br /&gt;
&amp;lt;/pre&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Frequency log file&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
[[Media:HYC116_NH3_FREQ.LOG]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Frequencies&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;pre&amp;gt;&lt;br /&gt;
Low frequencies ---   -8.5646   -8.5588   -0.0047    0.0454    0.1784   26.4183&lt;br /&gt;
Low frequencies --- 1089.7603 1694.1865 1694.1865&lt;br /&gt;
&amp;lt;/pre&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;jmol of NH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;&#039;&#039;&#039;&lt;br /&gt;
&amp;lt;jmol&amp;gt;&amp;lt;jmolApplet&amp;gt;&lt;br /&gt;
  &amp;lt;title&amp;gt;optimised NH3&amp;lt;/title&amp;gt;&lt;br /&gt;
  &amp;lt;color&amp;gt;black&amp;lt;/color&amp;gt;&lt;br /&gt;
  &amp;lt;size&amp;gt;200&amp;lt;/size&amp;gt;&lt;br /&gt;
  &amp;lt;uploadedFileContents&amp;gt;HYC116_NH3_FREQ.LOG&amp;lt;/uploadedFileContents&amp;gt;&lt;br /&gt;
&amp;lt;/jmolApplet&amp;gt;&amp;lt;/jmol&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
===NH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;BH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;===&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;Calculation type&amp;lt;/b&amp;gt;: Optimisation&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;Calculation Method&amp;lt;/b&amp;gt;: B3LYP&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;Basis set&amp;lt;/b&amp;gt;: 6-31G(d,p) &lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Summary table&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
[[file:Hyc116_nh3bh3_631g_summarytable1.png]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Items table&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;pre&amp;gt;&lt;br /&gt;
Item               Value     Threshold  Converged?&lt;br /&gt;
 Maximum Force            0.000121     0.000450     YES&lt;br /&gt;
 RMS     Force            0.000057     0.000300     YES&lt;br /&gt;
 Maximum Displacement     0.000501     0.001800     YES&lt;br /&gt;
 RMS     Displacement     0.000293     0.001200     YES&lt;br /&gt;
&amp;lt;/pre&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Frequency log file&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
[[Media:HYC116_NH3BH3_FREQ1.LOG]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Frequencies&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;pre&amp;gt;&lt;br /&gt;
Low frequencies ---   -0.0574   -0.0501   -0.0074   21.6276   21.6377   40.3839&lt;br /&gt;
Low frequencies ---  265.9973  632.3725  640.1275&lt;br /&gt;
&amp;lt;/pre&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;jmol of NH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;BH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;&#039;&#039;&#039;&lt;br /&gt;
&amp;lt;jmol&amp;gt;&amp;lt;jmolApplet&amp;gt;&lt;br /&gt;
  &amp;lt;title&amp;gt;optimised NH3BH3&amp;lt;/title&amp;gt;&lt;br /&gt;
  &amp;lt;color&amp;gt;black&amp;lt;/color&amp;gt;&lt;br /&gt;
  &amp;lt;size&amp;gt;200&amp;lt;/size&amp;gt;&lt;br /&gt;
  &amp;lt;uploadedFileContents&amp;gt;HYC116_NH3BH3_FREQ.LOG&amp;lt;/uploadedFileContents&amp;gt;&lt;br /&gt;
&amp;lt;/jmolApplet&amp;gt;&amp;lt;/jmol&amp;gt;&lt;br /&gt;
&lt;br /&gt;
===Association energy===&lt;br /&gt;
&lt;br /&gt;
E(BH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;) (using the optimisation with the correct symmetry) = -26.61532363 a.u. = &amp;lt;b&amp;gt;-26.61532 a.u. (5 d.p.)&amp;lt;/b&amp;gt;&lt;br /&gt;
&lt;br /&gt;
E(NH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;) = -56.55776873 a.u. = &amp;lt;b&amp;gt;-56.55777 a.u. (5 d.p.)&amp;lt;/b&amp;gt;&lt;br /&gt;
&lt;br /&gt;
E(NH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;BH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;) = -83.22468892 a.u. = &amp;lt;b&amp;gt;-83.22469 a.u. (5 d.p.)&amp;lt;/b&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
Carrying out calculations using numbers which has already been rounded up can possibly result in errors in the last digit. Hence, here the calculations were carried out using the numbers provided from the optimisations (i.e. with more decimal places than necessary); the answer was then rounded up to the desired accuracy. &lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
ΔE = E(NH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;BH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;)-[E(NH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;)+E(BH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;)]&lt;br /&gt;
&lt;br /&gt;
ΔE = -83.22468892 - (-56.55776873 + -26.61532363) = -0.05159656 a.u. &lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;ΔE = -0.05160 a.u. (5 d.p.)&amp;lt;/b&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Converting energy from a.u. to kJ/mol&#039;&#039;&#039;&lt;br /&gt;
An atomic unit for energy is Hartree, which is equal to 2625.5 kJ/mol.&lt;br /&gt;
&amp;lt;ref&amp;gt;https://cccbdb.nist.gov/hartree.asp (Accessed: 22.05.2018)&amp;lt;/ref&amp;gt;&lt;br /&gt;
 &lt;br /&gt;
&lt;br /&gt;
So ΔE in kJ/mol = -0.05159657 * 2625.5 = -135.46676828 kJ/mol&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;ΔE = -135 kJ/mol (nearest integer)&amp;lt;/b&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
The energy difference calculated above comes from the formation of the B-N dative bond. It is a relatively weak bond. According to a bond energy data sheet provided by the University of California,&amp;lt;ref&amp;gt;https://labs.chem.ucsb.edu/zakarian/armen/11---bonddissociationenergy.pdf (Accessed: 24.05.2018)&amp;lt;/ref&amp;gt;  the bond energy of the C-C bond of an ethane molecule is 368 kJ/mol. This is a fair comparison to the NH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;BH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt; molecule as the two molecules have the same structure, only with the carbon atoms on ethane swapped for Boron and Nitrogen in NH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;BH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;&lt;br /&gt;
&lt;br /&gt;
==Using a mixture of basis-sets and pseudo-potentials==&lt;br /&gt;
&lt;br /&gt;
===BBr&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;===&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;Calculation type&amp;lt;/b&amp;gt;: Optimisation&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;Calculation Method&amp;lt;/b&amp;gt;: B3LYP&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;Basis set&amp;lt;/b&amp;gt;: Boron: 6-31G(d,p) ; Br: LANL2DZ&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
Larger calculations are often sent to a web-server to run on a high-performance computer instead of a desktop. In order to experience and learn to use a web-server, the optimisation and the frequency analysis for BBr&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt; were both sent and done on a server instead of the desktop. The calculation results were downloaded from the web-server once they were finished.   &lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Summary table&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
[[file:Hyc116_bbr3_opt_summarytable.png]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Items table&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;pre&amp;gt;&lt;br /&gt;
Item               Value     Threshold  Converged?&lt;br /&gt;
 Maximum Force            0.000008     0.000450     YES&lt;br /&gt;
 RMS     Force            0.000005     0.000300     YES&lt;br /&gt;
 Maximum Displacement     0.000036     0.001800     YES&lt;br /&gt;
 RMS     Displacement     0.000023     0.001200     YES&lt;br /&gt;
&amp;lt;/pre&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Frequency log file&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
[[Media:Hyc116_bbr3_freq.log]]&lt;br /&gt;
&lt;br /&gt;
Attached above is the frequency file saved onto the computer from the SCAN server portal. The frequency file was also published on the chemistry database DSpace. {{DOI|10042/202442}}&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Frequencies&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;pre&amp;gt;&lt;br /&gt;
Low frequencies ---   -0.0137   -0.0064   -0.0046    2.4315    2.4315    4.8421&lt;br /&gt;
Low frequencies ---  155.9631  155.9651  267.7052&lt;br /&gt;
&amp;lt;/pre&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;jmol of BBr&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;&#039;&#039;&#039;&lt;br /&gt;
&amp;lt;jmol&amp;gt;&amp;lt;jmolApplet&amp;gt;&lt;br /&gt;
  &amp;lt;title&amp;gt;optimised BBr3&amp;lt;/title&amp;gt;&lt;br /&gt;
  &amp;lt;color&amp;gt;black&amp;lt;/color&amp;gt;&lt;br /&gt;
  &amp;lt;size&amp;gt;200&amp;lt;/size&amp;gt;&lt;br /&gt;
  &amp;lt;uploadedFileContents&amp;gt;Hyc116_bbr3_freq.log&amp;lt;/uploadedFileContents&amp;gt;&lt;br /&gt;
&amp;lt;/jmolApplet&amp;gt;&amp;lt;/jmol&amp;gt;&lt;br /&gt;
&lt;br /&gt;
==Mini project: Aromaticity==&lt;br /&gt;
&lt;br /&gt;
===Benzene===&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;Calculation type&amp;lt;/b&amp;gt;: Optimisation&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;Calculation Method&amp;lt;/b&amp;gt;: B3LYP&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;Basis set&amp;lt;/b&amp;gt;: 6-31G(d,p) &lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Summary table&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
[[file:Hyc116_c6h6_summarytable.png]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Items table&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;pre&amp;gt;&lt;br /&gt;
Item               Value     Threshold  Converged?&lt;br /&gt;
 Maximum Force            0.000193     0.000450     YES&lt;br /&gt;
 RMS     Force            0.000079     0.000300     YES&lt;br /&gt;
 Maximum Displacement     0.000830     0.001800     YES&lt;br /&gt;
 RMS     Displacement     0.000294     0.001200     YES&lt;br /&gt;
&amp;lt;/pre&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Frequency log file&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
[[Media:HYC116_C6H6_FREQ.LOG]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Frequencies&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;pre&amp;gt;&lt;br /&gt;
Low frequencies ---   -3.5606   -3.5606   -0.0089   -0.0043   -0.0043   10.0905&lt;br /&gt;
Low frequencies ---  413.9582  413.9582  621.1416&lt;br /&gt;
&amp;lt;/pre&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;jmol of C&amp;lt;sub&amp;gt;6&amp;lt;/sub&amp;gt;H&amp;lt;sub&amp;gt;6&amp;lt;/sub&amp;gt;&#039;&#039;&#039;&lt;br /&gt;
&amp;lt;jmol&amp;gt;&amp;lt;jmolApplet&amp;gt;&lt;br /&gt;
  &amp;lt;title&amp;gt;optimised Benzene&amp;lt;/title&amp;gt;&lt;br /&gt;
  &amp;lt;color&amp;gt;black&amp;lt;/color&amp;gt;&lt;br /&gt;
  &amp;lt;size&amp;gt;200&amp;lt;/size&amp;gt;&lt;br /&gt;
  &amp;lt;uploadedFileContents&amp;gt;HYC116_C6H6_FREQ.LOG&amp;lt;/uploadedFileContents&amp;gt;&lt;br /&gt;
&amp;lt;/jmolApplet&amp;gt;&amp;lt;/jmol&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
===Borazine===&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;Calculation type&amp;lt;/b&amp;gt;: Optimisation&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;Calculation Method&amp;lt;/b&amp;gt;: B3LYP&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;Basis set&amp;lt;/b&amp;gt;: 6-31G(d,p) &lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Summary table&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
[[file:Hyc116_borazine_summarytable.png]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Items table&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;pre&amp;gt;&lt;br /&gt;
Item               Value     Threshold  Converged?&lt;br /&gt;
 Maximum Force            0.000085     0.000450     YES&lt;br /&gt;
 RMS     Force            0.000033     0.000300     YES&lt;br /&gt;
 Maximum Displacement     0.000250     0.001800     YES&lt;br /&gt;
 RMS     Displacement     0.000074     0.001200     YES&lt;br /&gt;
&amp;lt;/pre&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Frequency log file&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
[[Media:HYC116_BORAZINE_FREQ.LOG]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Frequencies&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;pre&amp;gt;&lt;br /&gt;
Low frequencies ---  -12.6626  -12.6626   -8.9272   -0.0211   -0.0104   -0.0104&lt;br /&gt;
Low frequencies ---  289.1112  289.1112  403.8613&lt;br /&gt;
&amp;lt;/pre&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;jmol of Borazine&#039;&#039;&#039;&lt;br /&gt;
&amp;lt;jmol&amp;gt;&amp;lt;jmolApplet&amp;gt;&lt;br /&gt;
  &amp;lt;title&amp;gt;optimised Borazine&amp;lt;/title&amp;gt;&lt;br /&gt;
  &amp;lt;color&amp;gt;black&amp;lt;/color&amp;gt;&lt;br /&gt;
  &amp;lt;size&amp;gt;200&amp;lt;/size&amp;gt;&lt;br /&gt;
  &amp;lt;uploadedFileContents&amp;gt;HYC116_BORAZINE_FREQ.LOG&amp;lt;/uploadedFileContents&amp;gt;&lt;br /&gt;
&amp;lt;/jmolApplet&amp;gt;&amp;lt;/jmol&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
===Charge distribution===&lt;br /&gt;
&lt;br /&gt;
An NBO charge analysis was carried out on both the optimised benzene and borazine. Visualisations of the charge distribution are shown in the table below, with the colour range going from -1.102 to 1.102 for both molecule. This large scale was chosen as it allows direct comparison of the charge on any atoms in these two molecules and shows the relative magnitude of charges on all these atoms. Negative charges are shown in red, and positive charges are shown in green. A neutral charge is displayed in black, so the smaller a charge is (positive or negative), the darker its colour representation is. Larger charges are shown in brighter colours. The charges are also displayed on the atoms as numbers with a neutral charge being zero. Negative charges are shown as negative number and positive charges are shown as positive numbers. &lt;br /&gt;
&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot;&lt;br /&gt;
!&lt;br /&gt;
!Benzene&lt;br /&gt;
!Borazine&lt;br /&gt;
|-&lt;br /&gt;
!Visualisation of charge distribution&lt;br /&gt;
|[[File:Hyc116_benzene_charge_distribution1.png|500x500px|thumb|centre|Charge distribution of Benzene visualisation]]&lt;br /&gt;
|[[File:Hyc116_borazine_charge_distribution1.png|500x500px|thumb|centre|Charge distribution of Borazine visualisation]]&lt;br /&gt;
|-&lt;br /&gt;
!Charge &lt;br /&gt;
|Carbon: -0.239&lt;br /&gt;
&lt;br /&gt;
Hydrogen: 0.239&lt;br /&gt;
|Nitrogen: -1.102 &lt;br /&gt;
&lt;br /&gt;
Boron: 0.747&lt;br /&gt;
&lt;br /&gt;
Hydrogen (bonded to N): 0.432&lt;br /&gt;
&lt;br /&gt;
Hydrogen (bonded to B): -0.077&lt;br /&gt;
|-&lt;br /&gt;
!Discussion&lt;br /&gt;
|From the visualisation, it is shown that there is a slightly negative charge on the carbon atoms, and a positive charge of the same magnitude on the hydrogen atoms. All the carbon atoms have the same charge as they are in identical environments. The same applies to all the hydrogen atoms. This is due to the highly symmetrical structure of benzene. Since the same colour scale was used for both benzene and borazine, and the charges are much smaller in magnitude on atoms in benzene than atoms on borazine, the colours on the charge distribution visualisation is much darker. &lt;br /&gt;
|Polar bonds between nitrogen and boron are demonstration from the above visualisation. From the colours displayed on the charge distribution visualisation as well as the charge values, it is shown that nitrogen has a relatively large negative charge, while boron has a positive charge. This is due to the difference in electrogenativity between these atoms: nitrogen atoms are more electronegative than boron and tends to attract electrons towards themselves. It is worth noting that the hydrogen atoms do not all have the same charge. The hydrogen atoms bonded to boron have a slightly negative charge, and the ones bonded to nitrogen have a small positive charge. &lt;br /&gt;
&lt;br /&gt;
The fact that the same colour scale was used for both molecules comes in helpful here. It allows the charges on atoms to be compared directly. For example, just from looking at the colours, one can tell that or example, even though both carbon and nitrogen are electronegative, nitrogen is much more electronegative, which is quantitatively shown by Pauling&#039;s electronegativity scale.&amp;lt;ref&amp;gt;http://www.tutor-homework.com/Chemistry_Help/electronegativity_table/electronegativity.html (Accessed: 24.05.2018)&amp;lt;/ref&amp;gt;&lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
===Comparative MOs of Benzene and Borazine===&lt;br /&gt;
&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot;&lt;br /&gt;
!&lt;br /&gt;
!Benzene&lt;br /&gt;
!Borazine&lt;br /&gt;
!Comparison and Discussion&lt;br /&gt;
|-&lt;br /&gt;
!1st comparative pair&lt;br /&gt;
|[[File:Hyc116_benzene_1st_MO_pair_7.png|200x200px|centre]]&lt;br /&gt;
|[[File:Hyc116_borazine_1st_MO_pair_level9.png|200x200px|centre]]&lt;br /&gt;
|MO 9 of both benzene and borazine are comparable. They both show delocalised molecular orbital with an overall bonding character. There is a nodal plane across the molecular orbitals for both benzene and borazine. For benzene, there is contribution from all the carbon and hydrogen s orbitals. Moreover, the molecular orbitals are symmetric to their counterpart of opposite phase, giving an E&amp;lt;sub&amp;gt;1g&amp;lt;/sub&amp;gt; MO. That is not the case for borazine; they are less symmetric in borazine. This MO of borazine has an E&#039; symmetry. Nitrogen atoms are more electronegative than boron atoms and pull electron density towards themselves, resulting in a larger lobe. There is contribution from all the boron and nitrogen s orbitals, and three of the hydrogen s orbitals, though not all of them. &lt;br /&gt;
|-&lt;br /&gt;
!2nd comparative pair&lt;br /&gt;
|[[File:Hyc116_benzene_2nd_MO_pair_10.png|200x200px|centre]]&lt;br /&gt;
|[[File:Hyc116_borazine_2nd_MO_pair_level11.png|200x200px|centre]]&lt;br /&gt;
|MO 10 of benzene and MO 11 of borazine are comparable. Here shows a pair of rather delocalised molecular orbitals with slightly more antibonding character than the first pair shown above. On both MOs, there is no contribution from one pair of opposite hydrogen atoms, but contribution from s orbitals of all other atoms on both molecule. The benzene MO has an E&amp;lt;sub&amp;gt;2g&amp;lt;/sub&amp;gt; symmetry. In borazine, the lobes are in different sizes due to the higher electronegativity of nitrogen. The lobes at the nitrogen atoms are larger as they attract electrons towards themselves more so than boron atoms do. This borazine MO has an E&#039; symmetry. &lt;br /&gt;
|-&lt;br /&gt;
!3rd comparative pair&lt;br /&gt;
|[[File:Hyc116_benzene_3rd_MO_pair_21.png|200x200px|centre]]&lt;br /&gt;
|[[File:Hyc116_borazine_3rd_MO_pair_level21.png|200x200px|centre]]&lt;br /&gt;
|The HOMO (MO 21) of benzene and the HOMO (MO 21) of borazine are comparable. They are both made of p orbitals of all carbon atoms (or all boron and nitrogen atoms in the case of borazine); there is no contribution from hydrogen atoms as they do not have p orbitals. There is a nodal plan perpendicular to the z axis (highest rotational axis) and one parallel to the z axis. On benzene, the MO is very symmetric and has an E&amp;lt;sub&amp;gt;1g&amp;lt;/sub&amp;gt; symmetry; the lobes of the MO are the same in size. On borazine, the lobe where there are two nitrogen atoms is bigger in size, again due to the higher electronegtivity of nitrogen compared to boron. The borazine MO has an E&#039; &#039; symmetry.&lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
===Aromaticity: discussion===&lt;br /&gt;
&lt;br /&gt;
Aromatic compounds display properties such as their high stability and bond lengths between typical single and double bonds. A simple understanding of aromaticity involves the overlap of p orbitals perpendicular to the cyclic plane; the delocalisation of electrons on the pi system is identified to be responsible of the stability of aromatic systems. Aromatic compounds can be identified by the Huckel’s rule, which states that conjugated planar cyclic molecules with (4n +2) π electrons are aromatic. Both benzene and borazine obey the Huckel’s rule and fit the conventional description of aromaticity. &amp;lt;ref&amp;gt;Clayden, J., Greeves, N. &amp;amp; Warren, S. G. Organic chemistry. (Oxford University Press, 2012)&amp;lt;/ref&amp;gt;&lt;br /&gt;
&lt;br /&gt;
However, it is proved in recent years that the conventional criteria do not necessarily have to be obeyed for a compound to be aromatic. For instance, there has been shown that some non-planar compounds display aromaticity. This suggests that the criteria for aromaticity is not simply structural, and these advances give rise to concepts such as quasiaromaticity and pseudoaromaticity. Recent advances show that there are quantum mechanics basis on the idea of aromaticity.&amp;lt;ref&amp;gt;Palusiak, M. &amp;amp; Krygowski, T. M. Application of AIM Parameters at Ring Critical Points for Estimation of π-Electron Delocalization in Six-Membered Aromatic and Quasi-Aromatic Rings. Chemistry - A European Journal 13, 7996–8006 (2007).&amp;lt;/ref&amp;gt; &lt;br /&gt;
&lt;br /&gt;
In conclusion, while the overlap of pi orbitals provides a simple understanding for aromaticity, it is not a sufficient description for aromaticity. There is also sigma orbital and quantum mechanics contribution to aromaticity.&lt;br /&gt;
&lt;br /&gt;
==References==&lt;/div&gt;</summary>
		<author><name>Hyc116</name></author>
	</entry>
	<entry>
		<id>https://chemwiki.ch.ic.ac.uk/index.php?title=MO_hyc116&amp;diff=732648</id>
		<title>MO hyc116</title>
		<link rel="alternate" type="text/html" href="https://chemwiki.ch.ic.ac.uk/index.php?title=MO_hyc116&amp;diff=732648"/>
		<updated>2018-05-25T15:40:08Z</updated>

		<summary type="html">&lt;p&gt;Hyc116: /* Mini project: Aromaticity */&lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;==BH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;==&lt;br /&gt;
&lt;br /&gt;
===standard information===&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;Calculation type&amp;lt;/b&amp;gt;: Optimisation&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;Calculation Method&amp;lt;/b&amp;gt;: B3LYP&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;Basis set&amp;lt;/b&amp;gt;: 6-31G(d,p) &lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Summary table&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
[[file:Hyc116_bh3_631g_opt_summarytable.png]]&lt;br /&gt;
&lt;br /&gt;
The above summary table was obtained after the 2nd optimisation of BH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt; (after the initial optimisation using the 3-21G basis set). Notice how the symmetry is incorrect and shown as Cs. This is because the symmetry was manually broken at the beginning by changing the bond length of B-H bonds. The point group was manually adjusted and the molecule was optimised again before the frequency analysis and the new summary table is attached below.&lt;br /&gt;
&lt;br /&gt;
[[file:Hyc116_bh3_correctsummarytable.png]]&lt;br /&gt;
&lt;br /&gt;
The above summary table was obtained from the optimisation after adjusting the symmetry. The point shown in this summary table is D&amp;lt;sub&amp;gt;3h&amp;lt;/sub&amp;gt;, which is the correct for BH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;. &lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Items table&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
Below is the items table taken from the optimisation with the correct point group.&lt;br /&gt;
&lt;br /&gt;
&amp;lt;pre&amp;gt;&lt;br /&gt;
Item               Value     Threshold  Converged?&lt;br /&gt;
 Maximum Force            0.000015     0.000450     YES&lt;br /&gt;
 RMS     Force            0.000010     0.000300     YES&lt;br /&gt;
 Maximum Displacement     0.000058     0.001800     YES&lt;br /&gt;
 RMS     Displacement     0.000038     0.001200     YES&lt;br /&gt;
&amp;lt;/pre&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Frequency log file&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
[[Media:HYC116 BH3 FREQ.LOG]] &lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Frequencies&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;pre&amp;gt;&lt;br /&gt;
Low frequencies ---  -10.3498   -3.4492   -1.2454   -0.0055    0.4779    3.2165&lt;br /&gt;
Low frequencies --- 1162.9519 1213.1527 1213.1554&lt;br /&gt;
&amp;lt;/pre&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;jmol of BH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;&#039;&#039;&#039;&lt;br /&gt;
&amp;lt;jmol&amp;gt;&amp;lt;jmolApplet&amp;gt;&lt;br /&gt;
  &amp;lt;title&amp;gt;optimised BH3&amp;lt;/title&amp;gt;&lt;br /&gt;
  &amp;lt;color&amp;gt;black&amp;lt;/color&amp;gt;&lt;br /&gt;
  &amp;lt;size&amp;gt;200&amp;lt;/size&amp;gt;&lt;br /&gt;
  &amp;lt;uploadedFileContents&amp;gt;HYC116_BH3_FREQ.LOG&amp;lt;/uploadedFileContents&amp;gt;&lt;br /&gt;
&amp;lt;/jmolApplet&amp;gt;&amp;lt;/jmol&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
===Vibrational spectrum===&lt;br /&gt;
&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot;&lt;br /&gt;
!wavenumber (cm&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;)&lt;br /&gt;
!Intensity (arbitrary units)&lt;br /&gt;
!symmetry&lt;br /&gt;
!IR active?&lt;br /&gt;
!type&lt;br /&gt;
|-&lt;br /&gt;
|1163&lt;br /&gt;
|93&lt;br /&gt;
|A&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;&#039; &#039;&lt;br /&gt;
|Yes&lt;br /&gt;
|Out of plane bend&lt;br /&gt;
|-&lt;br /&gt;
|1213&lt;br /&gt;
|14&lt;br /&gt;
|E&#039;&lt;br /&gt;
|Very slight&lt;br /&gt;
|Bend&lt;br /&gt;
|-&lt;br /&gt;
|1213&lt;br /&gt;
|14&lt;br /&gt;
|E&#039;&lt;br /&gt;
|Very slight&lt;br /&gt;
|Bend&lt;br /&gt;
|-&lt;br /&gt;
|2582&lt;br /&gt;
|0&lt;br /&gt;
|A&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;&#039;&lt;br /&gt;
|No&lt;br /&gt;
|Symmetric stretch&lt;br /&gt;
|-&lt;br /&gt;
|2716&lt;br /&gt;
|126&lt;br /&gt;
|E&#039;&lt;br /&gt;
|Yes&lt;br /&gt;
|Asymmetric stretch&lt;br /&gt;
|-&lt;br /&gt;
|2716&lt;br /&gt;
|126&lt;br /&gt;
|E&#039;&lt;br /&gt;
|Yes&lt;br /&gt;
|Asymmetric stretch&lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;IR spectrum&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
[[file:Hyc116_ir_bh3.png|400*600]]&lt;br /&gt;
&lt;br /&gt;
There are only three peaks on the IR spectrum of BH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;, despite that there are 6 vibrational modes for the molecule. As shown in the table above, the symmetric stretching mode with A1 symmetry at 2582 cm&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt; is not IR active; naturally, that vibrational mode doesn’t give a peak on the IR spectrum. As shown from the table, two pairs of vibrational modes, the bond angle deformation/bend at 1213 cm&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt; and the asymmetric bond stretch at 2716 cm&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;, are degenerate with the symmetry label E. This means that they have the same energy, and hence give the same wavenumber on the IR spectrum. Each pair of degenerate vibrational modes give rise to one peak. This leaves three peaks, as confirmed by the IR spectrum above.&lt;br /&gt;
&lt;br /&gt;
===Molecular orbitals of BH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;===&lt;br /&gt;
&lt;br /&gt;
[[file:hyc116_bh3_MO_diagram.png]]&lt;br /&gt;
&lt;br /&gt;
The above molecular orbital diagram was taken from Dr Patricia Hunt&#039;s &amp;lt;i&amp;gt;Lecture 4 Tutorial Problem Model Answers&amp;lt;/i&amp;gt;.&amp;lt;ref&amp;gt;P. Hunt, &amp;quot;Lecture 4 Tutorial Problem Model Answers&amp;quot;, 2 (2018)&amp;lt;/ref&amp;gt; Diagrams of the &amp;quot;real&amp;quot; MOs were obtained from Gaussian.&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
There is no significant difference between the LCAO MOs and the real ones. Features such as orbital phases are shown clearly on both the LCAO MOs and the real MOs, illustrating the bonding/anti-bonding characters of the molecular orbitals. This suggests that the the qualitative MO theory is highly accurate and useful when studying the molecular orbitals of molecules.&lt;br /&gt;
&lt;br /&gt;
==Associated energies: ammonium borane==&lt;br /&gt;
&lt;br /&gt;
===NH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;===&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;Calculation type&amp;lt;/b&amp;gt;: Optimisation&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;Calculation Method&amp;lt;/b&amp;gt;: B3LYP&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;Basis set&amp;lt;/b&amp;gt;: 6-31G(d,p) &lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Summary table&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
[[file:Hyc116_nh3_631g_summarytable.png]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Items table&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;pre&amp;gt;&lt;br /&gt;
Item               Value     Threshold  Converged?&lt;br /&gt;
 Maximum Force            0.000006     0.000450     YES&lt;br /&gt;
 RMS     Force            0.000004     0.000300     YES&lt;br /&gt;
 Maximum Displacement     0.000012     0.001800     YES&lt;br /&gt;
 RMS     Displacement     0.000008     0.001200     YES&lt;br /&gt;
&amp;lt;/pre&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Frequency log file&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
[[Media:HYC116_NH3_FREQ.LOG]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Frequencies&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;pre&amp;gt;&lt;br /&gt;
Low frequencies ---   -8.5646   -8.5588   -0.0047    0.0454    0.1784   26.4183&lt;br /&gt;
Low frequencies --- 1089.7603 1694.1865 1694.1865&lt;br /&gt;
&amp;lt;/pre&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;jmol of NH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;&#039;&#039;&#039;&lt;br /&gt;
&amp;lt;jmol&amp;gt;&amp;lt;jmolApplet&amp;gt;&lt;br /&gt;
  &amp;lt;title&amp;gt;optimised NH3&amp;lt;/title&amp;gt;&lt;br /&gt;
  &amp;lt;color&amp;gt;black&amp;lt;/color&amp;gt;&lt;br /&gt;
  &amp;lt;size&amp;gt;200&amp;lt;/size&amp;gt;&lt;br /&gt;
  &amp;lt;uploadedFileContents&amp;gt;HYC116_NH3_FREQ.LOG&amp;lt;/uploadedFileContents&amp;gt;&lt;br /&gt;
&amp;lt;/jmolApplet&amp;gt;&amp;lt;/jmol&amp;gt;&lt;br /&gt;
&lt;br /&gt;
===NH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;BH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;===&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;Calculation type&amp;lt;/b&amp;gt;: Optimisation&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;Calculation Method&amp;lt;/b&amp;gt;: B3LYP&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;Basis set&amp;lt;/b&amp;gt;: 6-31G(d,p) &lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Summary table&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
[[file:Hyc116_nh3bh3_631g_summarytable1.png]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Items table&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;pre&amp;gt;&lt;br /&gt;
Item               Value     Threshold  Converged?&lt;br /&gt;
 Maximum Force            0.000121     0.000450     YES&lt;br /&gt;
 RMS     Force            0.000057     0.000300     YES&lt;br /&gt;
 Maximum Displacement     0.000501     0.001800     YES&lt;br /&gt;
 RMS     Displacement     0.000293     0.001200     YES&lt;br /&gt;
&amp;lt;/pre&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Frequency log file&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
[[Media:HYC116_NH3BH3_FREQ1.LOG]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Frequencies&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;pre&amp;gt;&lt;br /&gt;
Low frequencies ---   -0.0574   -0.0501   -0.0074   21.6276   21.6377   40.3839&lt;br /&gt;
Low frequencies ---  265.9973  632.3725  640.1275&lt;br /&gt;
&amp;lt;/pre&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;jmol of NH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;BH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;&#039;&#039;&#039;&lt;br /&gt;
&amp;lt;jmol&amp;gt;&amp;lt;jmolApplet&amp;gt;&lt;br /&gt;
  &amp;lt;title&amp;gt;optimised NH3BH3&amp;lt;/title&amp;gt;&lt;br /&gt;
  &amp;lt;color&amp;gt;black&amp;lt;/color&amp;gt;&lt;br /&gt;
  &amp;lt;size&amp;gt;200&amp;lt;/size&amp;gt;&lt;br /&gt;
  &amp;lt;uploadedFileContents&amp;gt;HYC116_NH3BH3_FREQ.LOG&amp;lt;/uploadedFileContents&amp;gt;&lt;br /&gt;
&amp;lt;/jmolApplet&amp;gt;&amp;lt;/jmol&amp;gt;&lt;br /&gt;
&lt;br /&gt;
===Association energy===&lt;br /&gt;
&lt;br /&gt;
E(BH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;) (using the optimisation with the correct symmetry) = -26.61532363 a.u. = &amp;lt;b&amp;gt;-26.61532 a.u. (5 d.p.)&amp;lt;/b&amp;gt;&lt;br /&gt;
&lt;br /&gt;
E(NH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;) = -56.55776873 a.u. = &amp;lt;b&amp;gt;-56.55777 a.u. (5 d.p.)&amp;lt;/b&amp;gt;&lt;br /&gt;
&lt;br /&gt;
E(NH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;BH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;) = -83.22468892 a.u. = &amp;lt;b&amp;gt;-83.22469 a.u. (5 d.p.)&amp;lt;/b&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
Carrying out calculations using numbers which has already been rounded up can possibly result in errors in the last digit. Hence, here the calculations were carried out using the numbers provided from the optimisations (i.e. with more decimal places than necessary); the answer was then rounded up to the desired accuracy. &lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
ΔE = E(NH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;BH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;)-[E(NH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;)+E(BH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;)]&lt;br /&gt;
&lt;br /&gt;
ΔE = -83.22468892 - (-56.55776873 + -26.61532363) = -0.05159656 a.u. &lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;ΔE = -0.05160 a.u. (5 d.p.)&amp;lt;/b&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Converting energy from a.u. to kJ/mol&#039;&#039;&#039;&lt;br /&gt;
An atomic unit for energy is Hartree, which is equal to 2625.5 kJ/mol.&lt;br /&gt;
&amp;lt;ref&amp;gt;https://cccbdb.nist.gov/hartree.asp (Accessed: 22.05.2018)&amp;lt;/ref&amp;gt;&lt;br /&gt;
 &lt;br /&gt;
&lt;br /&gt;
So ΔE in kJ/mol = -0.05159657 * 2625.5 = -135.46676828 kJ/mol&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;ΔE = -135 kJ/mol (nearest integer)&amp;lt;/b&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
The energy difference calculated above comes from the formation of the B-N dative bond. It is a relatively weak bond. According to a bond energy data sheet provided by the University of California,&amp;lt;ref&amp;gt;https://labs.chem.ucsb.edu/zakarian/armen/11---bonddissociationenergy.pdf (Accessed: 24.05.2018)&amp;lt;/ref&amp;gt;  the bond energy of the C-C bond of an ethane molecule is 368 kJ/mol. This is a fair comparison to the NH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;BH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt; molecule as the two molecules have the same structure, only with the carbon atoms on ethane swapped for Boron and Nitrogen in NH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;BH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;&lt;br /&gt;
&lt;br /&gt;
==Using a mixture of basis-sets and pseudo-potentials==&lt;br /&gt;
&lt;br /&gt;
===BBr&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;===&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;Calculation type&amp;lt;/b&amp;gt;: Optimisation&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;Calculation Method&amp;lt;/b&amp;gt;: B3LYP&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;Basis set&amp;lt;/b&amp;gt;: Boron: 6-31G(d,p) ; Br: LANL2DZ&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
Larger calculations are often sent to a web-server to run on a high-performance computer instead of a desktop. In order to experience and learn to use a web-server, the optimisation and the frequency analysis for BBr&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt; were both sent and done on a server instead of the desktop. The calculation results were downloaded from the web-server once they were finished.   &lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Summary table&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
[[file:Hyc116_bbr3_opt_summarytable.png]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Items table&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;pre&amp;gt;&lt;br /&gt;
Item               Value     Threshold  Converged?&lt;br /&gt;
 Maximum Force            0.000008     0.000450     YES&lt;br /&gt;
 RMS     Force            0.000005     0.000300     YES&lt;br /&gt;
 Maximum Displacement     0.000036     0.001800     YES&lt;br /&gt;
 RMS     Displacement     0.000023     0.001200     YES&lt;br /&gt;
&amp;lt;/pre&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Frequency log file&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
[[Media:Hyc116_bbr3_freq.log]]&lt;br /&gt;
&lt;br /&gt;
Attached above is the frequency file saved onto the computer from the SCAN server portal. The frequency file was also published on the chemistry database DSpace. {{DOI|10042/202442}}&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Frequencies&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;pre&amp;gt;&lt;br /&gt;
Low frequencies ---   -0.0137   -0.0064   -0.0046    2.4315    2.4315    4.8421&lt;br /&gt;
Low frequencies ---  155.9631  155.9651  267.7052&lt;br /&gt;
&amp;lt;/pre&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;jmol of BBr&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;&#039;&#039;&#039;&lt;br /&gt;
&amp;lt;jmol&amp;gt;&amp;lt;jmolApplet&amp;gt;&lt;br /&gt;
  &amp;lt;title&amp;gt;optimised BBr3&amp;lt;/title&amp;gt;&lt;br /&gt;
  &amp;lt;color&amp;gt;black&amp;lt;/color&amp;gt;&lt;br /&gt;
  &amp;lt;size&amp;gt;200&amp;lt;/size&amp;gt;&lt;br /&gt;
  &amp;lt;uploadedFileContents&amp;gt;Hyc116_bbr3_freq.log&amp;lt;/uploadedFileContents&amp;gt;&lt;br /&gt;
&amp;lt;/jmolApplet&amp;gt;&amp;lt;/jmol&amp;gt;&lt;br /&gt;
&lt;br /&gt;
==Mini project: Aromaticity==&lt;br /&gt;
&lt;br /&gt;
===Benzene===&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;Calculation type&amp;lt;/b&amp;gt;: Optimisation&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;Calculation Method&amp;lt;/b&amp;gt;: B3LYP&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;Basis set&amp;lt;/b&amp;gt;: 6-31G(d,p) &lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Summary table&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
[[file:Hyc116_c6h6_summarytable.png]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Items table&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;pre&amp;gt;&lt;br /&gt;
Item               Value     Threshold  Converged?&lt;br /&gt;
 Maximum Force            0.000193     0.000450     YES&lt;br /&gt;
 RMS     Force            0.000079     0.000300     YES&lt;br /&gt;
 Maximum Displacement     0.000830     0.001800     YES&lt;br /&gt;
 RMS     Displacement     0.000294     0.001200     YES&lt;br /&gt;
&amp;lt;/pre&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Frequency log file&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
[[Media:HYC116_C6H6_FREQ.LOG]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Frequencies&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;pre&amp;gt;&lt;br /&gt;
Low frequencies ---   -3.5606   -3.5606   -0.0089   -0.0043   -0.0043   10.0905&lt;br /&gt;
Low frequencies ---  413.9582  413.9582  621.1416&lt;br /&gt;
&amp;lt;/pre&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;jmol of C&amp;lt;sub&amp;gt;6&amp;lt;/sub&amp;gt;H&amp;lt;sub&amp;gt;6&amp;lt;/sub&amp;gt;&#039;&#039;&#039;&lt;br /&gt;
&amp;lt;jmol&amp;gt;&amp;lt;jmolApplet&amp;gt;&lt;br /&gt;
  &amp;lt;title&amp;gt;optimised Benzene&amp;lt;/title&amp;gt;&lt;br /&gt;
  &amp;lt;color&amp;gt;black&amp;lt;/color&amp;gt;&lt;br /&gt;
  &amp;lt;size&amp;gt;200&amp;lt;/size&amp;gt;&lt;br /&gt;
  &amp;lt;uploadedFileContents&amp;gt;HYC116_C6H6_FREQ.LOG&amp;lt;/uploadedFileContents&amp;gt;&lt;br /&gt;
&amp;lt;/jmolApplet&amp;gt;&amp;lt;/jmol&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
===Borazine===&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;Calculation type&amp;lt;/b&amp;gt;: Optimisation&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;Calculation Method&amp;lt;/b&amp;gt;: B3LYP&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;Basis set&amp;lt;/b&amp;gt;: 6-31G(d,p) &lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Summary table&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
[[file:Hyc116_borazine_summarytable.png]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Items table&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;pre&amp;gt;&lt;br /&gt;
Item               Value     Threshold  Converged?&lt;br /&gt;
 Maximum Force            0.000085     0.000450     YES&lt;br /&gt;
 RMS     Force            0.000033     0.000300     YES&lt;br /&gt;
 Maximum Displacement     0.000250     0.001800     YES&lt;br /&gt;
 RMS     Displacement     0.000074     0.001200     YES&lt;br /&gt;
&amp;lt;/pre&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Frequency log file&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
[[Media:HYC116_BORAZINE_FREQ.LOG]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Frequencies&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;pre&amp;gt;&lt;br /&gt;
Low frequencies ---  -12.6626  -12.6626   -8.9272   -0.0211   -0.0104   -0.0104&lt;br /&gt;
Low frequencies ---  289.1112  289.1112  403.8613&lt;br /&gt;
&amp;lt;/pre&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;jmol of Borazine&#039;&#039;&#039;&lt;br /&gt;
&amp;lt;jmol&amp;gt;&amp;lt;jmolApplet&amp;gt;&lt;br /&gt;
  &amp;lt;title&amp;gt;optimised Borazine&amp;lt;/title&amp;gt;&lt;br /&gt;
  &amp;lt;color&amp;gt;black&amp;lt;/color&amp;gt;&lt;br /&gt;
  &amp;lt;size&amp;gt;200&amp;lt;/size&amp;gt;&lt;br /&gt;
  &amp;lt;uploadedFileContents&amp;gt;HYC116_BORAZINE_FREQ.LOG&amp;lt;/uploadedFileContents&amp;gt;&lt;br /&gt;
&amp;lt;/jmolApplet&amp;gt;&amp;lt;/jmol&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
===Charge distribution===&lt;br /&gt;
&lt;br /&gt;
An NBO charge analysis was carried out on both the optimised benzene and borazine. Visualisations of the charge distribution are shown in the table below, with the colour range going from -1.102 to 1.102 for both molecule. This large scale was chosen as it allows direct comparison of the charge on any atoms in these two molecules and shows the relative magnitude of charges on all these atoms. Negative charges are shown in red, and positive charges are shown in green. A neutral charge is displayed in black, so the smaller a charge is (positive or negative), the darker its colour representation is. Larger charges are shown in brighter colours. The charges are also displayed on the atoms as numbers with a neutral charge being zero. Negative charges are shown as negative number and positive charges are shown as positive numbers. &lt;br /&gt;
&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot;&lt;br /&gt;
!&lt;br /&gt;
!Benzene&lt;br /&gt;
!Borazine&lt;br /&gt;
|-&lt;br /&gt;
!Visualisation of charge distribution&lt;br /&gt;
|[[File:Hyc116_benzene_charge_distribution1.png|500x500px|thumb|centre|Charge distribution of Benzene visualisation]]&lt;br /&gt;
|[[File:Hyc116_borazine_charge_distribution1.png|500x500px|thumb|centre|Charge distribution of Borazine visualisation]]&lt;br /&gt;
|-&lt;br /&gt;
!Charge &lt;br /&gt;
|Carbon: -0.239&lt;br /&gt;
&lt;br /&gt;
Hydrogen: 0.239&lt;br /&gt;
|Nitrogen: -1.102 &lt;br /&gt;
&lt;br /&gt;
Boron: 0.747&lt;br /&gt;
&lt;br /&gt;
Hydrogen (bonded to N): 0.432&lt;br /&gt;
&lt;br /&gt;
Hydrogen (bonded to B): -0.077&lt;br /&gt;
|-&lt;br /&gt;
!Discussion&lt;br /&gt;
|From the visualisation, it is shown that there is a slightly negative charge on the carbon atoms, and a positive charge of the same magnitude on the hydrogen atoms. All the carbon atoms have the same charge as they are in identical environments. The same applies to all the hydrogen atoms. This is due to the highly symmetrical structure of benzene. Since the same colour scale was used for both benzene and borazine, and the charges are much smaller in magnitude on atoms in benzene than atoms on borazine, the colours on the charge distribution visualisation is much darker. &lt;br /&gt;
|Polar bonds between nitrogen and boron are demonstration from the above visualisation. From the colours displayed on the charge distribution visualisation as well as the charge values, it is shown that nitrogen has a relatively large negative charge, while boron has a positive charge. This is due to the difference in electrogenativity between these atoms: nitrogen atoms are more electronegative than boron and tends to attract electrons towards themselves. It is worth noting that the hydrogen atoms do not all have the same charge. The hydrogen atoms bonded to boron have a slightly negative charge, and the ones bonded to nitrogen have a small positive charge. &lt;br /&gt;
&lt;br /&gt;
The fact that the same colour scale was used for both molecules comes in helpful here. It allows the charges on atoms to be compared directly. For example, just from looking at the colours, one can tell that or example, even though both carbon and nitrogen are electronegative, nitrogen is much more electronegative, which is quantitatively shown by Pauling&#039;s electronegativity scale.&amp;lt;ref&amp;gt;http://www.tutor-homework.com/Chemistry_Help/electronegativity_table/electronegativity.html (Accessed: 24.05.2018)&amp;lt;/ref&amp;gt;&lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
===Comparative MOs of Benzene and Borazine===&lt;br /&gt;
&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot;&lt;br /&gt;
!&lt;br /&gt;
!Benzene&lt;br /&gt;
!Borazine&lt;br /&gt;
!Comparison and Discussion&lt;br /&gt;
|-&lt;br /&gt;
!1st comparative pair&lt;br /&gt;
|[[File:Hyc116_benzene_1st_MO_pair_7.png|200x200px|centre]]&lt;br /&gt;
|[[File:Hyc116_borazine_1st_MO_pair_level9.png|200x200px|centre]]&lt;br /&gt;
|MO 9 of both benzene and borazine are comparable. They both show delocalised molecular orbital with an overall bonding character. There is a nodal plane across the molecular orbitals for both benzene and borazine. For benzene, there is contribution from all the carbon and hydrogen s orbitals. Moreover, the molecular orbitals are symmetric to their counterpart of opposite phase, giving an E&amp;lt;sub&amp;gt;1g&amp;lt;/sub&amp;gt; MO. That is not the case for borazine; they are less symmetric in borazine. This MO of borazine has an E&#039; symmetry. Nitrogen atoms are more electronegative than boron atoms and pull electron density towards themselves, resulting in a larger lobe. There is contribution from all the boron and nitrogen s orbitals, and three of the hydrogen s orbitals, though not all of them. &lt;br /&gt;
|-&lt;br /&gt;
!2nd comparative pair&lt;br /&gt;
|[[File:Hyc116_benzene_2nd_MO_pair_10.png|200x200px|centre]]&lt;br /&gt;
|[[File:Hyc116_borazine_2nd_MO_pair_level11.png|200x200px|centre]]&lt;br /&gt;
|MO 10 of benzene and MO 11 of borazine are comparable. Here shows a pair of rather delocalised molecular orbitals with slightly more antibonding character than the first pair shown above. On both MOs, there is no contribution from one pair of opposite hydrogen atoms, but contribution from s orbitals of all other atoms on both molecule. The benzene MO has an E&amp;lt;sub&amp;gt;2g&amp;lt;/sub&amp;gt; symmetry. In borazine, the lobes are in different sizes due to the higher electronegativity of nitrogen. The lobes at the nitrogen atoms are larger as they attract electrons towards themselves more so than boron atoms do. This borazine MO has an E&#039; symmetry. &lt;br /&gt;
|-&lt;br /&gt;
!3rd comparative pair&lt;br /&gt;
|[[File:Hyc116_benzene_3rd_MO_pair_21.png|200x200px|centre]]&lt;br /&gt;
|[[File:Hyc116_borazine_3rd_MO_pair_level21.png|200x200px|centre]]&lt;br /&gt;
|The HOMO (MO 21) of benzene and the HOMO (MO 21) of borazine are comparable. They are both made of p orbitals of all carbon atoms (or all boron and nitrogen atoms in the case of borazine); there is no contribution from hydrogen atoms as they do not have p orbitals. There is a nodal plan perpendicular to the z axis (highest rotational axis) and one parallel to the z axis. On benzene, the MO is very symmetric and has an E&amp;lt;sub&amp;gt;1g&amp;lt;/sub&amp;gt; symmetry; the lobes of the MO are the same in size. On borazine, the lobe where there are two nitrogen atoms is bigger in size, again due to the higher electronegtivity of nitrogen compared to boron. The borazine MO has an E&#039; &#039; symmetry.&lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
===Aromaticity: discussion===&lt;br /&gt;
&lt;br /&gt;
Aromatic compounds display properties such as their high stability and bond lengths between typical single and double bonds. A simple understanding of aromaticity involves the overlap of p orbitals perpendicular to the cyclic plane; the delocalisation of electrons on the pi system is identified to be responsible of the stability of aromatic systems. Aromatic compounds can be identified by the Huckel’s rule, which states that conjugated planar cyclic molecules with (4n +2) π electrons are aromatic. Both benzene and borazine obey the Huckel’s rule and fit the conventional description of aromaticity. &amp;lt;ref&amp;gt;Clayden, J., Greeves, N. &amp;amp; Warren, S. G. Organic chemistry. (Oxford University Press, 2012)&amp;lt;/ref&amp;gt;&lt;br /&gt;
&lt;br /&gt;
However, it is proved in recent years that the conventional criteria do not necessarily have to be obeyed for a compound to be aromatic. For instance, there has been shown that some non-planar compounds display aromaticity. This suggests that the criteria for aromaticity is not simply structural, and these advances give rise to concepts such as quasiaromaticity and pseudoaromaticity. Recent advances show that there are quantum mechanics basis on the idea of aromaticity.&amp;lt;ref&amp;gt;Palusiak, M. &amp;amp; Krygowski, T. M. Application of AIM Parameters at Ring Critical Points for Estimation of π-Electron Delocalization in Six-Membered Aromatic and Quasi-Aromatic Rings. Chemistry - A European Journal 13, 7996–8006 (2007).&amp;lt;/ref&amp;gt; &lt;br /&gt;
&lt;br /&gt;
In conclusion, while the overlap of pi orbitals provides a simple understanding for aromaticity, it is not a sufficient description for aromaticity. There is also sigma orbital and quantum mechanics contribution to aromaticity.&lt;br /&gt;
&lt;br /&gt;
==References==&lt;/div&gt;</summary>
		<author><name>Hyc116</name></author>
	</entry>
	<entry>
		<id>https://chemwiki.ch.ic.ac.uk/index.php?title=MO_hyc116&amp;diff=732640</id>
		<title>MO hyc116</title>
		<link rel="alternate" type="text/html" href="https://chemwiki.ch.ic.ac.uk/index.php?title=MO_hyc116&amp;diff=732640"/>
		<updated>2018-05-25T15:38:38Z</updated>

		<summary type="html">&lt;p&gt;Hyc116: /* Charge distribution */&lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;==BH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;==&lt;br /&gt;
&lt;br /&gt;
===standard information===&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;Calculation type&amp;lt;/b&amp;gt;: Optimisation&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;Calculation Method&amp;lt;/b&amp;gt;: B3LYP&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;Basis set&amp;lt;/b&amp;gt;: 6-31G(d,p) &lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Summary table&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
[[file:Hyc116_bh3_631g_opt_summarytable.png]]&lt;br /&gt;
&lt;br /&gt;
The above summary table was obtained after the 2nd optimisation of BH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt; (after the initial optimisation using the 3-21G basis set). Notice how the symmetry is incorrect and shown as Cs. This is because the symmetry was manually broken at the beginning by changing the bond length of B-H bonds. The point group was manually adjusted and the molecule was optimised again before the frequency analysis and the new summary table is attached below.&lt;br /&gt;
&lt;br /&gt;
[[file:Hyc116_bh3_correctsummarytable.png]]&lt;br /&gt;
&lt;br /&gt;
The above summary table was obtained from the optimisation after adjusting the symmetry. The point shown in this summary table is D&amp;lt;sub&amp;gt;3h&amp;lt;/sub&amp;gt;, which is the correct for BH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;. &lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Items table&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
Below is the items table taken from the optimisation with the correct point group.&lt;br /&gt;
&lt;br /&gt;
&amp;lt;pre&amp;gt;&lt;br /&gt;
Item               Value     Threshold  Converged?&lt;br /&gt;
 Maximum Force            0.000015     0.000450     YES&lt;br /&gt;
 RMS     Force            0.000010     0.000300     YES&lt;br /&gt;
 Maximum Displacement     0.000058     0.001800     YES&lt;br /&gt;
 RMS     Displacement     0.000038     0.001200     YES&lt;br /&gt;
&amp;lt;/pre&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Frequency log file&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
[[Media:HYC116 BH3 FREQ.LOG]] &lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Frequencies&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;pre&amp;gt;&lt;br /&gt;
Low frequencies ---  -10.3498   -3.4492   -1.2454   -0.0055    0.4779    3.2165&lt;br /&gt;
Low frequencies --- 1162.9519 1213.1527 1213.1554&lt;br /&gt;
&amp;lt;/pre&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;jmol of BH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;&#039;&#039;&#039;&lt;br /&gt;
&amp;lt;jmol&amp;gt;&amp;lt;jmolApplet&amp;gt;&lt;br /&gt;
  &amp;lt;title&amp;gt;optimised BH3&amp;lt;/title&amp;gt;&lt;br /&gt;
  &amp;lt;color&amp;gt;black&amp;lt;/color&amp;gt;&lt;br /&gt;
  &amp;lt;size&amp;gt;200&amp;lt;/size&amp;gt;&lt;br /&gt;
  &amp;lt;uploadedFileContents&amp;gt;HYC116_BH3_FREQ.LOG&amp;lt;/uploadedFileContents&amp;gt;&lt;br /&gt;
&amp;lt;/jmolApplet&amp;gt;&amp;lt;/jmol&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
===Vibrational spectrum===&lt;br /&gt;
&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot;&lt;br /&gt;
!wavenumber (cm&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;)&lt;br /&gt;
!Intensity (arbitrary units)&lt;br /&gt;
!symmetry&lt;br /&gt;
!IR active?&lt;br /&gt;
!type&lt;br /&gt;
|-&lt;br /&gt;
|1163&lt;br /&gt;
|93&lt;br /&gt;
|A&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;&#039; &#039;&lt;br /&gt;
|Yes&lt;br /&gt;
|Out of plane bend&lt;br /&gt;
|-&lt;br /&gt;
|1213&lt;br /&gt;
|14&lt;br /&gt;
|E&#039;&lt;br /&gt;
|Very slight&lt;br /&gt;
|Bend&lt;br /&gt;
|-&lt;br /&gt;
|1213&lt;br /&gt;
|14&lt;br /&gt;
|E&#039;&lt;br /&gt;
|Very slight&lt;br /&gt;
|Bend&lt;br /&gt;
|-&lt;br /&gt;
|2582&lt;br /&gt;
|0&lt;br /&gt;
|A&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;&#039;&lt;br /&gt;
|No&lt;br /&gt;
|Symmetric stretch&lt;br /&gt;
|-&lt;br /&gt;
|2716&lt;br /&gt;
|126&lt;br /&gt;
|E&#039;&lt;br /&gt;
|Yes&lt;br /&gt;
|Asymmetric stretch&lt;br /&gt;
|-&lt;br /&gt;
|2716&lt;br /&gt;
|126&lt;br /&gt;
|E&#039;&lt;br /&gt;
|Yes&lt;br /&gt;
|Asymmetric stretch&lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;IR spectrum&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
[[file:Hyc116_ir_bh3.png|400*600]]&lt;br /&gt;
&lt;br /&gt;
There are only three peaks on the IR spectrum of BH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;, despite that there are 6 vibrational modes for the molecule. As shown in the table above, the symmetric stretching mode with A1 symmetry at 2582 cm&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt; is not IR active; naturally, that vibrational mode doesn’t give a peak on the IR spectrum. As shown from the table, two pairs of vibrational modes, the bond angle deformation/bend at 1213 cm&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt; and the asymmetric bond stretch at 2716 cm&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;, are degenerate with the symmetry label E. This means that they have the same energy, and hence give the same wavenumber on the IR spectrum. Each pair of degenerate vibrational modes give rise to one peak. This leaves three peaks, as confirmed by the IR spectrum above.&lt;br /&gt;
&lt;br /&gt;
===Molecular orbitals of BH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;===&lt;br /&gt;
&lt;br /&gt;
[[file:hyc116_bh3_MO_diagram.png]]&lt;br /&gt;
&lt;br /&gt;
The above molecular orbital diagram was taken from Dr Patricia Hunt&#039;s &amp;lt;i&amp;gt;Lecture 4 Tutorial Problem Model Answers&amp;lt;/i&amp;gt;.&amp;lt;ref&amp;gt;P. Hunt, &amp;quot;Lecture 4 Tutorial Problem Model Answers&amp;quot;, 2 (2018)&amp;lt;/ref&amp;gt; Diagrams of the &amp;quot;real&amp;quot; MOs were obtained from Gaussian.&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
There is no significant difference between the LCAO MOs and the real ones. Features such as orbital phases are shown clearly on both the LCAO MOs and the real MOs, illustrating the bonding/anti-bonding characters of the molecular orbitals. This suggests that the the qualitative MO theory is highly accurate and useful when studying the molecular orbitals of molecules.&lt;br /&gt;
&lt;br /&gt;
==Associated energies: ammonium borane==&lt;br /&gt;
&lt;br /&gt;
===NH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;===&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;Calculation type&amp;lt;/b&amp;gt;: Optimisation&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;Calculation Method&amp;lt;/b&amp;gt;: B3LYP&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;Basis set&amp;lt;/b&amp;gt;: 6-31G(d,p) &lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Summary table&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
[[file:Hyc116_nh3_631g_summarytable.png]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Items table&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;pre&amp;gt;&lt;br /&gt;
Item               Value     Threshold  Converged?&lt;br /&gt;
 Maximum Force            0.000006     0.000450     YES&lt;br /&gt;
 RMS     Force            0.000004     0.000300     YES&lt;br /&gt;
 Maximum Displacement     0.000012     0.001800     YES&lt;br /&gt;
 RMS     Displacement     0.000008     0.001200     YES&lt;br /&gt;
&amp;lt;/pre&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Frequency log file&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
[[Media:HYC116_NH3_FREQ.LOG]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Frequencies&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;pre&amp;gt;&lt;br /&gt;
Low frequencies ---   -8.5646   -8.5588   -0.0047    0.0454    0.1784   26.4183&lt;br /&gt;
Low frequencies --- 1089.7603 1694.1865 1694.1865&lt;br /&gt;
&amp;lt;/pre&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;jmol of NH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;&#039;&#039;&#039;&lt;br /&gt;
&amp;lt;jmol&amp;gt;&amp;lt;jmolApplet&amp;gt;&lt;br /&gt;
  &amp;lt;title&amp;gt;optimised NH3&amp;lt;/title&amp;gt;&lt;br /&gt;
  &amp;lt;color&amp;gt;black&amp;lt;/color&amp;gt;&lt;br /&gt;
  &amp;lt;size&amp;gt;200&amp;lt;/size&amp;gt;&lt;br /&gt;
  &amp;lt;uploadedFileContents&amp;gt;HYC116_NH3_FREQ.LOG&amp;lt;/uploadedFileContents&amp;gt;&lt;br /&gt;
&amp;lt;/jmolApplet&amp;gt;&amp;lt;/jmol&amp;gt;&lt;br /&gt;
&lt;br /&gt;
===NH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;BH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;===&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;Calculation type&amp;lt;/b&amp;gt;: Optimisation&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;Calculation Method&amp;lt;/b&amp;gt;: B3LYP&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;Basis set&amp;lt;/b&amp;gt;: 6-31G(d,p) &lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Summary table&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
[[file:Hyc116_nh3bh3_631g_summarytable1.png]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Items table&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;pre&amp;gt;&lt;br /&gt;
Item               Value     Threshold  Converged?&lt;br /&gt;
 Maximum Force            0.000121     0.000450     YES&lt;br /&gt;
 RMS     Force            0.000057     0.000300     YES&lt;br /&gt;
 Maximum Displacement     0.000501     0.001800     YES&lt;br /&gt;
 RMS     Displacement     0.000293     0.001200     YES&lt;br /&gt;
&amp;lt;/pre&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Frequency log file&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
[[Media:HYC116_NH3BH3_FREQ1.LOG]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Frequencies&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;pre&amp;gt;&lt;br /&gt;
Low frequencies ---   -0.0574   -0.0501   -0.0074   21.6276   21.6377   40.3839&lt;br /&gt;
Low frequencies ---  265.9973  632.3725  640.1275&lt;br /&gt;
&amp;lt;/pre&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;jmol of NH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;BH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;&#039;&#039;&#039;&lt;br /&gt;
&amp;lt;jmol&amp;gt;&amp;lt;jmolApplet&amp;gt;&lt;br /&gt;
  &amp;lt;title&amp;gt;optimised NH3BH3&amp;lt;/title&amp;gt;&lt;br /&gt;
  &amp;lt;color&amp;gt;black&amp;lt;/color&amp;gt;&lt;br /&gt;
  &amp;lt;size&amp;gt;200&amp;lt;/size&amp;gt;&lt;br /&gt;
  &amp;lt;uploadedFileContents&amp;gt;HYC116_NH3BH3_FREQ.LOG&amp;lt;/uploadedFileContents&amp;gt;&lt;br /&gt;
&amp;lt;/jmolApplet&amp;gt;&amp;lt;/jmol&amp;gt;&lt;br /&gt;
&lt;br /&gt;
===Association energy===&lt;br /&gt;
&lt;br /&gt;
E(BH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;) (using the optimisation with the correct symmetry) = -26.61532363 a.u. = &amp;lt;b&amp;gt;-26.61532 a.u. (5 d.p.)&amp;lt;/b&amp;gt;&lt;br /&gt;
&lt;br /&gt;
E(NH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;) = -56.55776873 a.u. = &amp;lt;b&amp;gt;-56.55777 a.u. (5 d.p.)&amp;lt;/b&amp;gt;&lt;br /&gt;
&lt;br /&gt;
E(NH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;BH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;) = -83.22468892 a.u. = &amp;lt;b&amp;gt;-83.22469 a.u. (5 d.p.)&amp;lt;/b&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
Carrying out calculations using numbers which has already been rounded up can possibly result in errors in the last digit. Hence, here the calculations were carried out using the numbers provided from the optimisations (i.e. with more decimal places than necessary); the answer was then rounded up to the desired accuracy. &lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
ΔE = E(NH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;BH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;)-[E(NH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;)+E(BH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;)]&lt;br /&gt;
&lt;br /&gt;
ΔE = -83.22468892 - (-56.55776873 + -26.61532363) = -0.05159656 a.u. &lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;ΔE = -0.05160 a.u. (5 d.p.)&amp;lt;/b&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Converting energy from a.u. to kJ/mol&#039;&#039;&#039;&lt;br /&gt;
An atomic unit for energy is Hartree, which is equal to 2625.5 kJ/mol.&lt;br /&gt;
&amp;lt;ref&amp;gt;https://cccbdb.nist.gov/hartree.asp (Accessed: 22.05.2018)&amp;lt;/ref&amp;gt;&lt;br /&gt;
 &lt;br /&gt;
&lt;br /&gt;
So ΔE in kJ/mol = -0.05159657 * 2625.5 = -135.46676828 kJ/mol&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;ΔE = -135 kJ/mol (nearest integer)&amp;lt;/b&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
The energy difference calculated above comes from the formation of the B-N dative bond. It is a relatively weak bond. According to a bond energy data sheet provided by the University of California,&amp;lt;ref&amp;gt;https://labs.chem.ucsb.edu/zakarian/armen/11---bonddissociationenergy.pdf (Accessed: 24.05.2018)&amp;lt;/ref&amp;gt;  the bond energy of the C-C bond of an ethane molecule is 368 kJ/mol. This is a fair comparison to the NH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;BH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt; molecule as the two molecules have the same structure, only with the carbon atoms on ethane swapped for Boron and Nitrogen in NH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;BH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;&lt;br /&gt;
&lt;br /&gt;
==Using a mixture of basis-sets and pseudo-potentials==&lt;br /&gt;
&lt;br /&gt;
===BBr&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;===&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;Calculation type&amp;lt;/b&amp;gt;: Optimisation&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;Calculation Method&amp;lt;/b&amp;gt;: B3LYP&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;Basis set&amp;lt;/b&amp;gt;: Boron: 6-31G(d,p) ; Br: LANL2DZ&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
Larger calculations are often sent to a web-server to run on a high-performance computer instead of a desktop. In order to experience and learn to use a web-server, the optimisation and the frequency analysis for BBr&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt; were both sent and done on a server instead of the desktop. The calculation results were downloaded from the web-server once they were finished.   &lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Summary table&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
[[file:Hyc116_bbr3_opt_summarytable.png]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Items table&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;pre&amp;gt;&lt;br /&gt;
Item               Value     Threshold  Converged?&lt;br /&gt;
 Maximum Force            0.000008     0.000450     YES&lt;br /&gt;
 RMS     Force            0.000005     0.000300     YES&lt;br /&gt;
 Maximum Displacement     0.000036     0.001800     YES&lt;br /&gt;
 RMS     Displacement     0.000023     0.001200     YES&lt;br /&gt;
&amp;lt;/pre&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Frequency log file&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
[[Media:Hyc116_bbr3_freq.log]]&lt;br /&gt;
&lt;br /&gt;
Attached above is the frequency file saved onto the computer from the SCAN server portal. The frequency file was also published on the chemistry database DSpace. {{DOI|10042/202442}}&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Frequencies&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;pre&amp;gt;&lt;br /&gt;
Low frequencies ---   -0.0137   -0.0064   -0.0046    2.4315    2.4315    4.8421&lt;br /&gt;
Low frequencies ---  155.9631  155.9651  267.7052&lt;br /&gt;
&amp;lt;/pre&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;jmol of BBr&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;&#039;&#039;&#039;&lt;br /&gt;
&amp;lt;jmol&amp;gt;&amp;lt;jmolApplet&amp;gt;&lt;br /&gt;
  &amp;lt;title&amp;gt;optimised BBr3&amp;lt;/title&amp;gt;&lt;br /&gt;
  &amp;lt;color&amp;gt;black&amp;lt;/color&amp;gt;&lt;br /&gt;
  &amp;lt;size&amp;gt;200&amp;lt;/size&amp;gt;&lt;br /&gt;
  &amp;lt;uploadedFileContents&amp;gt;Hyc116_bbr3_freq.log&amp;lt;/uploadedFileContents&amp;gt;&lt;br /&gt;
&amp;lt;/jmolApplet&amp;gt;&amp;lt;/jmol&amp;gt;&lt;br /&gt;
&lt;br /&gt;
==Mini project: Aromaticity==&lt;br /&gt;
&lt;br /&gt;
===Benzene===&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;Calculation type&amp;lt;/b&amp;gt;: Optimisation&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;Calculation Method&amp;lt;/b&amp;gt;: B3LYP&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;Basis set&amp;lt;/b&amp;gt;: 6-31G(d,p) &lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Summary table&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
[[file:Hyc116_c6h6_summarytable.png]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Items table&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;pre&amp;gt;&lt;br /&gt;
Item               Value     Threshold  Converged?&lt;br /&gt;
 Maximum Force            0.000193     0.000450     YES&lt;br /&gt;
 RMS     Force            0.000079     0.000300     YES&lt;br /&gt;
 Maximum Displacement     0.000830     0.001800     YES&lt;br /&gt;
 RMS     Displacement     0.000294     0.001200     YES&lt;br /&gt;
&amp;lt;/pre&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Frequency log file&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
[[Media:HYC116_C6H6_FREQ.LOG]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Frequencies&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;pre&amp;gt;&lt;br /&gt;
Low frequencies ---   -3.5606   -3.5606   -0.0089   -0.0043   -0.0043   10.0905&lt;br /&gt;
Low frequencies ---  413.9582  413.9582  621.1416&lt;br /&gt;
&amp;lt;/pre&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;jmol of C&amp;lt;sub&amp;gt;6&amp;lt;/sub&amp;gt;H&amp;lt;sub&amp;gt;6&amp;lt;/sub&amp;gt;&#039;&#039;&#039;&lt;br /&gt;
&amp;lt;jmol&amp;gt;&amp;lt;jmolApplet&amp;gt;&lt;br /&gt;
  &amp;lt;title&amp;gt;optimised Benzene&amp;lt;/title&amp;gt;&lt;br /&gt;
  &amp;lt;color&amp;gt;black&amp;lt;/color&amp;gt;&lt;br /&gt;
  &amp;lt;size&amp;gt;200&amp;lt;/size&amp;gt;&lt;br /&gt;
  &amp;lt;uploadedFileContents&amp;gt;HYC116_C6H6_FREQ.LOG&amp;lt;/uploadedFileContents&amp;gt;&lt;br /&gt;
&amp;lt;/jmolApplet&amp;gt;&amp;lt;/jmol&amp;gt;&lt;br /&gt;
&lt;br /&gt;
===Borazine===&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;Calculation type&amp;lt;/b&amp;gt;: Optimisation&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;Calculation Method&amp;lt;/b&amp;gt;: B3LYP&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;Basis set&amp;lt;/b&amp;gt;: 6-31G(d,p) &lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Summary table&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
[[file:Hyc116_borazine_summarytable.png]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Items table&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;pre&amp;gt;&lt;br /&gt;
Item               Value     Threshold  Converged?&lt;br /&gt;
 Maximum Force            0.000085     0.000450     YES&lt;br /&gt;
 RMS     Force            0.000033     0.000300     YES&lt;br /&gt;
 Maximum Displacement     0.000250     0.001800     YES&lt;br /&gt;
 RMS     Displacement     0.000074     0.001200     YES&lt;br /&gt;
&amp;lt;/pre&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Frequency log file&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
[[Media:HYC116_BORAZINE_FREQ.LOG]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Frequencies&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;pre&amp;gt;&lt;br /&gt;
Low frequencies ---  -12.6626  -12.6626   -8.9272   -0.0211   -0.0104   -0.0104&lt;br /&gt;
Low frequencies ---  289.1112  289.1112  403.8613&lt;br /&gt;
&amp;lt;/pre&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;jmol of Borazine&#039;&#039;&#039;&lt;br /&gt;
&amp;lt;jmol&amp;gt;&amp;lt;jmolApplet&amp;gt;&lt;br /&gt;
  &amp;lt;title&amp;gt;optimised Borazine&amp;lt;/title&amp;gt;&lt;br /&gt;
  &amp;lt;color&amp;gt;black&amp;lt;/color&amp;gt;&lt;br /&gt;
  &amp;lt;size&amp;gt;200&amp;lt;/size&amp;gt;&lt;br /&gt;
  &amp;lt;uploadedFileContents&amp;gt;HYC116_BORAZINE_FREQ.LOG&amp;lt;/uploadedFileContents&amp;gt;&lt;br /&gt;
&amp;lt;/jmolApplet&amp;gt;&amp;lt;/jmol&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
===Charge distribution===&lt;br /&gt;
&lt;br /&gt;
An NBO charge analysis was carried out on both the optimised benzene and borazine. Visualisations of the charge distribution are shown in the table below, with the colour range going from -1.102 to 1.102 for both molecule. This large scale was chosen as it allows direct comparison of the charge on any atoms in these two molecules and shows the relative magnitude of charges on all these atoms. Negative charges are shown in red, and positive charges are shown in green. A neutral charge is displayed in black, so the smaller a charge is (positive or negative), the darker its colour representation is. Larger charges are shown in brighter colours. The charges are also displayed on the atoms as numbers with a neutral charge being zero. Negative charges are shown as negative number and positive charges are shown as positive numbers. &lt;br /&gt;
&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot;&lt;br /&gt;
!&lt;br /&gt;
!Benzene&lt;br /&gt;
!Borazine&lt;br /&gt;
|-&lt;br /&gt;
!Visualisation of charge distribution&lt;br /&gt;
|[[File:Hyc116_benzene_charge_distribution1.png|500x500px|thumb|centre|Charge distribution of Benzene visualisation]]&lt;br /&gt;
|[[File:Hyc116_borazine_charge_distribution1.png|500x500px|thumb|centre|Charge distribution of Borazine visualisation]]&lt;br /&gt;
|-&lt;br /&gt;
!Charge &lt;br /&gt;
|Carbon: -0.239&lt;br /&gt;
&lt;br /&gt;
Hydrogen: 0.239&lt;br /&gt;
|Nitrogen: -1.102 &lt;br /&gt;
&lt;br /&gt;
Boron: 0.747&lt;br /&gt;
&lt;br /&gt;
Hydrogen (bonded to N): 0.432&lt;br /&gt;
&lt;br /&gt;
Hydrogen (bonded to B): -0.077&lt;br /&gt;
|-&lt;br /&gt;
!Discussion&lt;br /&gt;
|From the visualisation, it is shown that there is a slightly negative charge on the carbon atoms, and a positive charge of the same magnitude on the hydrogen atoms. All the carbon atoms have the same charge as they are in identical environments. The same applies to all the hydrogen atoms. This is due to the highly symmetrical structure of benzene. Since the same colour scale was used for both benzene and borazine, and the charges are much smaller in magnitude on atoms in benzene than atoms on borazine, the colours on the charge distribution visualisation is much darker. &lt;br /&gt;
|Polar bonds between nitrogen and boron are demonstration from the above visualisation. From the colours displayed on the charge distribution visualisation as well as the charge values, it is shown that nitrogen has a relatively large negative charge, while boron has a positive charge. This is due to the difference in electrogenativity between these atoms: nitrogen atoms are more electronegative than boron and tends to attract electrons towards themselves. It is worth noting that the hydrogen atoms do not all have the same charge. The hydrogen atoms bonded to boron have a slightly negative charge, and the ones bonded to nitrogen have a small positive charge. &lt;br /&gt;
&lt;br /&gt;
The fact that the same colour scale was used for both molecules comes in helpful here. It allows the charges on atoms to be compared directly. For example, just from looking at the colours, one can tell that or example, even though both carbon and nitrogen are electronegative, nitrogen is much more electronegative, which is quantitatively shown by Pauling&#039;s electronegativity scale.&amp;lt;ref&amp;gt;http://www.tutor-homework.com/Chemistry_Help/electronegativity_table/electronegativity.html (Accessed: 24.05.2018)&amp;lt;/ref&amp;gt;&lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
===Comparative MOs of Benzene and Borazine===&lt;br /&gt;
&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot;&lt;br /&gt;
!&lt;br /&gt;
!Benzene&lt;br /&gt;
!Borazine&lt;br /&gt;
!Comparison and Discussion&lt;br /&gt;
|-&lt;br /&gt;
!1st comparative pair&lt;br /&gt;
|[[File:Hyc116_benzene_1st_MO_pair_7.png|200x200px|centre]]&lt;br /&gt;
|[[File:Hyc116_borazine_1st_MO_pair_level9.png|200x200px|centre]]&lt;br /&gt;
|MO 9 of both benzene and borazine are comparable. They both show delocalised molecular orbital with an overall bonding character. There is a nodal plane across the molecular orbitals for both benzene and borazine. For benzene, there is contribution from all the carbon and hydrogen s orbitals. Moreover, the molecular orbitals are symmetric to their counterpart of opposite phase, giving an E&amp;lt;sub&amp;gt;1g&amp;lt;/sub&amp;gt; MO. That is not the case for borazine; they are less symmetric in borazine. This MO of borazine has an E&#039; symmetry. Nitrogen atoms are more electronegative than boron atoms and pull electron density towards themselves, resulting in a larger lobe. There is contribution from all the boron and nitrogen s orbitals, and three of the hydrogen s orbitals, though not all of them. &lt;br /&gt;
|-&lt;br /&gt;
!2nd comparative pair&lt;br /&gt;
|[[File:Hyc116_benzene_2nd_MO_pair_10.png|200x200px|centre]]&lt;br /&gt;
|[[File:Hyc116_borazine_2nd_MO_pair_level11.png|200x200px|centre]]&lt;br /&gt;
|MO 10 of benzene and MO 11 of borazine are comparable. Here shows a pair of rather delocalised molecular orbitals with slightly more antibonding character than the first pair shown above. On both MOs, there is no contribution from one pair of opposite hydrogen atoms, but contribution from s orbitals of all other atoms on both molecule. The benzene MO has an E&amp;lt;sub&amp;gt;2g&amp;lt;/sub&amp;gt; symmetry. In borazine, the lobes are in different sizes due to the higher electronegativity of nitrogen. The lobes at the nitrogen atoms are larger as they attract electrons towards themselves more so than boron atoms do. This borazine MO has an E&#039; symmetry. &lt;br /&gt;
|-&lt;br /&gt;
!3rd comparative pair&lt;br /&gt;
|[[File:Hyc116_benzene_3rd_MO_pair_21.png|200x200px|centre]]&lt;br /&gt;
|[[File:Hyc116_borazine_3rd_MO_pair_level21.png|200x200px|centre]]&lt;br /&gt;
|The HOMO (MO 21) of benzene and the HOMO (MO 21) of borazine are comparable. They are both made of p orbitals of all carbon atoms (or all boron and nitrogen atoms in the case of borazine); there is no contribution from hydrogen atoms as they do not have p orbitals. There is a nodal plan perpendicular to the z axis (highest rotational axis) and one parallel to the z axis. On benzene, the MO is very symmetric and has an E&amp;lt;sub&amp;gt;1g&amp;lt;/sub&amp;gt; symmetry; the lobes of the MO are the same in size. On borazine, the lobe where there are two nitrogen atoms is bigger in size, again due to the higher electronegtivity of nitrogen compared to boron. The borazine MO has an E&#039; &#039; symmetry.&lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
===Aromaticity: discussion===&lt;br /&gt;
&lt;br /&gt;
Aromatic compounds display properties such as their high stability and bond lengths between typical single and double bonds. A simple understanding of aromaticity involves the overlap of p orbitals perpendicular to the cyclic plane; the delocalisation of electrons on the pi system is identified to be responsible of the stability of aromatic systems. Aromatic compounds can be identified by the Huckel’s rule, which states that conjugated planar cyclic molecules with (4n +2) π electrons are aromatic. Both benzene and borazine obey the Huckel’s rule and fit the conventional description of aromaticity. &amp;lt;ref&amp;gt;Clayden, J., Greeves, N. &amp;amp; Warren, S. G. Organic chemistry. (Oxford University Press, 2012)&amp;lt;/ref&amp;gt;&lt;br /&gt;
&lt;br /&gt;
However, it is proved in recent years that the conventional criteria do not necessarily have to be obeyed for a compound to be aromatic. For instance, there has been shown that some non-planar compounds display aromaticity. This suggests that the criteria for aromaticity is not simply structural, and these advances give rise to concepts such as quasiaromaticity and pseudoaromaticity. Recent advances show that there are quantum mechanics basis on the idea of aromaticity.&amp;lt;ref&amp;gt;Palusiak, M. &amp;amp; Krygowski, T. M. Application of AIM Parameters at Ring Critical Points for Estimation of π-Electron Delocalization in Six-Membered Aromatic and Quasi-Aromatic Rings. Chemistry - A European Journal 13, 7996–8006 (2007).&amp;lt;/ref&amp;gt; &lt;br /&gt;
&lt;br /&gt;
In conclusion, while the overlap of pi orbitals provides a simple understanding for aromaticity, it is not a sufficient description for aromaticity. There is also sigma orbital and quantum mechanics contribution to aromaticity.&lt;br /&gt;
&lt;br /&gt;
==References==&lt;/div&gt;</summary>
		<author><name>Hyc116</name></author>
	</entry>
	<entry>
		<id>https://chemwiki.ch.ic.ac.uk/index.php?title=MO_hyc116&amp;diff=732637</id>
		<title>MO hyc116</title>
		<link rel="alternate" type="text/html" href="https://chemwiki.ch.ic.ac.uk/index.php?title=MO_hyc116&amp;diff=732637"/>
		<updated>2018-05-25T15:37:27Z</updated>

		<summary type="html">&lt;p&gt;Hyc116: /* Aromaticity: discussion */&lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;==BH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;==&lt;br /&gt;
&lt;br /&gt;
===standard information===&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;Calculation type&amp;lt;/b&amp;gt;: Optimisation&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;Calculation Method&amp;lt;/b&amp;gt;: B3LYP&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;Basis set&amp;lt;/b&amp;gt;: 6-31G(d,p) &lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Summary table&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
[[file:Hyc116_bh3_631g_opt_summarytable.png]]&lt;br /&gt;
&lt;br /&gt;
The above summary table was obtained after the 2nd optimisation of BH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt; (after the initial optimisation using the 3-21G basis set). Notice how the symmetry is incorrect and shown as Cs. This is because the symmetry was manually broken at the beginning by changing the bond length of B-H bonds. The point group was manually adjusted and the molecule was optimised again before the frequency analysis and the new summary table is attached below.&lt;br /&gt;
&lt;br /&gt;
[[file:Hyc116_bh3_correctsummarytable.png]]&lt;br /&gt;
&lt;br /&gt;
The above summary table was obtained from the optimisation after adjusting the symmetry. The point shown in this summary table is D&amp;lt;sub&amp;gt;3h&amp;lt;/sub&amp;gt;, which is the correct for BH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;. &lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Items table&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
Below is the items table taken from the optimisation with the correct point group.&lt;br /&gt;
&lt;br /&gt;
&amp;lt;pre&amp;gt;&lt;br /&gt;
Item               Value     Threshold  Converged?&lt;br /&gt;
 Maximum Force            0.000015     0.000450     YES&lt;br /&gt;
 RMS     Force            0.000010     0.000300     YES&lt;br /&gt;
 Maximum Displacement     0.000058     0.001800     YES&lt;br /&gt;
 RMS     Displacement     0.000038     0.001200     YES&lt;br /&gt;
&amp;lt;/pre&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Frequency log file&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
[[Media:HYC116 BH3 FREQ.LOG]] &lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Frequencies&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;pre&amp;gt;&lt;br /&gt;
Low frequencies ---  -10.3498   -3.4492   -1.2454   -0.0055    0.4779    3.2165&lt;br /&gt;
Low frequencies --- 1162.9519 1213.1527 1213.1554&lt;br /&gt;
&amp;lt;/pre&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;jmol of BH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;&#039;&#039;&#039;&lt;br /&gt;
&amp;lt;jmol&amp;gt;&amp;lt;jmolApplet&amp;gt;&lt;br /&gt;
  &amp;lt;title&amp;gt;optimised BH3&amp;lt;/title&amp;gt;&lt;br /&gt;
  &amp;lt;color&amp;gt;black&amp;lt;/color&amp;gt;&lt;br /&gt;
  &amp;lt;size&amp;gt;200&amp;lt;/size&amp;gt;&lt;br /&gt;
  &amp;lt;uploadedFileContents&amp;gt;HYC116_BH3_FREQ.LOG&amp;lt;/uploadedFileContents&amp;gt;&lt;br /&gt;
&amp;lt;/jmolApplet&amp;gt;&amp;lt;/jmol&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
===Vibrational spectrum===&lt;br /&gt;
&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot;&lt;br /&gt;
!wavenumber (cm&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;)&lt;br /&gt;
!Intensity (arbitrary units)&lt;br /&gt;
!symmetry&lt;br /&gt;
!IR active?&lt;br /&gt;
!type&lt;br /&gt;
|-&lt;br /&gt;
|1163&lt;br /&gt;
|93&lt;br /&gt;
|A&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;&#039; &#039;&lt;br /&gt;
|Yes&lt;br /&gt;
|Out of plane bend&lt;br /&gt;
|-&lt;br /&gt;
|1213&lt;br /&gt;
|14&lt;br /&gt;
|E&#039;&lt;br /&gt;
|Very slight&lt;br /&gt;
|Bend&lt;br /&gt;
|-&lt;br /&gt;
|1213&lt;br /&gt;
|14&lt;br /&gt;
|E&#039;&lt;br /&gt;
|Very slight&lt;br /&gt;
|Bend&lt;br /&gt;
|-&lt;br /&gt;
|2582&lt;br /&gt;
|0&lt;br /&gt;
|A&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;&#039;&lt;br /&gt;
|No&lt;br /&gt;
|Symmetric stretch&lt;br /&gt;
|-&lt;br /&gt;
|2716&lt;br /&gt;
|126&lt;br /&gt;
|E&#039;&lt;br /&gt;
|Yes&lt;br /&gt;
|Asymmetric stretch&lt;br /&gt;
|-&lt;br /&gt;
|2716&lt;br /&gt;
|126&lt;br /&gt;
|E&#039;&lt;br /&gt;
|Yes&lt;br /&gt;
|Asymmetric stretch&lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;IR spectrum&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
[[file:Hyc116_ir_bh3.png|400*600]]&lt;br /&gt;
&lt;br /&gt;
There are only three peaks on the IR spectrum of BH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;, despite that there are 6 vibrational modes for the molecule. As shown in the table above, the symmetric stretching mode with A1 symmetry at 2582 cm&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt; is not IR active; naturally, that vibrational mode doesn’t give a peak on the IR spectrum. As shown from the table, two pairs of vibrational modes, the bond angle deformation/bend at 1213 cm&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt; and the asymmetric bond stretch at 2716 cm&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;, are degenerate with the symmetry label E. This means that they have the same energy, and hence give the same wavenumber on the IR spectrum. Each pair of degenerate vibrational modes give rise to one peak. This leaves three peaks, as confirmed by the IR spectrum above.&lt;br /&gt;
&lt;br /&gt;
===Molecular orbitals of BH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;===&lt;br /&gt;
&lt;br /&gt;
[[file:hyc116_bh3_MO_diagram.png]]&lt;br /&gt;
&lt;br /&gt;
The above molecular orbital diagram was taken from Dr Patricia Hunt&#039;s &amp;lt;i&amp;gt;Lecture 4 Tutorial Problem Model Answers&amp;lt;/i&amp;gt;.&amp;lt;ref&amp;gt;P. Hunt, &amp;quot;Lecture 4 Tutorial Problem Model Answers&amp;quot;, 2 (2018)&amp;lt;/ref&amp;gt; Diagrams of the &amp;quot;real&amp;quot; MOs were obtained from Gaussian.&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
There is no significant difference between the LCAO MOs and the real ones. Features such as orbital phases are shown clearly on both the LCAO MOs and the real MOs, illustrating the bonding/anti-bonding characters of the molecular orbitals. This suggests that the the qualitative MO theory is highly accurate and useful when studying the molecular orbitals of molecules.&lt;br /&gt;
&lt;br /&gt;
==Associated energies: ammonium borane==&lt;br /&gt;
&lt;br /&gt;
===NH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;===&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;Calculation type&amp;lt;/b&amp;gt;: Optimisation&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;Calculation Method&amp;lt;/b&amp;gt;: B3LYP&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;Basis set&amp;lt;/b&amp;gt;: 6-31G(d,p) &lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Summary table&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
[[file:Hyc116_nh3_631g_summarytable.png]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Items table&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;pre&amp;gt;&lt;br /&gt;
Item               Value     Threshold  Converged?&lt;br /&gt;
 Maximum Force            0.000006     0.000450     YES&lt;br /&gt;
 RMS     Force            0.000004     0.000300     YES&lt;br /&gt;
 Maximum Displacement     0.000012     0.001800     YES&lt;br /&gt;
 RMS     Displacement     0.000008     0.001200     YES&lt;br /&gt;
&amp;lt;/pre&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Frequency log file&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
[[Media:HYC116_NH3_FREQ.LOG]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Frequencies&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;pre&amp;gt;&lt;br /&gt;
Low frequencies ---   -8.5646   -8.5588   -0.0047    0.0454    0.1784   26.4183&lt;br /&gt;
Low frequencies --- 1089.7603 1694.1865 1694.1865&lt;br /&gt;
&amp;lt;/pre&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;jmol of NH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;&#039;&#039;&#039;&lt;br /&gt;
&amp;lt;jmol&amp;gt;&amp;lt;jmolApplet&amp;gt;&lt;br /&gt;
  &amp;lt;title&amp;gt;optimised NH3&amp;lt;/title&amp;gt;&lt;br /&gt;
  &amp;lt;color&amp;gt;black&amp;lt;/color&amp;gt;&lt;br /&gt;
  &amp;lt;size&amp;gt;200&amp;lt;/size&amp;gt;&lt;br /&gt;
  &amp;lt;uploadedFileContents&amp;gt;HYC116_NH3_FREQ.LOG&amp;lt;/uploadedFileContents&amp;gt;&lt;br /&gt;
&amp;lt;/jmolApplet&amp;gt;&amp;lt;/jmol&amp;gt;&lt;br /&gt;
&lt;br /&gt;
===NH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;BH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;===&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;Calculation type&amp;lt;/b&amp;gt;: Optimisation&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;Calculation Method&amp;lt;/b&amp;gt;: B3LYP&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;Basis set&amp;lt;/b&amp;gt;: 6-31G(d,p) &lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Summary table&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
[[file:Hyc116_nh3bh3_631g_summarytable1.png]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Items table&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;pre&amp;gt;&lt;br /&gt;
Item               Value     Threshold  Converged?&lt;br /&gt;
 Maximum Force            0.000121     0.000450     YES&lt;br /&gt;
 RMS     Force            0.000057     0.000300     YES&lt;br /&gt;
 Maximum Displacement     0.000501     0.001800     YES&lt;br /&gt;
 RMS     Displacement     0.000293     0.001200     YES&lt;br /&gt;
&amp;lt;/pre&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Frequency log file&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
[[Media:HYC116_NH3BH3_FREQ1.LOG]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Frequencies&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;pre&amp;gt;&lt;br /&gt;
Low frequencies ---   -0.0574   -0.0501   -0.0074   21.6276   21.6377   40.3839&lt;br /&gt;
Low frequencies ---  265.9973  632.3725  640.1275&lt;br /&gt;
&amp;lt;/pre&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;jmol of NH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;BH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;&#039;&#039;&#039;&lt;br /&gt;
&amp;lt;jmol&amp;gt;&amp;lt;jmolApplet&amp;gt;&lt;br /&gt;
  &amp;lt;title&amp;gt;optimised NH3BH3&amp;lt;/title&amp;gt;&lt;br /&gt;
  &amp;lt;color&amp;gt;black&amp;lt;/color&amp;gt;&lt;br /&gt;
  &amp;lt;size&amp;gt;200&amp;lt;/size&amp;gt;&lt;br /&gt;
  &amp;lt;uploadedFileContents&amp;gt;HYC116_NH3BH3_FREQ.LOG&amp;lt;/uploadedFileContents&amp;gt;&lt;br /&gt;
&amp;lt;/jmolApplet&amp;gt;&amp;lt;/jmol&amp;gt;&lt;br /&gt;
&lt;br /&gt;
===Association energy===&lt;br /&gt;
&lt;br /&gt;
E(BH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;) (using the optimisation with the correct symmetry) = -26.61532363 a.u. = &amp;lt;b&amp;gt;-26.61532 a.u. (5 d.p.)&amp;lt;/b&amp;gt;&lt;br /&gt;
&lt;br /&gt;
E(NH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;) = -56.55776873 a.u. = &amp;lt;b&amp;gt;-56.55777 a.u. (5 d.p.)&amp;lt;/b&amp;gt;&lt;br /&gt;
&lt;br /&gt;
E(NH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;BH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;) = -83.22468892 a.u. = &amp;lt;b&amp;gt;-83.22469 a.u. (5 d.p.)&amp;lt;/b&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
Carrying out calculations using numbers which has already been rounded up can possibly result in errors in the last digit. Hence, here the calculations were carried out using the numbers provided from the optimisations (i.e. with more decimal places than necessary); the answer was then rounded up to the desired accuracy. &lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
ΔE = E(NH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;BH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;)-[E(NH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;)+E(BH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;)]&lt;br /&gt;
&lt;br /&gt;
ΔE = -83.22468892 - (-56.55776873 + -26.61532363) = -0.05159656 a.u. &lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;ΔE = -0.05160 a.u. (5 d.p.)&amp;lt;/b&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Converting energy from a.u. to kJ/mol&#039;&#039;&#039;&lt;br /&gt;
An atomic unit for energy is Hartree, which is equal to 2625.5 kJ/mol.&lt;br /&gt;
&amp;lt;ref&amp;gt;https://cccbdb.nist.gov/hartree.asp (Accessed: 22.05.2018)&amp;lt;/ref&amp;gt;&lt;br /&gt;
 &lt;br /&gt;
&lt;br /&gt;
So ΔE in kJ/mol = -0.05159657 * 2625.5 = -135.46676828 kJ/mol&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;ΔE = -135 kJ/mol (nearest integer)&amp;lt;/b&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
The energy difference calculated above comes from the formation of the B-N dative bond. It is a relatively weak bond. According to a bond energy data sheet provided by the University of California,&amp;lt;ref&amp;gt;https://labs.chem.ucsb.edu/zakarian/armen/11---bonddissociationenergy.pdf (Accessed: 24.05.2018)&amp;lt;/ref&amp;gt;  the bond energy of the C-C bond of an ethane molecule is 368 kJ/mol. This is a fair comparison to the NH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;BH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt; molecule as the two molecules have the same structure, only with the carbon atoms on ethane swapped for Boron and Nitrogen in NH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;BH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;&lt;br /&gt;
&lt;br /&gt;
==Using a mixture of basis-sets and pseudo-potentials==&lt;br /&gt;
&lt;br /&gt;
===BBr&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;===&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;Calculation type&amp;lt;/b&amp;gt;: Optimisation&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;Calculation Method&amp;lt;/b&amp;gt;: B3LYP&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;Basis set&amp;lt;/b&amp;gt;: Boron: 6-31G(d,p) ; Br: LANL2DZ&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
Larger calculations are often sent to a web-server to run on a high-performance computer instead of a desktop. In order to experience and learn to use a web-server, the optimisation and the frequency analysis for BBr&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt; were both sent and done on a server instead of the desktop. The calculation results were downloaded from the web-server once they were finished.   &lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Summary table&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
[[file:Hyc116_bbr3_opt_summarytable.png]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Items table&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;pre&amp;gt;&lt;br /&gt;
Item               Value     Threshold  Converged?&lt;br /&gt;
 Maximum Force            0.000008     0.000450     YES&lt;br /&gt;
 RMS     Force            0.000005     0.000300     YES&lt;br /&gt;
 Maximum Displacement     0.000036     0.001800     YES&lt;br /&gt;
 RMS     Displacement     0.000023     0.001200     YES&lt;br /&gt;
&amp;lt;/pre&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Frequency log file&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
[[Media:Hyc116_bbr3_freq.log]]&lt;br /&gt;
&lt;br /&gt;
Attached above is the frequency file saved onto the computer from the SCAN server portal. The frequency file was also published on the chemistry database DSpace. {{DOI|10042/202442}}&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Frequencies&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;pre&amp;gt;&lt;br /&gt;
Low frequencies ---   -0.0137   -0.0064   -0.0046    2.4315    2.4315    4.8421&lt;br /&gt;
Low frequencies ---  155.9631  155.9651  267.7052&lt;br /&gt;
&amp;lt;/pre&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;jmol of BBr&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;&#039;&#039;&#039;&lt;br /&gt;
&amp;lt;jmol&amp;gt;&amp;lt;jmolApplet&amp;gt;&lt;br /&gt;
  &amp;lt;title&amp;gt;optimised BBr3&amp;lt;/title&amp;gt;&lt;br /&gt;
  &amp;lt;color&amp;gt;black&amp;lt;/color&amp;gt;&lt;br /&gt;
  &amp;lt;size&amp;gt;200&amp;lt;/size&amp;gt;&lt;br /&gt;
  &amp;lt;uploadedFileContents&amp;gt;Hyc116_bbr3_freq.log&amp;lt;/uploadedFileContents&amp;gt;&lt;br /&gt;
&amp;lt;/jmolApplet&amp;gt;&amp;lt;/jmol&amp;gt;&lt;br /&gt;
&lt;br /&gt;
==Mini project: Aromaticity==&lt;br /&gt;
&lt;br /&gt;
===Benzene===&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;Calculation type&amp;lt;/b&amp;gt;: Optimisation&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;Calculation Method&amp;lt;/b&amp;gt;: B3LYP&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;Basis set&amp;lt;/b&amp;gt;: 6-31G(d,p) &lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Summary table&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
[[file:Hyc116_c6h6_summarytable.png]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Items table&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;pre&amp;gt;&lt;br /&gt;
Item               Value     Threshold  Converged?&lt;br /&gt;
 Maximum Force            0.000193     0.000450     YES&lt;br /&gt;
 RMS     Force            0.000079     0.000300     YES&lt;br /&gt;
 Maximum Displacement     0.000830     0.001800     YES&lt;br /&gt;
 RMS     Displacement     0.000294     0.001200     YES&lt;br /&gt;
&amp;lt;/pre&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Frequency log file&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
[[Media:HYC116_C6H6_FREQ.LOG]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Frequencies&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;pre&amp;gt;&lt;br /&gt;
Low frequencies ---   -3.5606   -3.5606   -0.0089   -0.0043   -0.0043   10.0905&lt;br /&gt;
Low frequencies ---  413.9582  413.9582  621.1416&lt;br /&gt;
&amp;lt;/pre&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;jmol of C&amp;lt;sub&amp;gt;6&amp;lt;/sub&amp;gt;H&amp;lt;sub&amp;gt;6&amp;lt;/sub&amp;gt;&#039;&#039;&#039;&lt;br /&gt;
&amp;lt;jmol&amp;gt;&amp;lt;jmolApplet&amp;gt;&lt;br /&gt;
  &amp;lt;title&amp;gt;optimised Benzene&amp;lt;/title&amp;gt;&lt;br /&gt;
  &amp;lt;color&amp;gt;black&amp;lt;/color&amp;gt;&lt;br /&gt;
  &amp;lt;size&amp;gt;200&amp;lt;/size&amp;gt;&lt;br /&gt;
  &amp;lt;uploadedFileContents&amp;gt;HYC116_C6H6_FREQ.LOG&amp;lt;/uploadedFileContents&amp;gt;&lt;br /&gt;
&amp;lt;/jmolApplet&amp;gt;&amp;lt;/jmol&amp;gt;&lt;br /&gt;
&lt;br /&gt;
===Borazine===&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;Calculation type&amp;lt;/b&amp;gt;: Optimisation&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;Calculation Method&amp;lt;/b&amp;gt;: B3LYP&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;Basis set&amp;lt;/b&amp;gt;: 6-31G(d,p) &lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Summary table&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
[[file:Hyc116_borazine_summarytable.png]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Items table&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;pre&amp;gt;&lt;br /&gt;
Item               Value     Threshold  Converged?&lt;br /&gt;
 Maximum Force            0.000085     0.000450     YES&lt;br /&gt;
 RMS     Force            0.000033     0.000300     YES&lt;br /&gt;
 Maximum Displacement     0.000250     0.001800     YES&lt;br /&gt;
 RMS     Displacement     0.000074     0.001200     YES&lt;br /&gt;
&amp;lt;/pre&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Frequency log file&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
[[Media:HYC116_BORAZINE_FREQ.LOG]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Frequencies&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;pre&amp;gt;&lt;br /&gt;
Low frequencies ---  -12.6626  -12.6626   -8.9272   -0.0211   -0.0104   -0.0104&lt;br /&gt;
Low frequencies ---  289.1112  289.1112  403.8613&lt;br /&gt;
&amp;lt;/pre&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;jmol of Borazine&#039;&#039;&#039;&lt;br /&gt;
&amp;lt;jmol&amp;gt;&amp;lt;jmolApplet&amp;gt;&lt;br /&gt;
  &amp;lt;title&amp;gt;optimised Borazine&amp;lt;/title&amp;gt;&lt;br /&gt;
  &amp;lt;color&amp;gt;black&amp;lt;/color&amp;gt;&lt;br /&gt;
  &amp;lt;size&amp;gt;200&amp;lt;/size&amp;gt;&lt;br /&gt;
  &amp;lt;uploadedFileContents&amp;gt;HYC116_BORAZINE_FREQ.LOG&amp;lt;/uploadedFileContents&amp;gt;&lt;br /&gt;
&amp;lt;/jmolApplet&amp;gt;&amp;lt;/jmol&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
===Charge distribution===&lt;br /&gt;
&lt;br /&gt;
An NBO charge analysis was carried out on both the optimised benzene and borazine. Visualisations of the charge distribution are shown in the table below, with the colour range going from -1.102 to 1.102 for both molecule. This large scale was chosen as it allows direct comparison of the charge on any atoms in these two molecules and shows the relative magnitude of charges on all these atoms. Negative charges are shown in red, and positive charges are shown in green. A neutral charge is displayed in black, so the smaller a charge is (positive or negative), the darker its colour representation is. Larger charges are shown in brighter colours. The charges are also displayed on the atoms as numbers with a neutral charge being zero. Negative charges are shown as negative number and positive charges are shown as positive numbers. &lt;br /&gt;
&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot;&lt;br /&gt;
!&lt;br /&gt;
!Benzene&lt;br /&gt;
!Borazine&lt;br /&gt;
|-&lt;br /&gt;
!Visualisation of charge distribution&lt;br /&gt;
|[[File:Hyc116_benzene_charge_distribution1.png|500x500px|thumb|centre|Charge distribution of Benzene visualisation]]&lt;br /&gt;
|[[File:Hyc116_borazine_charge_distribution1.png|500x500px|thumb|centre|Charge distribution of Borazine visualisation]]&lt;br /&gt;
|-&lt;br /&gt;
!Charge &lt;br /&gt;
|Carbon: -0.239&lt;br /&gt;
&lt;br /&gt;
Hydrogen: 0.239&lt;br /&gt;
|Nitrogen: -1.102 &lt;br /&gt;
&lt;br /&gt;
Boron: 0.747&lt;br /&gt;
&lt;br /&gt;
Hydrogen (bonded to N): 0.432&lt;br /&gt;
&lt;br /&gt;
Hydrogen (bonded to B): -0.077&lt;br /&gt;
|-&lt;br /&gt;
!Discussion&lt;br /&gt;
|From the visualisation, it is shown that there is a slightly negative charge on the carbon atoms, and a positive charge of the same magnitude on the hydrogen atoms. All the carbon atoms have the same charge as they are in identical environments. The same applies to all the hydrogen atoms. This is due to the highly symmetrical structure of benzene. Since the same colour scale was used for both benzene and borazine, and the charges are much smaller in magnitude on atoms in benzene than atoms on borazine, the colours on the charge distribution visualisation is much darker. &lt;br /&gt;
|Polar bonds between nitrogen and boron are demonstration from the above visualisation. From the colours displayed on the charge distribution visualisation as well as the charge values, it is shown that nitrogen has a relatively large negative charge, while boron has a positive charge. This is due to the difference in electrogenativity between these atoms: nitrogen atoms are more electronegative than boron and tends to attract electrons towards themselves. It is worth noting that the hydrogen atoms do not all have the same charge. The hydrogen atoms bonded to boron have a slightly negative charge, and the ones bonded to nitrogen have a small positive charge. &lt;br /&gt;
&lt;br /&gt;
The fact that the same colour scale was used for both molecules comes in helpful here. It allows the charges on atoms to be compared directly. For example, just from looking at the colours, one can tell that or example, even though both carbon and nitrogen are electronegative, nitrogen is much more electronegative, which is quantitatively shown by Pauling&#039;s electronegativity scale.&amp;lt;ref&amp;gt;http://www.tutor-homework.com/Chemistry_Help/electronegativity_table/electronegativity.html (Accessed: 24.0502018&amp;lt;/ref&amp;gt;&lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
===Comparative MOs of Benzene and Borazine===&lt;br /&gt;
&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot;&lt;br /&gt;
!&lt;br /&gt;
!Benzene&lt;br /&gt;
!Borazine&lt;br /&gt;
!Comparison and Discussion&lt;br /&gt;
|-&lt;br /&gt;
!1st comparative pair&lt;br /&gt;
|[[File:Hyc116_benzene_1st_MO_pair_7.png|200x200px|centre]]&lt;br /&gt;
|[[File:Hyc116_borazine_1st_MO_pair_level9.png|200x200px|centre]]&lt;br /&gt;
|MO 9 of both benzene and borazine are comparable. They both show delocalised molecular orbital with an overall bonding character. There is a nodal plane across the molecular orbitals for both benzene and borazine. For benzene, there is contribution from all the carbon and hydrogen s orbitals. Moreover, the molecular orbitals are symmetric to their counterpart of opposite phase, giving an E&amp;lt;sub&amp;gt;1g&amp;lt;/sub&amp;gt; MO. That is not the case for borazine; they are less symmetric in borazine. This MO of borazine has an E&#039; symmetry. Nitrogen atoms are more electronegative than boron atoms and pull electron density towards themselves, resulting in a larger lobe. There is contribution from all the boron and nitrogen s orbitals, and three of the hydrogen s orbitals, though not all of them. &lt;br /&gt;
|-&lt;br /&gt;
!2nd comparative pair&lt;br /&gt;
|[[File:Hyc116_benzene_2nd_MO_pair_10.png|200x200px|centre]]&lt;br /&gt;
|[[File:Hyc116_borazine_2nd_MO_pair_level11.png|200x200px|centre]]&lt;br /&gt;
|MO 10 of benzene and MO 11 of borazine are comparable. Here shows a pair of rather delocalised molecular orbitals with slightly more antibonding character than the first pair shown above. On both MOs, there is no contribution from one pair of opposite hydrogen atoms, but contribution from s orbitals of all other atoms on both molecule. The benzene MO has an E&amp;lt;sub&amp;gt;2g&amp;lt;/sub&amp;gt; symmetry. In borazine, the lobes are in different sizes due to the higher electronegativity of nitrogen. The lobes at the nitrogen atoms are larger as they attract electrons towards themselves more so than boron atoms do. This borazine MO has an E&#039; symmetry. &lt;br /&gt;
|-&lt;br /&gt;
!3rd comparative pair&lt;br /&gt;
|[[File:Hyc116_benzene_3rd_MO_pair_21.png|200x200px|centre]]&lt;br /&gt;
|[[File:Hyc116_borazine_3rd_MO_pair_level21.png|200x200px|centre]]&lt;br /&gt;
|The HOMO (MO 21) of benzene and the HOMO (MO 21) of borazine are comparable. They are both made of p orbitals of all carbon atoms (or all boron and nitrogen atoms in the case of borazine); there is no contribution from hydrogen atoms as they do not have p orbitals. There is a nodal plan perpendicular to the z axis (highest rotational axis) and one parallel to the z axis. On benzene, the MO is very symmetric and has an E&amp;lt;sub&amp;gt;1g&amp;lt;/sub&amp;gt; symmetry; the lobes of the MO are the same in size. On borazine, the lobe where there are two nitrogen atoms is bigger in size, again due to the higher electronegtivity of nitrogen compared to boron. The borazine MO has an E&#039; &#039; symmetry.&lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
===Aromaticity: discussion===&lt;br /&gt;
&lt;br /&gt;
Aromatic compounds display properties such as their high stability and bond lengths between typical single and double bonds. A simple understanding of aromaticity involves the overlap of p orbitals perpendicular to the cyclic plane; the delocalisation of electrons on the pi system is identified to be responsible of the stability of aromatic systems. Aromatic compounds can be identified by the Huckel’s rule, which states that conjugated planar cyclic molecules with (4n +2) π electrons are aromatic. Both benzene and borazine obey the Huckel’s rule and fit the conventional description of aromaticity. &amp;lt;ref&amp;gt;Clayden, J., Greeves, N. &amp;amp; Warren, S. G. Organic chemistry. (Oxford University Press, 2012)&amp;lt;/ref&amp;gt;&lt;br /&gt;
&lt;br /&gt;
However, it is proved in recent years that the conventional criteria do not necessarily have to be obeyed for a compound to be aromatic. For instance, there has been shown that some non-planar compounds display aromaticity. This suggests that the criteria for aromaticity is not simply structural, and these advances give rise to concepts such as quasiaromaticity and pseudoaromaticity. Recent advances show that there are quantum mechanics basis on the idea of aromaticity.&amp;lt;ref&amp;gt;Palusiak, M. &amp;amp; Krygowski, T. M. Application of AIM Parameters at Ring Critical Points for Estimation of π-Electron Delocalization in Six-Membered Aromatic and Quasi-Aromatic Rings. Chemistry - A European Journal 13, 7996–8006 (2007).&amp;lt;/ref&amp;gt; &lt;br /&gt;
&lt;br /&gt;
In conclusion, while the overlap of pi orbitals provides a simple understanding for aromaticity, it is not a sufficient description for aromaticity. There is also sigma orbital and quantum mechanics contribution to aromaticity.&lt;br /&gt;
&lt;br /&gt;
==References==&lt;/div&gt;</summary>
		<author><name>Hyc116</name></author>
	</entry>
	<entry>
		<id>https://chemwiki.ch.ic.ac.uk/index.php?title=MO_hyc116&amp;diff=732629</id>
		<title>MO hyc116</title>
		<link rel="alternate" type="text/html" href="https://chemwiki.ch.ic.ac.uk/index.php?title=MO_hyc116&amp;diff=732629"/>
		<updated>2018-05-25T15:36:07Z</updated>

		<summary type="html">&lt;p&gt;Hyc116: /* References */&lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;==BH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;==&lt;br /&gt;
&lt;br /&gt;
===standard information===&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;Calculation type&amp;lt;/b&amp;gt;: Optimisation&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;Calculation Method&amp;lt;/b&amp;gt;: B3LYP&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;Basis set&amp;lt;/b&amp;gt;: 6-31G(d,p) &lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Summary table&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
[[file:Hyc116_bh3_631g_opt_summarytable.png]]&lt;br /&gt;
&lt;br /&gt;
The above summary table was obtained after the 2nd optimisation of BH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt; (after the initial optimisation using the 3-21G basis set). Notice how the symmetry is incorrect and shown as Cs. This is because the symmetry was manually broken at the beginning by changing the bond length of B-H bonds. The point group was manually adjusted and the molecule was optimised again before the frequency analysis and the new summary table is attached below.&lt;br /&gt;
&lt;br /&gt;
[[file:Hyc116_bh3_correctsummarytable.png]]&lt;br /&gt;
&lt;br /&gt;
The above summary table was obtained from the optimisation after adjusting the symmetry. The point shown in this summary table is D&amp;lt;sub&amp;gt;3h&amp;lt;/sub&amp;gt;, which is the correct for BH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;. &lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Items table&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
Below is the items table taken from the optimisation with the correct point group.&lt;br /&gt;
&lt;br /&gt;
&amp;lt;pre&amp;gt;&lt;br /&gt;
Item               Value     Threshold  Converged?&lt;br /&gt;
 Maximum Force            0.000015     0.000450     YES&lt;br /&gt;
 RMS     Force            0.000010     0.000300     YES&lt;br /&gt;
 Maximum Displacement     0.000058     0.001800     YES&lt;br /&gt;
 RMS     Displacement     0.000038     0.001200     YES&lt;br /&gt;
&amp;lt;/pre&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Frequency log file&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
[[Media:HYC116 BH3 FREQ.LOG]] &lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Frequencies&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;pre&amp;gt;&lt;br /&gt;
Low frequencies ---  -10.3498   -3.4492   -1.2454   -0.0055    0.4779    3.2165&lt;br /&gt;
Low frequencies --- 1162.9519 1213.1527 1213.1554&lt;br /&gt;
&amp;lt;/pre&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;jmol of BH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;&#039;&#039;&#039;&lt;br /&gt;
&amp;lt;jmol&amp;gt;&amp;lt;jmolApplet&amp;gt;&lt;br /&gt;
  &amp;lt;title&amp;gt;optimised BH3&amp;lt;/title&amp;gt;&lt;br /&gt;
  &amp;lt;color&amp;gt;black&amp;lt;/color&amp;gt;&lt;br /&gt;
  &amp;lt;size&amp;gt;200&amp;lt;/size&amp;gt;&lt;br /&gt;
  &amp;lt;uploadedFileContents&amp;gt;HYC116_BH3_FREQ.LOG&amp;lt;/uploadedFileContents&amp;gt;&lt;br /&gt;
&amp;lt;/jmolApplet&amp;gt;&amp;lt;/jmol&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
===Vibrational spectrum===&lt;br /&gt;
&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot;&lt;br /&gt;
!wavenumber (cm&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;)&lt;br /&gt;
!Intensity (arbitrary units)&lt;br /&gt;
!symmetry&lt;br /&gt;
!IR active?&lt;br /&gt;
!type&lt;br /&gt;
|-&lt;br /&gt;
|1163&lt;br /&gt;
|93&lt;br /&gt;
|A&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;&#039; &#039;&lt;br /&gt;
|Yes&lt;br /&gt;
|Out of plane bend&lt;br /&gt;
|-&lt;br /&gt;
|1213&lt;br /&gt;
|14&lt;br /&gt;
|E&#039;&lt;br /&gt;
|Very slight&lt;br /&gt;
|Bend&lt;br /&gt;
|-&lt;br /&gt;
|1213&lt;br /&gt;
|14&lt;br /&gt;
|E&#039;&lt;br /&gt;
|Very slight&lt;br /&gt;
|Bend&lt;br /&gt;
|-&lt;br /&gt;
|2582&lt;br /&gt;
|0&lt;br /&gt;
|A&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;&#039;&lt;br /&gt;
|No&lt;br /&gt;
|Symmetric stretch&lt;br /&gt;
|-&lt;br /&gt;
|2716&lt;br /&gt;
|126&lt;br /&gt;
|E&#039;&lt;br /&gt;
|Yes&lt;br /&gt;
|Asymmetric stretch&lt;br /&gt;
|-&lt;br /&gt;
|2716&lt;br /&gt;
|126&lt;br /&gt;
|E&#039;&lt;br /&gt;
|Yes&lt;br /&gt;
|Asymmetric stretch&lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;IR spectrum&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
[[file:Hyc116_ir_bh3.png|400*600]]&lt;br /&gt;
&lt;br /&gt;
There are only three peaks on the IR spectrum of BH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;, despite that there are 6 vibrational modes for the molecule. As shown in the table above, the symmetric stretching mode with A1 symmetry at 2582 cm&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt; is not IR active; naturally, that vibrational mode doesn’t give a peak on the IR spectrum. As shown from the table, two pairs of vibrational modes, the bond angle deformation/bend at 1213 cm&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt; and the asymmetric bond stretch at 2716 cm&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;, are degenerate with the symmetry label E. This means that they have the same energy, and hence give the same wavenumber on the IR spectrum. Each pair of degenerate vibrational modes give rise to one peak. This leaves three peaks, as confirmed by the IR spectrum above.&lt;br /&gt;
&lt;br /&gt;
===Molecular orbitals of BH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;===&lt;br /&gt;
&lt;br /&gt;
[[file:hyc116_bh3_MO_diagram.png]]&lt;br /&gt;
&lt;br /&gt;
The above molecular orbital diagram was taken from Dr Patricia Hunt&#039;s &amp;lt;i&amp;gt;Lecture 4 Tutorial Problem Model Answers&amp;lt;/i&amp;gt;.&amp;lt;ref&amp;gt;P. Hunt, &amp;quot;Lecture 4 Tutorial Problem Model Answers&amp;quot;, 2 (2018)&amp;lt;/ref&amp;gt; Diagrams of the &amp;quot;real&amp;quot; MOs were obtained from Gaussian.&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
There is no significant difference between the LCAO MOs and the real ones. Features such as orbital phases are shown clearly on both the LCAO MOs and the real MOs, illustrating the bonding/anti-bonding characters of the molecular orbitals. This suggests that the the qualitative MO theory is highly accurate and useful when studying the molecular orbitals of molecules.&lt;br /&gt;
&lt;br /&gt;
==Associated energies: ammonium borane==&lt;br /&gt;
&lt;br /&gt;
===NH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;===&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;Calculation type&amp;lt;/b&amp;gt;: Optimisation&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;Calculation Method&amp;lt;/b&amp;gt;: B3LYP&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;Basis set&amp;lt;/b&amp;gt;: 6-31G(d,p) &lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Summary table&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
[[file:Hyc116_nh3_631g_summarytable.png]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Items table&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;pre&amp;gt;&lt;br /&gt;
Item               Value     Threshold  Converged?&lt;br /&gt;
 Maximum Force            0.000006     0.000450     YES&lt;br /&gt;
 RMS     Force            0.000004     0.000300     YES&lt;br /&gt;
 Maximum Displacement     0.000012     0.001800     YES&lt;br /&gt;
 RMS     Displacement     0.000008     0.001200     YES&lt;br /&gt;
&amp;lt;/pre&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Frequency log file&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
[[Media:HYC116_NH3_FREQ.LOG]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Frequencies&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;pre&amp;gt;&lt;br /&gt;
Low frequencies ---   -8.5646   -8.5588   -0.0047    0.0454    0.1784   26.4183&lt;br /&gt;
Low frequencies --- 1089.7603 1694.1865 1694.1865&lt;br /&gt;
&amp;lt;/pre&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;jmol of NH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;&#039;&#039;&#039;&lt;br /&gt;
&amp;lt;jmol&amp;gt;&amp;lt;jmolApplet&amp;gt;&lt;br /&gt;
  &amp;lt;title&amp;gt;optimised NH3&amp;lt;/title&amp;gt;&lt;br /&gt;
  &amp;lt;color&amp;gt;black&amp;lt;/color&amp;gt;&lt;br /&gt;
  &amp;lt;size&amp;gt;200&amp;lt;/size&amp;gt;&lt;br /&gt;
  &amp;lt;uploadedFileContents&amp;gt;HYC116_NH3_FREQ.LOG&amp;lt;/uploadedFileContents&amp;gt;&lt;br /&gt;
&amp;lt;/jmolApplet&amp;gt;&amp;lt;/jmol&amp;gt;&lt;br /&gt;
&lt;br /&gt;
===NH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;BH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;===&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;Calculation type&amp;lt;/b&amp;gt;: Optimisation&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;Calculation Method&amp;lt;/b&amp;gt;: B3LYP&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;Basis set&amp;lt;/b&amp;gt;: 6-31G(d,p) &lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Summary table&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
[[file:Hyc116_nh3bh3_631g_summarytable1.png]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Items table&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;pre&amp;gt;&lt;br /&gt;
Item               Value     Threshold  Converged?&lt;br /&gt;
 Maximum Force            0.000121     0.000450     YES&lt;br /&gt;
 RMS     Force            0.000057     0.000300     YES&lt;br /&gt;
 Maximum Displacement     0.000501     0.001800     YES&lt;br /&gt;
 RMS     Displacement     0.000293     0.001200     YES&lt;br /&gt;
&amp;lt;/pre&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Frequency log file&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
[[Media:HYC116_NH3BH3_FREQ1.LOG]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Frequencies&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;pre&amp;gt;&lt;br /&gt;
Low frequencies ---   -0.0574   -0.0501   -0.0074   21.6276   21.6377   40.3839&lt;br /&gt;
Low frequencies ---  265.9973  632.3725  640.1275&lt;br /&gt;
&amp;lt;/pre&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;jmol of NH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;BH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;&#039;&#039;&#039;&lt;br /&gt;
&amp;lt;jmol&amp;gt;&amp;lt;jmolApplet&amp;gt;&lt;br /&gt;
  &amp;lt;title&amp;gt;optimised NH3BH3&amp;lt;/title&amp;gt;&lt;br /&gt;
  &amp;lt;color&amp;gt;black&amp;lt;/color&amp;gt;&lt;br /&gt;
  &amp;lt;size&amp;gt;200&amp;lt;/size&amp;gt;&lt;br /&gt;
  &amp;lt;uploadedFileContents&amp;gt;HYC116_NH3BH3_FREQ.LOG&amp;lt;/uploadedFileContents&amp;gt;&lt;br /&gt;
&amp;lt;/jmolApplet&amp;gt;&amp;lt;/jmol&amp;gt;&lt;br /&gt;
&lt;br /&gt;
===Association energy===&lt;br /&gt;
&lt;br /&gt;
E(BH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;) (using the optimisation with the correct symmetry) = -26.61532363 a.u. = &amp;lt;b&amp;gt;-26.61532 a.u. (5 d.p.)&amp;lt;/b&amp;gt;&lt;br /&gt;
&lt;br /&gt;
E(NH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;) = -56.55776873 a.u. = &amp;lt;b&amp;gt;-56.55777 a.u. (5 d.p.)&amp;lt;/b&amp;gt;&lt;br /&gt;
&lt;br /&gt;
E(NH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;BH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;) = -83.22468892 a.u. = &amp;lt;b&amp;gt;-83.22469 a.u. (5 d.p.)&amp;lt;/b&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
Carrying out calculations using numbers which has already been rounded up can possibly result in errors in the last digit. Hence, here the calculations were carried out using the numbers provided from the optimisations (i.e. with more decimal places than necessary); the answer was then rounded up to the desired accuracy. &lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
ΔE = E(NH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;BH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;)-[E(NH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;)+E(BH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;)]&lt;br /&gt;
&lt;br /&gt;
ΔE = -83.22468892 - (-56.55776873 + -26.61532363) = -0.05159656 a.u. &lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;ΔE = -0.05160 a.u. (5 d.p.)&amp;lt;/b&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Converting energy from a.u. to kJ/mol&#039;&#039;&#039;&lt;br /&gt;
An atomic unit for energy is Hartree, which is equal to 2625.5 kJ/mol.&lt;br /&gt;
&amp;lt;ref&amp;gt;https://cccbdb.nist.gov/hartree.asp (Accessed: 22.05.2018)&amp;lt;/ref&amp;gt;&lt;br /&gt;
 &lt;br /&gt;
&lt;br /&gt;
So ΔE in kJ/mol = -0.05159657 * 2625.5 = -135.46676828 kJ/mol&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;ΔE = -135 kJ/mol (nearest integer)&amp;lt;/b&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
The energy difference calculated above comes from the formation of the B-N dative bond. It is a relatively weak bond. According to a bond energy data sheet provided by the University of California,&amp;lt;ref&amp;gt;https://labs.chem.ucsb.edu/zakarian/armen/11---bonddissociationenergy.pdf (Accessed: 24.05.2018)&amp;lt;/ref&amp;gt;  the bond energy of the C-C bond of an ethane molecule is 368 kJ/mol. This is a fair comparison to the NH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;BH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt; molecule as the two molecules have the same structure, only with the carbon atoms on ethane swapped for Boron and Nitrogen in NH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;BH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;&lt;br /&gt;
&lt;br /&gt;
==Using a mixture of basis-sets and pseudo-potentials==&lt;br /&gt;
&lt;br /&gt;
===BBr&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;===&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;Calculation type&amp;lt;/b&amp;gt;: Optimisation&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;Calculation Method&amp;lt;/b&amp;gt;: B3LYP&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;Basis set&amp;lt;/b&amp;gt;: Boron: 6-31G(d,p) ; Br: LANL2DZ&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
Larger calculations are often sent to a web-server to run on a high-performance computer instead of a desktop. In order to experience and learn to use a web-server, the optimisation and the frequency analysis for BBr&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt; were both sent and done on a server instead of the desktop. The calculation results were downloaded from the web-server once they were finished.   &lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Summary table&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
[[file:Hyc116_bbr3_opt_summarytable.png]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Items table&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;pre&amp;gt;&lt;br /&gt;
Item               Value     Threshold  Converged?&lt;br /&gt;
 Maximum Force            0.000008     0.000450     YES&lt;br /&gt;
 RMS     Force            0.000005     0.000300     YES&lt;br /&gt;
 Maximum Displacement     0.000036     0.001800     YES&lt;br /&gt;
 RMS     Displacement     0.000023     0.001200     YES&lt;br /&gt;
&amp;lt;/pre&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Frequency log file&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
[[Media:Hyc116_bbr3_freq.log]]&lt;br /&gt;
&lt;br /&gt;
Attached above is the frequency file saved onto the computer from the SCAN server portal. The frequency file was also published on the chemistry database DSpace. {{DOI|10042/202442}}&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Frequencies&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;pre&amp;gt;&lt;br /&gt;
Low frequencies ---   -0.0137   -0.0064   -0.0046    2.4315    2.4315    4.8421&lt;br /&gt;
Low frequencies ---  155.9631  155.9651  267.7052&lt;br /&gt;
&amp;lt;/pre&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;jmol of BBr&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;&#039;&#039;&#039;&lt;br /&gt;
&amp;lt;jmol&amp;gt;&amp;lt;jmolApplet&amp;gt;&lt;br /&gt;
  &amp;lt;title&amp;gt;optimised BBr3&amp;lt;/title&amp;gt;&lt;br /&gt;
  &amp;lt;color&amp;gt;black&amp;lt;/color&amp;gt;&lt;br /&gt;
  &amp;lt;size&amp;gt;200&amp;lt;/size&amp;gt;&lt;br /&gt;
  &amp;lt;uploadedFileContents&amp;gt;Hyc116_bbr3_freq.log&amp;lt;/uploadedFileContents&amp;gt;&lt;br /&gt;
&amp;lt;/jmolApplet&amp;gt;&amp;lt;/jmol&amp;gt;&lt;br /&gt;
&lt;br /&gt;
==Mini project: Aromaticity==&lt;br /&gt;
&lt;br /&gt;
===Benzene===&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;Calculation type&amp;lt;/b&amp;gt;: Optimisation&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;Calculation Method&amp;lt;/b&amp;gt;: B3LYP&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;Basis set&amp;lt;/b&amp;gt;: 6-31G(d,p) &lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Summary table&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
[[file:Hyc116_c6h6_summarytable.png]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Items table&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;pre&amp;gt;&lt;br /&gt;
Item               Value     Threshold  Converged?&lt;br /&gt;
 Maximum Force            0.000193     0.000450     YES&lt;br /&gt;
 RMS     Force            0.000079     0.000300     YES&lt;br /&gt;
 Maximum Displacement     0.000830     0.001800     YES&lt;br /&gt;
 RMS     Displacement     0.000294     0.001200     YES&lt;br /&gt;
&amp;lt;/pre&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Frequency log file&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
[[Media:HYC116_C6H6_FREQ.LOG]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Frequencies&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;pre&amp;gt;&lt;br /&gt;
Low frequencies ---   -3.5606   -3.5606   -0.0089   -0.0043   -0.0043   10.0905&lt;br /&gt;
Low frequencies ---  413.9582  413.9582  621.1416&lt;br /&gt;
&amp;lt;/pre&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;jmol of C&amp;lt;sub&amp;gt;6&amp;lt;/sub&amp;gt;H&amp;lt;sub&amp;gt;6&amp;lt;/sub&amp;gt;&#039;&#039;&#039;&lt;br /&gt;
&amp;lt;jmol&amp;gt;&amp;lt;jmolApplet&amp;gt;&lt;br /&gt;
  &amp;lt;title&amp;gt;optimised Benzene&amp;lt;/title&amp;gt;&lt;br /&gt;
  &amp;lt;color&amp;gt;black&amp;lt;/color&amp;gt;&lt;br /&gt;
  &amp;lt;size&amp;gt;200&amp;lt;/size&amp;gt;&lt;br /&gt;
  &amp;lt;uploadedFileContents&amp;gt;HYC116_C6H6_FREQ.LOG&amp;lt;/uploadedFileContents&amp;gt;&lt;br /&gt;
&amp;lt;/jmolApplet&amp;gt;&amp;lt;/jmol&amp;gt;&lt;br /&gt;
&lt;br /&gt;
===Borazine===&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;Calculation type&amp;lt;/b&amp;gt;: Optimisation&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;Calculation Method&amp;lt;/b&amp;gt;: B3LYP&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;Basis set&amp;lt;/b&amp;gt;: 6-31G(d,p) &lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Summary table&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
[[file:Hyc116_borazine_summarytable.png]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Items table&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;pre&amp;gt;&lt;br /&gt;
Item               Value     Threshold  Converged?&lt;br /&gt;
 Maximum Force            0.000085     0.000450     YES&lt;br /&gt;
 RMS     Force            0.000033     0.000300     YES&lt;br /&gt;
 Maximum Displacement     0.000250     0.001800     YES&lt;br /&gt;
 RMS     Displacement     0.000074     0.001200     YES&lt;br /&gt;
&amp;lt;/pre&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Frequency log file&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
[[Media:HYC116_BORAZINE_FREQ.LOG]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Frequencies&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;pre&amp;gt;&lt;br /&gt;
Low frequencies ---  -12.6626  -12.6626   -8.9272   -0.0211   -0.0104   -0.0104&lt;br /&gt;
Low frequencies ---  289.1112  289.1112  403.8613&lt;br /&gt;
&amp;lt;/pre&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;jmol of Borazine&#039;&#039;&#039;&lt;br /&gt;
&amp;lt;jmol&amp;gt;&amp;lt;jmolApplet&amp;gt;&lt;br /&gt;
  &amp;lt;title&amp;gt;optimised Borazine&amp;lt;/title&amp;gt;&lt;br /&gt;
  &amp;lt;color&amp;gt;black&amp;lt;/color&amp;gt;&lt;br /&gt;
  &amp;lt;size&amp;gt;200&amp;lt;/size&amp;gt;&lt;br /&gt;
  &amp;lt;uploadedFileContents&amp;gt;HYC116_BORAZINE_FREQ.LOG&amp;lt;/uploadedFileContents&amp;gt;&lt;br /&gt;
&amp;lt;/jmolApplet&amp;gt;&amp;lt;/jmol&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
===Charge distribution===&lt;br /&gt;
&lt;br /&gt;
An NBO charge analysis was carried out on both the optimised benzene and borazine. Visualisations of the charge distribution are shown in the table below, with the colour range going from -1.102 to 1.102 for both molecule. This large scale was chosen as it allows direct comparison of the charge on any atoms in these two molecules and shows the relative magnitude of charges on all these atoms. Negative charges are shown in red, and positive charges are shown in green. A neutral charge is displayed in black, so the smaller a charge is (positive or negative), the darker its colour representation is. Larger charges are shown in brighter colours. The charges are also displayed on the atoms as numbers with a neutral charge being zero. Negative charges are shown as negative number and positive charges are shown as positive numbers. &lt;br /&gt;
&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot;&lt;br /&gt;
!&lt;br /&gt;
!Benzene&lt;br /&gt;
!Borazine&lt;br /&gt;
|-&lt;br /&gt;
!Visualisation of charge distribution&lt;br /&gt;
|[[File:Hyc116_benzene_charge_distribution1.png|500x500px|thumb|centre|Charge distribution of Benzene visualisation]]&lt;br /&gt;
|[[File:Hyc116_borazine_charge_distribution1.png|500x500px|thumb|centre|Charge distribution of Borazine visualisation]]&lt;br /&gt;
|-&lt;br /&gt;
!Charge &lt;br /&gt;
|Carbon: -0.239&lt;br /&gt;
&lt;br /&gt;
Hydrogen: 0.239&lt;br /&gt;
|Nitrogen: -1.102 &lt;br /&gt;
&lt;br /&gt;
Boron: 0.747&lt;br /&gt;
&lt;br /&gt;
Hydrogen (bonded to N): 0.432&lt;br /&gt;
&lt;br /&gt;
Hydrogen (bonded to B): -0.077&lt;br /&gt;
|-&lt;br /&gt;
!Discussion&lt;br /&gt;
|From the visualisation, it is shown that there is a slightly negative charge on the carbon atoms, and a positive charge of the same magnitude on the hydrogen atoms. All the carbon atoms have the same charge as they are in identical environments. The same applies to all the hydrogen atoms. This is due to the highly symmetrical structure of benzene. Since the same colour scale was used for both benzene and borazine, and the charges are much smaller in magnitude on atoms in benzene than atoms on borazine, the colours on the charge distribution visualisation is much darker. &lt;br /&gt;
|Polar bonds between nitrogen and boron are demonstration from the above visualisation. From the colours displayed on the charge distribution visualisation as well as the charge values, it is shown that nitrogen has a relatively large negative charge, while boron has a positive charge. This is due to the difference in electrogenativity between these atoms: nitrogen atoms are more electronegative than boron and tends to attract electrons towards themselves. It is worth noting that the hydrogen atoms do not all have the same charge. The hydrogen atoms bonded to boron have a slightly negative charge, and the ones bonded to nitrogen have a small positive charge. &lt;br /&gt;
&lt;br /&gt;
The fact that the same colour scale was used for both molecules comes in helpful here. It allows the charges on atoms to be compared directly. For example, just from looking at the colours, one can tell that or example, even though both carbon and nitrogen are electronegative, nitrogen is much more electronegative, which is quantitatively shown by Pauling&#039;s electronegativity scale.&amp;lt;ref&amp;gt;http://www.tutor-homework.com/Chemistry_Help/electronegativity_table/electronegativity.html (Accessed: 24.0502018&amp;lt;/ref&amp;gt;&lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
===Comparative MOs of Benzene and Borazine===&lt;br /&gt;
&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot;&lt;br /&gt;
!&lt;br /&gt;
!Benzene&lt;br /&gt;
!Borazine&lt;br /&gt;
!Comparison and Discussion&lt;br /&gt;
|-&lt;br /&gt;
!1st comparative pair&lt;br /&gt;
|[[File:Hyc116_benzene_1st_MO_pair_7.png|200x200px|centre]]&lt;br /&gt;
|[[File:Hyc116_borazine_1st_MO_pair_level9.png|200x200px|centre]]&lt;br /&gt;
|MO 9 of both benzene and borazine are comparable. They both show delocalised molecular orbital with an overall bonding character. There is a nodal plane across the molecular orbitals for both benzene and borazine. For benzene, there is contribution from all the carbon and hydrogen s orbitals. Moreover, the molecular orbitals are symmetric to their counterpart of opposite phase, giving an E&amp;lt;sub&amp;gt;1g&amp;lt;/sub&amp;gt; MO. That is not the case for borazine; they are less symmetric in borazine. This MO of borazine has an E&#039; symmetry. Nitrogen atoms are more electronegative than boron atoms and pull electron density towards themselves, resulting in a larger lobe. There is contribution from all the boron and nitrogen s orbitals, and three of the hydrogen s orbitals, though not all of them. &lt;br /&gt;
|-&lt;br /&gt;
!2nd comparative pair&lt;br /&gt;
|[[File:Hyc116_benzene_2nd_MO_pair_10.png|200x200px|centre]]&lt;br /&gt;
|[[File:Hyc116_borazine_2nd_MO_pair_level11.png|200x200px|centre]]&lt;br /&gt;
|MO 10 of benzene and MO 11 of borazine are comparable. Here shows a pair of rather delocalised molecular orbitals with slightly more antibonding character than the first pair shown above. On both MOs, there is no contribution from one pair of opposite hydrogen atoms, but contribution from s orbitals of all other atoms on both molecule. The benzene MO has an E&amp;lt;sub&amp;gt;2g&amp;lt;/sub&amp;gt; symmetry. In borazine, the lobes are in different sizes due to the higher electronegativity of nitrogen. The lobes at the nitrogen atoms are larger as they attract electrons towards themselves more so than boron atoms do. This borazine MO has an E&#039; symmetry. &lt;br /&gt;
|-&lt;br /&gt;
!3rd comparative pair&lt;br /&gt;
|[[File:Hyc116_benzene_3rd_MO_pair_21.png|200x200px|centre]]&lt;br /&gt;
|[[File:Hyc116_borazine_3rd_MO_pair_level21.png|200x200px|centre]]&lt;br /&gt;
|The HOMO (MO 21) of benzene and the HOMO (MO 21) of borazine are comparable. They are both made of p orbitals of all carbon atoms (or all boron and nitrogen atoms in the case of borazine); there is no contribution from hydrogen atoms as they do not have p orbitals. There is a nodal plan perpendicular to the z axis (highest rotational axis) and one parallel to the z axis. On benzene, the MO is very symmetric and has an E&amp;lt;sub&amp;gt;1g&amp;lt;/sub&amp;gt; symmetry; the lobes of the MO are the same in size. On borazine, the lobe where there are two nitrogen atoms is bigger in size, again due to the higher electronegtivity of nitrogen compared to boron. The borazine MO has an E&#039; &#039; symmetry.&lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
===Aromaticity: discussion===&lt;br /&gt;
&lt;br /&gt;
Aromatic compounds display properties such as their high stability and bond lengths between typical single and double bonds. A simple understanding of aromaticity involves the overlap of p orbitals perpendicular to the cyclic plane; the delocalisation of electrons on the pi system is identified to be responsible of the stability of aromatic systems. Aromatic compounds can be identified by the Huckel’s rule, which states that conjugated planar cyclic molecules with (4n +2) π electrons are aromatic. Both benzene and borazine obey the Huckel’s rule and fit the conventional description of aromaticity. &amp;lt;ref&amp;gt;Clayden, J., Greeves, N. &amp;amp; Warren, S. G. Organic chemistry. (Oxford University Press, 2012)&amp;lt;/ref&amp;gt;&lt;br /&gt;
&lt;br /&gt;
However, it is proved in recent years that the conventional criteria do not necessarily have to be obeyed for a compound to be aromatic. For instance, there has been shown that some non-planar compounds display aromaticity. This suggests that the criteria for aromaticity is not simply structural, and these advances give rise to concepts such as quasiaromaticity and pseudoaromaticity. Recent advances show that there are quantum mechanics basis on the idea of aromaticity.&amp;lt;ref&amp;gt;Palusiak, M. &amp;amp; Krygowski, T. M. Application of AIM Parameters at Ring Critical Points for Estimation of π-Electron Delocalization in Six-Membered Aromatic and Quasi-Aromatic Rings. Chemistry - A European Journal 13, 7996–8006 (2007).&amp;lt;/ref&amp;gt; &lt;br /&gt;
&lt;br /&gt;
In conclusion, while the overlap of pi orbitals provides a simple understanding for aromaticity, it is not a sufficient description for aromaticity.&lt;br /&gt;
&lt;br /&gt;
==References==&lt;/div&gt;</summary>
		<author><name>Hyc116</name></author>
	</entry>
	<entry>
		<id>https://chemwiki.ch.ic.ac.uk/index.php?title=MO_hyc116&amp;diff=732368</id>
		<title>MO hyc116</title>
		<link rel="alternate" type="text/html" href="https://chemwiki.ch.ic.ac.uk/index.php?title=MO_hyc116&amp;diff=732368"/>
		<updated>2018-05-25T15:05:39Z</updated>

		<summary type="html">&lt;p&gt;Hyc116: /* Aromaticity: some theories */&lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;==BH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;==&lt;br /&gt;
&lt;br /&gt;
===standard information===&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;Calculation type&amp;lt;/b&amp;gt;: Optimisation&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;Calculation Method&amp;lt;/b&amp;gt;: B3LYP&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;Basis set&amp;lt;/b&amp;gt;: 6-31G(d,p) &lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Summary table&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
[[file:Hyc116_bh3_631g_opt_summarytable.png]]&lt;br /&gt;
&lt;br /&gt;
The above summary table was obtained after the 2nd optimisation of BH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt; (after the initial optimisation using the 3-21G basis set). Notice how the symmetry is incorrect and shown as Cs. This is because the symmetry was manually broken at the beginning by changing the bond length of B-H bonds. The point group was manually adjusted and the molecule was optimised again before the frequency analysis and the new summary table is attached below.&lt;br /&gt;
&lt;br /&gt;
[[file:Hyc116_bh3_correctsummarytable.png]]&lt;br /&gt;
&lt;br /&gt;
The above summary table was obtained from the optimisation after adjusting the symmetry. The point shown in this summary table is D&amp;lt;sub&amp;gt;3h&amp;lt;/sub&amp;gt;, which is the correct for BH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;. &lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Items table&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
Below is the items table taken from the optimisation with the correct point group.&lt;br /&gt;
&lt;br /&gt;
&amp;lt;pre&amp;gt;&lt;br /&gt;
Item               Value     Threshold  Converged?&lt;br /&gt;
 Maximum Force            0.000015     0.000450     YES&lt;br /&gt;
 RMS     Force            0.000010     0.000300     YES&lt;br /&gt;
 Maximum Displacement     0.000058     0.001800     YES&lt;br /&gt;
 RMS     Displacement     0.000038     0.001200     YES&lt;br /&gt;
&amp;lt;/pre&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Frequency log file&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
[[Media:HYC116 BH3 FREQ.LOG]] &lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Frequencies&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;pre&amp;gt;&lt;br /&gt;
Low frequencies ---  -10.3498   -3.4492   -1.2454   -0.0055    0.4779    3.2165&lt;br /&gt;
Low frequencies --- 1162.9519 1213.1527 1213.1554&lt;br /&gt;
&amp;lt;/pre&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;jmol of BH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;&#039;&#039;&#039;&lt;br /&gt;
&amp;lt;jmol&amp;gt;&amp;lt;jmolApplet&amp;gt;&lt;br /&gt;
  &amp;lt;title&amp;gt;optimised BH3&amp;lt;/title&amp;gt;&lt;br /&gt;
  &amp;lt;color&amp;gt;black&amp;lt;/color&amp;gt;&lt;br /&gt;
  &amp;lt;size&amp;gt;200&amp;lt;/size&amp;gt;&lt;br /&gt;
  &amp;lt;uploadedFileContents&amp;gt;HYC116_BH3_FREQ.LOG&amp;lt;/uploadedFileContents&amp;gt;&lt;br /&gt;
&amp;lt;/jmolApplet&amp;gt;&amp;lt;/jmol&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
===Vibrational spectrum===&lt;br /&gt;
&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot;&lt;br /&gt;
!wavenumber (cm&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;)&lt;br /&gt;
!Intensity (arbitrary units)&lt;br /&gt;
!symmetry&lt;br /&gt;
!IR active?&lt;br /&gt;
!type&lt;br /&gt;
|-&lt;br /&gt;
|1163&lt;br /&gt;
|93&lt;br /&gt;
|A&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;&#039; &#039;&lt;br /&gt;
|Yes&lt;br /&gt;
|Out of plane bend&lt;br /&gt;
|-&lt;br /&gt;
|1213&lt;br /&gt;
|14&lt;br /&gt;
|E&#039;&lt;br /&gt;
|Very slight&lt;br /&gt;
|Bend&lt;br /&gt;
|-&lt;br /&gt;
|1213&lt;br /&gt;
|14&lt;br /&gt;
|E&#039;&lt;br /&gt;
|Very slight&lt;br /&gt;
|Bend&lt;br /&gt;
|-&lt;br /&gt;
|2582&lt;br /&gt;
|0&lt;br /&gt;
|A&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;&#039;&lt;br /&gt;
|No&lt;br /&gt;
|Symmetric stretch&lt;br /&gt;
|-&lt;br /&gt;
|2716&lt;br /&gt;
|126&lt;br /&gt;
|E&#039;&lt;br /&gt;
|Yes&lt;br /&gt;
|Asymmetric stretch&lt;br /&gt;
|-&lt;br /&gt;
|2716&lt;br /&gt;
|126&lt;br /&gt;
|E&#039;&lt;br /&gt;
|Yes&lt;br /&gt;
|Asymmetric stretch&lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;IR spectrum&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
[[file:Hyc116_ir_bh3.png|400*600]]&lt;br /&gt;
&lt;br /&gt;
There are only three peaks on the IR spectrum of BH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;, despite that there are 6 vibrational modes for the molecule. As shown in the table above, the symmetric stretching mode with A1 symmetry at 2582 cm&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt; is not IR active; naturally, that vibrational mode doesn’t give a peak on the IR spectrum. As shown from the table, two pairs of vibrational modes, the bond angle deformation/bend at 1213 cm&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt; and the asymmetric bond stretch at 2716 cm&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;, are degenerate with the symmetry label E. This means that they have the same energy, and hence give the same wavenumber on the IR spectrum. Each pair of degenerate vibrational modes give rise to one peak. This leaves three peaks, as confirmed by the IR spectrum above.&lt;br /&gt;
&lt;br /&gt;
===Molecular orbitals of BH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;===&lt;br /&gt;
&lt;br /&gt;
[[file:hyc116_bh3_MO_diagram.png]]&lt;br /&gt;
&lt;br /&gt;
The above molecular orbital diagram was taken from Dr Patricia Hunt&#039;s &amp;lt;i&amp;gt;Lecture 4 Tutorial Problem Model Answers&amp;lt;/i&amp;gt;.&amp;lt;ref&amp;gt;P. Hunt, &amp;quot;Lecture 4 Tutorial Problem Model Answers&amp;quot;, 2 (2018)&amp;lt;/ref&amp;gt; Diagrams of the &amp;quot;real&amp;quot; MOs were obtained from Gaussian.&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
There is no significant difference between the LCAO MOs and the real ones. Features such as orbital phases are shown clearly on both the LCAO MOs and the real MOs, illustrating the bonding/anti-bonding characters of the molecular orbitals. This suggests that the the qualitative MO theory is highly accurate and useful when studying the molecular orbitals of molecules.&lt;br /&gt;
&lt;br /&gt;
==Associated energies: ammonium borane==&lt;br /&gt;
&lt;br /&gt;
===NH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;===&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;Calculation type&amp;lt;/b&amp;gt;: Optimisation&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;Calculation Method&amp;lt;/b&amp;gt;: B3LYP&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;Basis set&amp;lt;/b&amp;gt;: 6-31G(d,p) &lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Summary table&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
[[file:Hyc116_nh3_631g_summarytable.png]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Items table&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;pre&amp;gt;&lt;br /&gt;
Item               Value     Threshold  Converged?&lt;br /&gt;
 Maximum Force            0.000006     0.000450     YES&lt;br /&gt;
 RMS     Force            0.000004     0.000300     YES&lt;br /&gt;
 Maximum Displacement     0.000012     0.001800     YES&lt;br /&gt;
 RMS     Displacement     0.000008     0.001200     YES&lt;br /&gt;
&amp;lt;/pre&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Frequency log file&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
[[Media:HYC116_NH3_FREQ.LOG]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Frequencies&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;pre&amp;gt;&lt;br /&gt;
Low frequencies ---   -8.5646   -8.5588   -0.0047    0.0454    0.1784   26.4183&lt;br /&gt;
Low frequencies --- 1089.7603 1694.1865 1694.1865&lt;br /&gt;
&amp;lt;/pre&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;jmol of NH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;&#039;&#039;&#039;&lt;br /&gt;
&amp;lt;jmol&amp;gt;&amp;lt;jmolApplet&amp;gt;&lt;br /&gt;
  &amp;lt;title&amp;gt;optimised NH3&amp;lt;/title&amp;gt;&lt;br /&gt;
  &amp;lt;color&amp;gt;black&amp;lt;/color&amp;gt;&lt;br /&gt;
  &amp;lt;size&amp;gt;200&amp;lt;/size&amp;gt;&lt;br /&gt;
  &amp;lt;uploadedFileContents&amp;gt;HYC116_NH3_FREQ.LOG&amp;lt;/uploadedFileContents&amp;gt;&lt;br /&gt;
&amp;lt;/jmolApplet&amp;gt;&amp;lt;/jmol&amp;gt;&lt;br /&gt;
&lt;br /&gt;
===NH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;BH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;===&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;Calculation type&amp;lt;/b&amp;gt;: Optimisation&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;Calculation Method&amp;lt;/b&amp;gt;: B3LYP&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;Basis set&amp;lt;/b&amp;gt;: 6-31G(d,p) &lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Summary table&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
[[file:Hyc116_nh3bh3_631g_summarytable1.png]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Items table&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;pre&amp;gt;&lt;br /&gt;
Item               Value     Threshold  Converged?&lt;br /&gt;
 Maximum Force            0.000121     0.000450     YES&lt;br /&gt;
 RMS     Force            0.000057     0.000300     YES&lt;br /&gt;
 Maximum Displacement     0.000501     0.001800     YES&lt;br /&gt;
 RMS     Displacement     0.000293     0.001200     YES&lt;br /&gt;
&amp;lt;/pre&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Frequency log file&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
[[Media:HYC116_NH3BH3_FREQ1.LOG]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Frequencies&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;pre&amp;gt;&lt;br /&gt;
Low frequencies ---   -0.0574   -0.0501   -0.0074   21.6276   21.6377   40.3839&lt;br /&gt;
Low frequencies ---  265.9973  632.3725  640.1275&lt;br /&gt;
&amp;lt;/pre&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;jmol of NH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;BH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;&#039;&#039;&#039;&lt;br /&gt;
&amp;lt;jmol&amp;gt;&amp;lt;jmolApplet&amp;gt;&lt;br /&gt;
  &amp;lt;title&amp;gt;optimised NH3BH3&amp;lt;/title&amp;gt;&lt;br /&gt;
  &amp;lt;color&amp;gt;black&amp;lt;/color&amp;gt;&lt;br /&gt;
  &amp;lt;size&amp;gt;200&amp;lt;/size&amp;gt;&lt;br /&gt;
  &amp;lt;uploadedFileContents&amp;gt;HYC116_NH3BH3_FREQ.LOG&amp;lt;/uploadedFileContents&amp;gt;&lt;br /&gt;
&amp;lt;/jmolApplet&amp;gt;&amp;lt;/jmol&amp;gt;&lt;br /&gt;
&lt;br /&gt;
===Association energy===&lt;br /&gt;
&lt;br /&gt;
E(BH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;) (using the optimisation with the correct symmetry) = -26.61532363 a.u. = &amp;lt;b&amp;gt;-26.61532 a.u. (5 d.p.)&amp;lt;/b&amp;gt;&lt;br /&gt;
&lt;br /&gt;
E(NH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;) = -56.55776873 a.u. = &amp;lt;b&amp;gt;-56.55777 a.u. (5 d.p.)&amp;lt;/b&amp;gt;&lt;br /&gt;
&lt;br /&gt;
E(NH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;BH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;) = -83.22468892 a.u. = &amp;lt;b&amp;gt;-83.22469 a.u. (5 d.p.)&amp;lt;/b&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
Carrying out calculations using numbers which has already been rounded up can possibly result in errors in the last digit. Hence, here the calculations were carried out using the numbers provided from the optimisations (i.e. with more decimal places than necessary); the answer was then rounded up to the desired accuracy. &lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
ΔE = E(NH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;BH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;)-[E(NH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;)+E(BH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;)]&lt;br /&gt;
&lt;br /&gt;
ΔE = -83.22468892 - (-56.55776873 + -26.61532363) = -0.05159656 a.u. &lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;ΔE = -0.05160 a.u. (5 d.p.)&amp;lt;/b&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Converting energy from a.u. to kJ/mol&#039;&#039;&#039;&lt;br /&gt;
An atomic unit for energy is Hartree, which is equal to 2625.5 kJ/mol.&lt;br /&gt;
&amp;lt;ref&amp;gt;https://cccbdb.nist.gov/hartree.asp (Accessed: 22.05.2018)&amp;lt;/ref&amp;gt;&lt;br /&gt;
 &lt;br /&gt;
&lt;br /&gt;
So ΔE in kJ/mol = -0.05159657 * 2625.5 = -135.46676828 kJ/mol&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;ΔE = -135 kJ/mol (nearest integer)&amp;lt;/b&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
The energy difference calculated above comes from the formation of the B-N dative bond. It is a relatively weak bond. According to a bond energy data sheet provided by the University of California,&amp;lt;ref&amp;gt;https://labs.chem.ucsb.edu/zakarian/armen/11---bonddissociationenergy.pdf (Accessed: 24.05.2018)&amp;lt;/ref&amp;gt;  the bond energy of the C-C bond of an ethane molecule is 368 kJ/mol. This is a fair comparison to the NH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;BH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt; molecule as the two molecules have the same structure, only with the carbon atoms on ethane swapped for Boron and Nitrogen in NH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;BH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;&lt;br /&gt;
&lt;br /&gt;
==Using a mixture of basis-sets and pseudo-potentials==&lt;br /&gt;
&lt;br /&gt;
===BBr&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;===&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;Calculation type&amp;lt;/b&amp;gt;: Optimisation&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;Calculation Method&amp;lt;/b&amp;gt;: B3LYP&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;Basis set&amp;lt;/b&amp;gt;: Boron: 6-31G(d,p) ; Br: LANL2DZ&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
Larger calculations are often sent to a web-server to run on a high-performance computer instead of a desktop. In order to experience and learn to use a web-server, the optimisation and the frequency analysis for BBr&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt; were both sent and done on a server instead of the desktop. The calculation results were downloaded from the web-server once they were finished.   &lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Summary table&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
[[file:Hyc116_bbr3_opt_summarytable.png]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Items table&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;pre&amp;gt;&lt;br /&gt;
Item               Value     Threshold  Converged?&lt;br /&gt;
 Maximum Force            0.000008     0.000450     YES&lt;br /&gt;
 RMS     Force            0.000005     0.000300     YES&lt;br /&gt;
 Maximum Displacement     0.000036     0.001800     YES&lt;br /&gt;
 RMS     Displacement     0.000023     0.001200     YES&lt;br /&gt;
&amp;lt;/pre&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Frequency log file&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
[[Media:Hyc116_bbr3_freq.log]]&lt;br /&gt;
&lt;br /&gt;
Attached above is the frequency file saved onto the computer from the SCAN server portal. The frequency file was also published on the chemistry database DSpace. {{DOI|10042/202442}}&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Frequencies&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;pre&amp;gt;&lt;br /&gt;
Low frequencies ---   -0.0137   -0.0064   -0.0046    2.4315    2.4315    4.8421&lt;br /&gt;
Low frequencies ---  155.9631  155.9651  267.7052&lt;br /&gt;
&amp;lt;/pre&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;jmol of BBr&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;&#039;&#039;&#039;&lt;br /&gt;
&amp;lt;jmol&amp;gt;&amp;lt;jmolApplet&amp;gt;&lt;br /&gt;
  &amp;lt;title&amp;gt;optimised BBr3&amp;lt;/title&amp;gt;&lt;br /&gt;
  &amp;lt;color&amp;gt;black&amp;lt;/color&amp;gt;&lt;br /&gt;
  &amp;lt;size&amp;gt;200&amp;lt;/size&amp;gt;&lt;br /&gt;
  &amp;lt;uploadedFileContents&amp;gt;Hyc116_bbr3_freq.log&amp;lt;/uploadedFileContents&amp;gt;&lt;br /&gt;
&amp;lt;/jmolApplet&amp;gt;&amp;lt;/jmol&amp;gt;&lt;br /&gt;
&lt;br /&gt;
==Mini project: Aromaticity==&lt;br /&gt;
&lt;br /&gt;
===Benzene===&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;Calculation type&amp;lt;/b&amp;gt;: Optimisation&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;Calculation Method&amp;lt;/b&amp;gt;: B3LYP&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;Basis set&amp;lt;/b&amp;gt;: 6-31G(d,p) &lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Summary table&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
[[file:Hyc116_c6h6_summarytable.png]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Items table&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;pre&amp;gt;&lt;br /&gt;
Item               Value     Threshold  Converged?&lt;br /&gt;
 Maximum Force            0.000193     0.000450     YES&lt;br /&gt;
 RMS     Force            0.000079     0.000300     YES&lt;br /&gt;
 Maximum Displacement     0.000830     0.001800     YES&lt;br /&gt;
 RMS     Displacement     0.000294     0.001200     YES&lt;br /&gt;
&amp;lt;/pre&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Frequency log file&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
[[Media:HYC116_C6H6_FREQ.LOG]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Frequencies&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;pre&amp;gt;&lt;br /&gt;
Low frequencies ---   -3.5606   -3.5606   -0.0089   -0.0043   -0.0043   10.0905&lt;br /&gt;
Low frequencies ---  413.9582  413.9582  621.1416&lt;br /&gt;
&amp;lt;/pre&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;jmol of C&amp;lt;sub&amp;gt;6&amp;lt;/sub&amp;gt;H&amp;lt;sub&amp;gt;6&amp;lt;/sub&amp;gt;&#039;&#039;&#039;&lt;br /&gt;
&amp;lt;jmol&amp;gt;&amp;lt;jmolApplet&amp;gt;&lt;br /&gt;
  &amp;lt;title&amp;gt;optimised Benzene&amp;lt;/title&amp;gt;&lt;br /&gt;
  &amp;lt;color&amp;gt;black&amp;lt;/color&amp;gt;&lt;br /&gt;
  &amp;lt;size&amp;gt;200&amp;lt;/size&amp;gt;&lt;br /&gt;
  &amp;lt;uploadedFileContents&amp;gt;HYC116_C6H6_FREQ.LOG&amp;lt;/uploadedFileContents&amp;gt;&lt;br /&gt;
&amp;lt;/jmolApplet&amp;gt;&amp;lt;/jmol&amp;gt;&lt;br /&gt;
&lt;br /&gt;
===Borazine===&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;Calculation type&amp;lt;/b&amp;gt;: Optimisation&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;Calculation Method&amp;lt;/b&amp;gt;: B3LYP&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;Basis set&amp;lt;/b&amp;gt;: 6-31G(d,p) &lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Summary table&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
[[file:Hyc116_borazine_summarytable.png]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Items table&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;pre&amp;gt;&lt;br /&gt;
Item               Value     Threshold  Converged?&lt;br /&gt;
 Maximum Force            0.000085     0.000450     YES&lt;br /&gt;
 RMS     Force            0.000033     0.000300     YES&lt;br /&gt;
 Maximum Displacement     0.000250     0.001800     YES&lt;br /&gt;
 RMS     Displacement     0.000074     0.001200     YES&lt;br /&gt;
&amp;lt;/pre&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Frequency log file&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
[[Media:HYC116_BORAZINE_FREQ.LOG]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Frequencies&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;pre&amp;gt;&lt;br /&gt;
Low frequencies ---  -12.6626  -12.6626   -8.9272   -0.0211   -0.0104   -0.0104&lt;br /&gt;
Low frequencies ---  289.1112  289.1112  403.8613&lt;br /&gt;
&amp;lt;/pre&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;jmol of Borazine&#039;&#039;&#039;&lt;br /&gt;
&amp;lt;jmol&amp;gt;&amp;lt;jmolApplet&amp;gt;&lt;br /&gt;
  &amp;lt;title&amp;gt;optimised Borazine&amp;lt;/title&amp;gt;&lt;br /&gt;
  &amp;lt;color&amp;gt;black&amp;lt;/color&amp;gt;&lt;br /&gt;
  &amp;lt;size&amp;gt;200&amp;lt;/size&amp;gt;&lt;br /&gt;
  &amp;lt;uploadedFileContents&amp;gt;HYC116_BORAZINE_FREQ.LOG&amp;lt;/uploadedFileContents&amp;gt;&lt;br /&gt;
&amp;lt;/jmolApplet&amp;gt;&amp;lt;/jmol&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
===Charge distribution===&lt;br /&gt;
&lt;br /&gt;
An NBO charge analysis was carried out on both the optimised benzene and borazine. Visualisations of the charge distribution are shown in the table below, with the colour range going from -1.102 to 1.102 for both molecule. This large scale was chosen as it allows direct comparison of the charge on any atoms in these two molecules and shows the relative magnitude of charges on all these atoms. Negative charges are shown in red, and positive charges are shown in green. A neutral charge is displayed in black, so the smaller a charge is (positive or negative), the darker its colour representation is. Larger charges are shown in brighter colours. The charges are also displayed on the atoms as numbers with a neutral charge being zero. Negative charges are shown as negative number and positive charges are shown as positive numbers. &lt;br /&gt;
&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot;&lt;br /&gt;
!&lt;br /&gt;
!Benzene&lt;br /&gt;
!Borazine&lt;br /&gt;
|-&lt;br /&gt;
!Visualisation of charge distribution&lt;br /&gt;
|[[File:Hyc116_benzene_charge_distribution1.png|500x500px|thumb|centre|Charge distribution of Benzene visualisation]]&lt;br /&gt;
|[[File:Hyc116_borazine_charge_distribution1.png|500x500px|thumb|centre|Charge distribution of Borazine visualisation]]&lt;br /&gt;
|-&lt;br /&gt;
!Charge &lt;br /&gt;
|Carbon: -0.239&lt;br /&gt;
&lt;br /&gt;
Hydrogen: 0.239&lt;br /&gt;
|Nitrogen: -1.102 &lt;br /&gt;
&lt;br /&gt;
Boron: 0.747&lt;br /&gt;
&lt;br /&gt;
Hydrogen (bonded to N): 0.432&lt;br /&gt;
&lt;br /&gt;
Hydrogen (bonded to B): -0.077&lt;br /&gt;
|-&lt;br /&gt;
!Discussion&lt;br /&gt;
|From the visualisation, it is shown that there is a slightly negative charge on the carbon atoms, and a positive charge of the same magnitude on the hydrogen atoms. All the carbon atoms have the same charge as they are in identical environments. The same applies to all the hydrogen atoms. This is due to the highly symmetrical structure of benzene. Since the same colour scale was used for both benzene and borazine, and the charges are much smaller in magnitude on atoms in benzene than atoms on borazine, the colours on the charge distribution visualisation is much darker. &lt;br /&gt;
|Polar bonds between nitrogen and boron are demonstration from the above visualisation. From the colours displayed on the charge distribution visualisation as well as the charge values, it is shown that nitrogen has a relatively large negative charge, while boron has a positive charge. This is due to the difference in electrogenativity between these atoms: nitrogen atoms are more electronegative than boron and tends to attract electrons towards themselves. It is worth noting that the hydrogen atoms do not all have the same charge. The hydrogen atoms bonded to boron have a slightly negative charge, and the ones bonded to nitrogen have a small positive charge. &lt;br /&gt;
&lt;br /&gt;
The fact that the same colour scale was used for both molecules comes in helpful here. It allows the charges on atoms to be compared directly. For example, just from looking at the colours, one can tell that or example, even though both carbon and nitrogen are electronegative, nitrogen is much more electronegative, which is quantitatively shown by Pauling&#039;s electronegativity scale.&amp;lt;ref&amp;gt;http://www.tutor-homework.com/Chemistry_Help/electronegativity_table/electronegativity.html (Accessed: 24.0502018&amp;lt;/ref&amp;gt;&lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
===Comparative MOs of Benzene and Borazine===&lt;br /&gt;
&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot;&lt;br /&gt;
!&lt;br /&gt;
!Benzene&lt;br /&gt;
!Borazine&lt;br /&gt;
!Comparison and Discussion&lt;br /&gt;
|-&lt;br /&gt;
!1st comparative pair&lt;br /&gt;
|[[File:Hyc116_benzene_1st_MO_pair_7.png|200x200px|centre]]&lt;br /&gt;
|[[File:Hyc116_borazine_1st_MO_pair_level9.png|200x200px|centre]]&lt;br /&gt;
|MO 9 of both benzene and borazine are comparable. They both show delocalised molecular orbital with an overall bonding character. There is a nodal plane across the molecular orbitals for both benzene and borazine. For benzene, there is contribution from all the carbon and hydrogen s orbitals. Moreover, the molecular orbitals are symmetric to their counterpart of opposite phase, giving an E&amp;lt;sub&amp;gt;1g&amp;lt;/sub&amp;gt; MO. That is not the case for borazine; they are less symmetric in borazine. This MO of borazine has an E&#039; symmetry. Nitrogen atoms are more electronegative than boron atoms and pull electron density towards themselves, resulting in a larger lobe. There is contribution from all the boron and nitrogen s orbitals, and three of the hydrogen s orbitals, though not all of them. &lt;br /&gt;
|-&lt;br /&gt;
!2nd comparative pair&lt;br /&gt;
|[[File:Hyc116_benzene_2nd_MO_pair_10.png|200x200px|centre]]&lt;br /&gt;
|[[File:Hyc116_borazine_2nd_MO_pair_level11.png|200x200px|centre]]&lt;br /&gt;
|MO 10 of benzene and MO 11 of borazine are comparable. Here shows a pair of rather delocalised molecular orbitals with slightly more antibonding character than the first pair shown above. On both MOs, there is no contribution from one pair of opposite hydrogen atoms, but contribution from s orbitals of all other atoms on both molecule. The benzene MO has an E&amp;lt;sub&amp;gt;2g&amp;lt;/sub&amp;gt; symmetry. In borazine, the lobes are in different sizes due to the higher electronegativity of nitrogen. The lobes at the nitrogen atoms are larger as they attract electrons towards themselves more so than boron atoms do. This borazine MO has an E&#039; symmetry. &lt;br /&gt;
|-&lt;br /&gt;
!3rd comparative pair&lt;br /&gt;
|[[File:Hyc116_benzene_3rd_MO_pair_21.png|200x200px|centre]]&lt;br /&gt;
|[[File:Hyc116_borazine_3rd_MO_pair_level21.png|200x200px|centre]]&lt;br /&gt;
|The HOMO (MO 21) of benzene and the HOMO (MO 21) of borazine are comparable. They are both made of p orbitals of all carbon atoms (or all boron and nitrogen atoms in the case of borazine); there is no contribution from hydrogen atoms as they do not have p orbitals. There is a nodal plan perpendicular to the z axis (highest rotational axis) and one parallel to the z axis. On benzene, the MO is very symmetric and has an E&amp;lt;sub&amp;gt;1g&amp;lt;/sub&amp;gt; symmetry; the lobes of the MO are the same in size. On borazine, the lobe where there are two nitrogen atoms is bigger in size, again due to the higher electronegtivity of nitrogen compared to boron. The borazine MO has an E&#039; &#039; symmetry.&lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
===Aromaticity: discussion===&lt;br /&gt;
&lt;br /&gt;
Aromatic compounds display properties such as their high stability and bond lengths between typical single and double bonds. A simple understanding of aromaticity involves the overlap of p orbitals perpendicular to the cyclic plane; the delocalisation of electrons on the pi system is identified to be responsible of the stability of aromatic systems. Aromatic compounds can be identified by the Huckel’s rule, which states that conjugated planar cyclic molecules with (4n +2) π electrons are aromatic. Both benzene and borazine obey the Huckel’s rule and fit the conventional description of aromaticity. &amp;lt;ref&amp;gt;Clayden, J., Greeves, N. &amp;amp; Warren, S. G. Organic chemistry. (Oxford University Press, 2012)&amp;lt;/ref&amp;gt;&lt;br /&gt;
&lt;br /&gt;
However, it is proved in recent years that the conventional criteria do not necessarily have to be obeyed for a compound to be aromatic. For instance, there has been shown that some non-planar compounds display aromaticity. This suggests that the criteria for aromaticity is not simply structural, and these advances give rise to concepts such as quasiaromaticity and pseudoaromaticity. Recent advances show that there are quantum mechanics basis on the idea of aromaticity.&amp;lt;ref&amp;gt;Palusiak, M. &amp;amp; Krygowski, T. M. Application of AIM Parameters at Ring Critical Points for Estimation of π-Electron Delocalization in Six-Membered Aromatic and Quasi-Aromatic Rings. Chemistry - A European Journal 13, 7996–8006 (2007).&amp;lt;/ref&amp;gt; &lt;br /&gt;
&lt;br /&gt;
In conclusion, while the overlap of pi orbitals provides a simple understanding for aromaticity, it is not a sufficient description for aromaticity.&lt;br /&gt;
&lt;br /&gt;
==References==&lt;br /&gt;
{{reflist}}&lt;/div&gt;</summary>
		<author><name>Hyc116</name></author>
	</entry>
	<entry>
		<id>https://chemwiki.ch.ic.ac.uk/index.php?title=MO_hyc116&amp;diff=732357</id>
		<title>MO hyc116</title>
		<link rel="alternate" type="text/html" href="https://chemwiki.ch.ic.ac.uk/index.php?title=MO_hyc116&amp;diff=732357"/>
		<updated>2018-05-25T15:02:54Z</updated>

		<summary type="html">&lt;p&gt;Hyc116: /* Aromaticity: some theories */&lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;==BH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;==&lt;br /&gt;
&lt;br /&gt;
===standard information===&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;Calculation type&amp;lt;/b&amp;gt;: Optimisation&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;Calculation Method&amp;lt;/b&amp;gt;: B3LYP&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;Basis set&amp;lt;/b&amp;gt;: 6-31G(d,p) &lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Summary table&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
[[file:Hyc116_bh3_631g_opt_summarytable.png]]&lt;br /&gt;
&lt;br /&gt;
The above summary table was obtained after the 2nd optimisation of BH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt; (after the initial optimisation using the 3-21G basis set). Notice how the symmetry is incorrect and shown as Cs. This is because the symmetry was manually broken at the beginning by changing the bond length of B-H bonds. The point group was manually adjusted and the molecule was optimised again before the frequency analysis and the new summary table is attached below.&lt;br /&gt;
&lt;br /&gt;
[[file:Hyc116_bh3_correctsummarytable.png]]&lt;br /&gt;
&lt;br /&gt;
The above summary table was obtained from the optimisation after adjusting the symmetry. The point shown in this summary table is D&amp;lt;sub&amp;gt;3h&amp;lt;/sub&amp;gt;, which is the correct for BH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;. &lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Items table&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
Below is the items table taken from the optimisation with the correct point group.&lt;br /&gt;
&lt;br /&gt;
&amp;lt;pre&amp;gt;&lt;br /&gt;
Item               Value     Threshold  Converged?&lt;br /&gt;
 Maximum Force            0.000015     0.000450     YES&lt;br /&gt;
 RMS     Force            0.000010     0.000300     YES&lt;br /&gt;
 Maximum Displacement     0.000058     0.001800     YES&lt;br /&gt;
 RMS     Displacement     0.000038     0.001200     YES&lt;br /&gt;
&amp;lt;/pre&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Frequency log file&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
[[Media:HYC116 BH3 FREQ.LOG]] &lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Frequencies&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;pre&amp;gt;&lt;br /&gt;
Low frequencies ---  -10.3498   -3.4492   -1.2454   -0.0055    0.4779    3.2165&lt;br /&gt;
Low frequencies --- 1162.9519 1213.1527 1213.1554&lt;br /&gt;
&amp;lt;/pre&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;jmol of BH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;&#039;&#039;&#039;&lt;br /&gt;
&amp;lt;jmol&amp;gt;&amp;lt;jmolApplet&amp;gt;&lt;br /&gt;
  &amp;lt;title&amp;gt;optimised BH3&amp;lt;/title&amp;gt;&lt;br /&gt;
  &amp;lt;color&amp;gt;black&amp;lt;/color&amp;gt;&lt;br /&gt;
  &amp;lt;size&amp;gt;200&amp;lt;/size&amp;gt;&lt;br /&gt;
  &amp;lt;uploadedFileContents&amp;gt;HYC116_BH3_FREQ.LOG&amp;lt;/uploadedFileContents&amp;gt;&lt;br /&gt;
&amp;lt;/jmolApplet&amp;gt;&amp;lt;/jmol&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
===Vibrational spectrum===&lt;br /&gt;
&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot;&lt;br /&gt;
!wavenumber (cm&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;)&lt;br /&gt;
!Intensity (arbitrary units)&lt;br /&gt;
!symmetry&lt;br /&gt;
!IR active?&lt;br /&gt;
!type&lt;br /&gt;
|-&lt;br /&gt;
|1163&lt;br /&gt;
|93&lt;br /&gt;
|A&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;&#039; &#039;&lt;br /&gt;
|Yes&lt;br /&gt;
|Out of plane bend&lt;br /&gt;
|-&lt;br /&gt;
|1213&lt;br /&gt;
|14&lt;br /&gt;
|E&#039;&lt;br /&gt;
|Very slight&lt;br /&gt;
|Bend&lt;br /&gt;
|-&lt;br /&gt;
|1213&lt;br /&gt;
|14&lt;br /&gt;
|E&#039;&lt;br /&gt;
|Very slight&lt;br /&gt;
|Bend&lt;br /&gt;
|-&lt;br /&gt;
|2582&lt;br /&gt;
|0&lt;br /&gt;
|A&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;&#039;&lt;br /&gt;
|No&lt;br /&gt;
|Symmetric stretch&lt;br /&gt;
|-&lt;br /&gt;
|2716&lt;br /&gt;
|126&lt;br /&gt;
|E&#039;&lt;br /&gt;
|Yes&lt;br /&gt;
|Asymmetric stretch&lt;br /&gt;
|-&lt;br /&gt;
|2716&lt;br /&gt;
|126&lt;br /&gt;
|E&#039;&lt;br /&gt;
|Yes&lt;br /&gt;
|Asymmetric stretch&lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;IR spectrum&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
[[file:Hyc116_ir_bh3.png|400*600]]&lt;br /&gt;
&lt;br /&gt;
There are only three peaks on the IR spectrum of BH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;, despite that there are 6 vibrational modes for the molecule. As shown in the table above, the symmetric stretching mode with A1 symmetry at 2582 cm&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt; is not IR active; naturally, that vibrational mode doesn’t give a peak on the IR spectrum. As shown from the table, two pairs of vibrational modes, the bond angle deformation/bend at 1213 cm&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt; and the asymmetric bond stretch at 2716 cm&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;, are degenerate with the symmetry label E. This means that they have the same energy, and hence give the same wavenumber on the IR spectrum. Each pair of degenerate vibrational modes give rise to one peak. This leaves three peaks, as confirmed by the IR spectrum above.&lt;br /&gt;
&lt;br /&gt;
===Molecular orbitals of BH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;===&lt;br /&gt;
&lt;br /&gt;
[[file:hyc116_bh3_MO_diagram.png]]&lt;br /&gt;
&lt;br /&gt;
The above molecular orbital diagram was taken from Dr Patricia Hunt&#039;s &amp;lt;i&amp;gt;Lecture 4 Tutorial Problem Model Answers&amp;lt;/i&amp;gt;.&amp;lt;ref&amp;gt;P. Hunt, &amp;quot;Lecture 4 Tutorial Problem Model Answers&amp;quot;, 2 (2018)&amp;lt;/ref&amp;gt; Diagrams of the &amp;quot;real&amp;quot; MOs were obtained from Gaussian.&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
There is no significant difference between the LCAO MOs and the real ones. Features such as orbital phases are shown clearly on both the LCAO MOs and the real MOs, illustrating the bonding/anti-bonding characters of the molecular orbitals. This suggests that the the qualitative MO theory is highly accurate and useful when studying the molecular orbitals of molecules.&lt;br /&gt;
&lt;br /&gt;
==Associated energies: ammonium borane==&lt;br /&gt;
&lt;br /&gt;
===NH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;===&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;Calculation type&amp;lt;/b&amp;gt;: Optimisation&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;Calculation Method&amp;lt;/b&amp;gt;: B3LYP&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;Basis set&amp;lt;/b&amp;gt;: 6-31G(d,p) &lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Summary table&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
[[file:Hyc116_nh3_631g_summarytable.png]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Items table&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;pre&amp;gt;&lt;br /&gt;
Item               Value     Threshold  Converged?&lt;br /&gt;
 Maximum Force            0.000006     0.000450     YES&lt;br /&gt;
 RMS     Force            0.000004     0.000300     YES&lt;br /&gt;
 Maximum Displacement     0.000012     0.001800     YES&lt;br /&gt;
 RMS     Displacement     0.000008     0.001200     YES&lt;br /&gt;
&amp;lt;/pre&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Frequency log file&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
[[Media:HYC116_NH3_FREQ.LOG]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Frequencies&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;pre&amp;gt;&lt;br /&gt;
Low frequencies ---   -8.5646   -8.5588   -0.0047    0.0454    0.1784   26.4183&lt;br /&gt;
Low frequencies --- 1089.7603 1694.1865 1694.1865&lt;br /&gt;
&amp;lt;/pre&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;jmol of NH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;&#039;&#039;&#039;&lt;br /&gt;
&amp;lt;jmol&amp;gt;&amp;lt;jmolApplet&amp;gt;&lt;br /&gt;
  &amp;lt;title&amp;gt;optimised NH3&amp;lt;/title&amp;gt;&lt;br /&gt;
  &amp;lt;color&amp;gt;black&amp;lt;/color&amp;gt;&lt;br /&gt;
  &amp;lt;size&amp;gt;200&amp;lt;/size&amp;gt;&lt;br /&gt;
  &amp;lt;uploadedFileContents&amp;gt;HYC116_NH3_FREQ.LOG&amp;lt;/uploadedFileContents&amp;gt;&lt;br /&gt;
&amp;lt;/jmolApplet&amp;gt;&amp;lt;/jmol&amp;gt;&lt;br /&gt;
&lt;br /&gt;
===NH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;BH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;===&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;Calculation type&amp;lt;/b&amp;gt;: Optimisation&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;Calculation Method&amp;lt;/b&amp;gt;: B3LYP&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;Basis set&amp;lt;/b&amp;gt;: 6-31G(d,p) &lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Summary table&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
[[file:Hyc116_nh3bh3_631g_summarytable1.png]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Items table&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;pre&amp;gt;&lt;br /&gt;
Item               Value     Threshold  Converged?&lt;br /&gt;
 Maximum Force            0.000121     0.000450     YES&lt;br /&gt;
 RMS     Force            0.000057     0.000300     YES&lt;br /&gt;
 Maximum Displacement     0.000501     0.001800     YES&lt;br /&gt;
 RMS     Displacement     0.000293     0.001200     YES&lt;br /&gt;
&amp;lt;/pre&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Frequency log file&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
[[Media:HYC116_NH3BH3_FREQ1.LOG]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Frequencies&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;pre&amp;gt;&lt;br /&gt;
Low frequencies ---   -0.0574   -0.0501   -0.0074   21.6276   21.6377   40.3839&lt;br /&gt;
Low frequencies ---  265.9973  632.3725  640.1275&lt;br /&gt;
&amp;lt;/pre&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;jmol of NH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;BH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;&#039;&#039;&#039;&lt;br /&gt;
&amp;lt;jmol&amp;gt;&amp;lt;jmolApplet&amp;gt;&lt;br /&gt;
  &amp;lt;title&amp;gt;optimised NH3BH3&amp;lt;/title&amp;gt;&lt;br /&gt;
  &amp;lt;color&amp;gt;black&amp;lt;/color&amp;gt;&lt;br /&gt;
  &amp;lt;size&amp;gt;200&amp;lt;/size&amp;gt;&lt;br /&gt;
  &amp;lt;uploadedFileContents&amp;gt;HYC116_NH3BH3_FREQ.LOG&amp;lt;/uploadedFileContents&amp;gt;&lt;br /&gt;
&amp;lt;/jmolApplet&amp;gt;&amp;lt;/jmol&amp;gt;&lt;br /&gt;
&lt;br /&gt;
===Association energy===&lt;br /&gt;
&lt;br /&gt;
E(BH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;) (using the optimisation with the correct symmetry) = -26.61532363 a.u. = &amp;lt;b&amp;gt;-26.61532 a.u. (5 d.p.)&amp;lt;/b&amp;gt;&lt;br /&gt;
&lt;br /&gt;
E(NH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;) = -56.55776873 a.u. = &amp;lt;b&amp;gt;-56.55777 a.u. (5 d.p.)&amp;lt;/b&amp;gt;&lt;br /&gt;
&lt;br /&gt;
E(NH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;BH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;) = -83.22468892 a.u. = &amp;lt;b&amp;gt;-83.22469 a.u. (5 d.p.)&amp;lt;/b&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
Carrying out calculations using numbers which has already been rounded up can possibly result in errors in the last digit. Hence, here the calculations were carried out using the numbers provided from the optimisations (i.e. with more decimal places than necessary); the answer was then rounded up to the desired accuracy. &lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
ΔE = E(NH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;BH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;)-[E(NH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;)+E(BH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;)]&lt;br /&gt;
&lt;br /&gt;
ΔE = -83.22468892 - (-56.55776873 + -26.61532363) = -0.05159656 a.u. &lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;ΔE = -0.05160 a.u. (5 d.p.)&amp;lt;/b&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Converting energy from a.u. to kJ/mol&#039;&#039;&#039;&lt;br /&gt;
An atomic unit for energy is Hartree, which is equal to 2625.5 kJ/mol.&lt;br /&gt;
&amp;lt;ref&amp;gt;https://cccbdb.nist.gov/hartree.asp (Accessed: 22.05.2018)&amp;lt;/ref&amp;gt;&lt;br /&gt;
 &lt;br /&gt;
&lt;br /&gt;
So ΔE in kJ/mol = -0.05159657 * 2625.5 = -135.46676828 kJ/mol&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;ΔE = -135 kJ/mol (nearest integer)&amp;lt;/b&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
The energy difference calculated above comes from the formation of the B-N dative bond. It is a relatively weak bond. According to a bond energy data sheet provided by the University of California,&amp;lt;ref&amp;gt;https://labs.chem.ucsb.edu/zakarian/armen/11---bonddissociationenergy.pdf (Accessed: 24.05.2018)&amp;lt;/ref&amp;gt;  the bond energy of the C-C bond of an ethane molecule is 368 kJ/mol. This is a fair comparison to the NH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;BH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt; molecule as the two molecules have the same structure, only with the carbon atoms on ethane swapped for Boron and Nitrogen in NH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;BH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;&lt;br /&gt;
&lt;br /&gt;
==Using a mixture of basis-sets and pseudo-potentials==&lt;br /&gt;
&lt;br /&gt;
===BBr&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;===&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;Calculation type&amp;lt;/b&amp;gt;: Optimisation&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;Calculation Method&amp;lt;/b&amp;gt;: B3LYP&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;Basis set&amp;lt;/b&amp;gt;: Boron: 6-31G(d,p) ; Br: LANL2DZ&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
Larger calculations are often sent to a web-server to run on a high-performance computer instead of a desktop. In order to experience and learn to use a web-server, the optimisation and the frequency analysis for BBr&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt; were both sent and done on a server instead of the desktop. The calculation results were downloaded from the web-server once they were finished.   &lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Summary table&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
[[file:Hyc116_bbr3_opt_summarytable.png]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Items table&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;pre&amp;gt;&lt;br /&gt;
Item               Value     Threshold  Converged?&lt;br /&gt;
 Maximum Force            0.000008     0.000450     YES&lt;br /&gt;
 RMS     Force            0.000005     0.000300     YES&lt;br /&gt;
 Maximum Displacement     0.000036     0.001800     YES&lt;br /&gt;
 RMS     Displacement     0.000023     0.001200     YES&lt;br /&gt;
&amp;lt;/pre&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Frequency log file&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
[[Media:Hyc116_bbr3_freq.log]]&lt;br /&gt;
&lt;br /&gt;
Attached above is the frequency file saved onto the computer from the SCAN server portal. The frequency file was also published on the chemistry database DSpace. {{DOI|10042/202442}}&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Frequencies&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;pre&amp;gt;&lt;br /&gt;
Low frequencies ---   -0.0137   -0.0064   -0.0046    2.4315    2.4315    4.8421&lt;br /&gt;
Low frequencies ---  155.9631  155.9651  267.7052&lt;br /&gt;
&amp;lt;/pre&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;jmol of BBr&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;&#039;&#039;&#039;&lt;br /&gt;
&amp;lt;jmol&amp;gt;&amp;lt;jmolApplet&amp;gt;&lt;br /&gt;
  &amp;lt;title&amp;gt;optimised BBr3&amp;lt;/title&amp;gt;&lt;br /&gt;
  &amp;lt;color&amp;gt;black&amp;lt;/color&amp;gt;&lt;br /&gt;
  &amp;lt;size&amp;gt;200&amp;lt;/size&amp;gt;&lt;br /&gt;
  &amp;lt;uploadedFileContents&amp;gt;Hyc116_bbr3_freq.log&amp;lt;/uploadedFileContents&amp;gt;&lt;br /&gt;
&amp;lt;/jmolApplet&amp;gt;&amp;lt;/jmol&amp;gt;&lt;br /&gt;
&lt;br /&gt;
==Mini project: Aromaticity==&lt;br /&gt;
&lt;br /&gt;
===Benzene===&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;Calculation type&amp;lt;/b&amp;gt;: Optimisation&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;Calculation Method&amp;lt;/b&amp;gt;: B3LYP&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;Basis set&amp;lt;/b&amp;gt;: 6-31G(d,p) &lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Summary table&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
[[file:Hyc116_c6h6_summarytable.png]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Items table&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;pre&amp;gt;&lt;br /&gt;
Item               Value     Threshold  Converged?&lt;br /&gt;
 Maximum Force            0.000193     0.000450     YES&lt;br /&gt;
 RMS     Force            0.000079     0.000300     YES&lt;br /&gt;
 Maximum Displacement     0.000830     0.001800     YES&lt;br /&gt;
 RMS     Displacement     0.000294     0.001200     YES&lt;br /&gt;
&amp;lt;/pre&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Frequency log file&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
[[Media:HYC116_C6H6_FREQ.LOG]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Frequencies&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;pre&amp;gt;&lt;br /&gt;
Low frequencies ---   -3.5606   -3.5606   -0.0089   -0.0043   -0.0043   10.0905&lt;br /&gt;
Low frequencies ---  413.9582  413.9582  621.1416&lt;br /&gt;
&amp;lt;/pre&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;jmol of C&amp;lt;sub&amp;gt;6&amp;lt;/sub&amp;gt;H&amp;lt;sub&amp;gt;6&amp;lt;/sub&amp;gt;&#039;&#039;&#039;&lt;br /&gt;
&amp;lt;jmol&amp;gt;&amp;lt;jmolApplet&amp;gt;&lt;br /&gt;
  &amp;lt;title&amp;gt;optimised Benzene&amp;lt;/title&amp;gt;&lt;br /&gt;
  &amp;lt;color&amp;gt;black&amp;lt;/color&amp;gt;&lt;br /&gt;
  &amp;lt;size&amp;gt;200&amp;lt;/size&amp;gt;&lt;br /&gt;
  &amp;lt;uploadedFileContents&amp;gt;HYC116_C6H6_FREQ.LOG&amp;lt;/uploadedFileContents&amp;gt;&lt;br /&gt;
&amp;lt;/jmolApplet&amp;gt;&amp;lt;/jmol&amp;gt;&lt;br /&gt;
&lt;br /&gt;
===Borazine===&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;Calculation type&amp;lt;/b&amp;gt;: Optimisation&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;Calculation Method&amp;lt;/b&amp;gt;: B3LYP&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;Basis set&amp;lt;/b&amp;gt;: 6-31G(d,p) &lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Summary table&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
[[file:Hyc116_borazine_summarytable.png]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Items table&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;pre&amp;gt;&lt;br /&gt;
Item               Value     Threshold  Converged?&lt;br /&gt;
 Maximum Force            0.000085     0.000450     YES&lt;br /&gt;
 RMS     Force            0.000033     0.000300     YES&lt;br /&gt;
 Maximum Displacement     0.000250     0.001800     YES&lt;br /&gt;
 RMS     Displacement     0.000074     0.001200     YES&lt;br /&gt;
&amp;lt;/pre&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Frequency log file&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
[[Media:HYC116_BORAZINE_FREQ.LOG]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Frequencies&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;pre&amp;gt;&lt;br /&gt;
Low frequencies ---  -12.6626  -12.6626   -8.9272   -0.0211   -0.0104   -0.0104&lt;br /&gt;
Low frequencies ---  289.1112  289.1112  403.8613&lt;br /&gt;
&amp;lt;/pre&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;jmol of Borazine&#039;&#039;&#039;&lt;br /&gt;
&amp;lt;jmol&amp;gt;&amp;lt;jmolApplet&amp;gt;&lt;br /&gt;
  &amp;lt;title&amp;gt;optimised Borazine&amp;lt;/title&amp;gt;&lt;br /&gt;
  &amp;lt;color&amp;gt;black&amp;lt;/color&amp;gt;&lt;br /&gt;
  &amp;lt;size&amp;gt;200&amp;lt;/size&amp;gt;&lt;br /&gt;
  &amp;lt;uploadedFileContents&amp;gt;HYC116_BORAZINE_FREQ.LOG&amp;lt;/uploadedFileContents&amp;gt;&lt;br /&gt;
&amp;lt;/jmolApplet&amp;gt;&amp;lt;/jmol&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
===Charge distribution===&lt;br /&gt;
&lt;br /&gt;
An NBO charge analysis was carried out on both the optimised benzene and borazine. Visualisations of the charge distribution are shown in the table below, with the colour range going from -1.102 to 1.102 for both molecule. This large scale was chosen as it allows direct comparison of the charge on any atoms in these two molecules and shows the relative magnitude of charges on all these atoms. Negative charges are shown in red, and positive charges are shown in green. A neutral charge is displayed in black, so the smaller a charge is (positive or negative), the darker its colour representation is. Larger charges are shown in brighter colours. The charges are also displayed on the atoms as numbers with a neutral charge being zero. Negative charges are shown as negative number and positive charges are shown as positive numbers. &lt;br /&gt;
&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot;&lt;br /&gt;
!&lt;br /&gt;
!Benzene&lt;br /&gt;
!Borazine&lt;br /&gt;
|-&lt;br /&gt;
!Visualisation of charge distribution&lt;br /&gt;
|[[File:Hyc116_benzene_charge_distribution1.png|500x500px|thumb|centre|Charge distribution of Benzene visualisation]]&lt;br /&gt;
|[[File:Hyc116_borazine_charge_distribution1.png|500x500px|thumb|centre|Charge distribution of Borazine visualisation]]&lt;br /&gt;
|-&lt;br /&gt;
!Charge &lt;br /&gt;
|Carbon: -0.239&lt;br /&gt;
&lt;br /&gt;
Hydrogen: 0.239&lt;br /&gt;
|Nitrogen: -1.102 &lt;br /&gt;
&lt;br /&gt;
Boron: 0.747&lt;br /&gt;
&lt;br /&gt;
Hydrogen (bonded to N): 0.432&lt;br /&gt;
&lt;br /&gt;
Hydrogen (bonded to B): -0.077&lt;br /&gt;
|-&lt;br /&gt;
!Discussion&lt;br /&gt;
|From the visualisation, it is shown that there is a slightly negative charge on the carbon atoms, and a positive charge of the same magnitude on the hydrogen atoms. All the carbon atoms have the same charge as they are in identical environments. The same applies to all the hydrogen atoms. This is due to the highly symmetrical structure of benzene. Since the same colour scale was used for both benzene and borazine, and the charges are much smaller in magnitude on atoms in benzene than atoms on borazine, the colours on the charge distribution visualisation is much darker. &lt;br /&gt;
|Polar bonds between nitrogen and boron are demonstration from the above visualisation. From the colours displayed on the charge distribution visualisation as well as the charge values, it is shown that nitrogen has a relatively large negative charge, while boron has a positive charge. This is due to the difference in electrogenativity between these atoms: nitrogen atoms are more electronegative than boron and tends to attract electrons towards themselves. It is worth noting that the hydrogen atoms do not all have the same charge. The hydrogen atoms bonded to boron have a slightly negative charge, and the ones bonded to nitrogen have a small positive charge. &lt;br /&gt;
&lt;br /&gt;
The fact that the same colour scale was used for both molecules comes in helpful here. It allows the charges on atoms to be compared directly. For example, just from looking at the colours, one can tell that or example, even though both carbon and nitrogen are electronegative, nitrogen is much more electronegative, which is quantitatively shown by Pauling&#039;s electronegativity scale.&amp;lt;ref&amp;gt;http://www.tutor-homework.com/Chemistry_Help/electronegativity_table/electronegativity.html (Accessed: 24.0502018&amp;lt;/ref&amp;gt;&lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
===Comparative MOs of Benzene and Borazine===&lt;br /&gt;
&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot;&lt;br /&gt;
!&lt;br /&gt;
!Benzene&lt;br /&gt;
!Borazine&lt;br /&gt;
!Comparison and Discussion&lt;br /&gt;
|-&lt;br /&gt;
!1st comparative pair&lt;br /&gt;
|[[File:Hyc116_benzene_1st_MO_pair_7.png|200x200px|centre]]&lt;br /&gt;
|[[File:Hyc116_borazine_1st_MO_pair_level9.png|200x200px|centre]]&lt;br /&gt;
|MO 9 of both benzene and borazine are comparable. They both show delocalised molecular orbital with an overall bonding character. There is a nodal plane across the molecular orbitals for both benzene and borazine. For benzene, there is contribution from all the carbon and hydrogen s orbitals. Moreover, the molecular orbitals are symmetric to their counterpart of opposite phase, giving an E&amp;lt;sub&amp;gt;1g&amp;lt;/sub&amp;gt; MO. That is not the case for borazine; they are less symmetric in borazine. This MO of borazine has an E&#039; symmetry. Nitrogen atoms are more electronegative than boron atoms and pull electron density towards themselves, resulting in a larger lobe. There is contribution from all the boron and nitrogen s orbitals, and three of the hydrogen s orbitals, though not all of them. &lt;br /&gt;
|-&lt;br /&gt;
!2nd comparative pair&lt;br /&gt;
|[[File:Hyc116_benzene_2nd_MO_pair_10.png|200x200px|centre]]&lt;br /&gt;
|[[File:Hyc116_borazine_2nd_MO_pair_level11.png|200x200px|centre]]&lt;br /&gt;
|MO 10 of benzene and MO 11 of borazine are comparable. Here shows a pair of rather delocalised molecular orbitals with slightly more antibonding character than the first pair shown above. On both MOs, there is no contribution from one pair of opposite hydrogen atoms, but contribution from s orbitals of all other atoms on both molecule. The benzene MO has an E&amp;lt;sub&amp;gt;2g&amp;lt;/sub&amp;gt; symmetry. In borazine, the lobes are in different sizes due to the higher electronegativity of nitrogen. The lobes at the nitrogen atoms are larger as they attract electrons towards themselves more so than boron atoms do. This borazine MO has an E&#039; symmetry. &lt;br /&gt;
|-&lt;br /&gt;
!3rd comparative pair&lt;br /&gt;
|[[File:Hyc116_benzene_3rd_MO_pair_21.png|200x200px|centre]]&lt;br /&gt;
|[[File:Hyc116_borazine_3rd_MO_pair_level21.png|200x200px|centre]]&lt;br /&gt;
|The HOMO (MO 21) of benzene and the HOMO (MO 21) of borazine are comparable. They are both made of p orbitals of all carbon atoms (or all boron and nitrogen atoms in the case of borazine); there is no contribution from hydrogen atoms as they do not have p orbitals. There is a nodal plan perpendicular to the z axis (highest rotational axis) and one parallel to the z axis. On benzene, the MO is very symmetric and has an E&amp;lt;sub&amp;gt;1g&amp;lt;/sub&amp;gt; symmetry; the lobes of the MO are the same in size. On borazine, the lobe where there are two nitrogen atoms is bigger in size, again due to the higher electronegtivity of nitrogen compared to boron. The borazine MO has an E&#039; &#039; symmetry.&lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
===Aromaticity: some theories===&lt;br /&gt;
&lt;br /&gt;
Aromatic compounds display properties such as their high stability and bond lengths between typical single and double bonds. A simple understanding of aromaticity involves the overlap of p orbitals perpendicular to the cyclic plane; the delocalisation of electrons on the pi system is identified to be responsible of the stability of aromatic systems. Aromatic compounds can be identified by the Huckel’s rule, which states that conjugated planar cyclic molecules with (4n +2) π electrons are aromatic. Both benzene and borazine obey the Huckel’s rule and fit the conventional description of aromaticity. &amp;lt;ref&amp;gt;Clayden, J., Greeves, N. &amp;amp; Warren, S. G. Organic chemistry. (Oxford University Press, 2012)&amp;lt;/ref&amp;gt;&lt;br /&gt;
&lt;br /&gt;
However, it is proved in recent years that the conventional criteria do not necessarily have to be obeyed for a compound to be aromatic. For instance, there has been shown that some non-planar compounds display aromaticity. This suggests that the criteria for aromaticity is not simply structural, and these advances give rise to concepts such as quasiaromaticity and pseudoaromaticity. Recent advances show that there are quantum mechanics basis on the idea of aromaticity.&amp;lt;ref&amp;gt;Palusiak, M. &amp;amp; Krygowski, T. M. Application of AIM Parameters at Ring Critical Points for Estimation of π-Electron Delocalization in Six-Membered Aromatic and Quasi-Aromatic Rings. Chemistry - A European Journal 13, 7996–8006 (2007).&amp;lt;/ref&amp;gt; &lt;br /&gt;
&lt;br /&gt;
In conclusion, while the overlap of pi orbitals provides a simple understanding for aromaticity, it is not a sufficient description for aromaticity.&lt;br /&gt;
&lt;br /&gt;
==References==&lt;br /&gt;
{{reflist}}&lt;/div&gt;</summary>
		<author><name>Hyc116</name></author>
	</entry>
	<entry>
		<id>https://chemwiki.ch.ic.ac.uk/index.php?title=MO_hyc116&amp;diff=732327</id>
		<title>MO hyc116</title>
		<link rel="alternate" type="text/html" href="https://chemwiki.ch.ic.ac.uk/index.php?title=MO_hyc116&amp;diff=732327"/>
		<updated>2018-05-25T14:57:43Z</updated>

		<summary type="html">&lt;p&gt;Hyc116: /* Aromaticity */&lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;==BH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;==&lt;br /&gt;
&lt;br /&gt;
===standard information===&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;Calculation type&amp;lt;/b&amp;gt;: Optimisation&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;Calculation Method&amp;lt;/b&amp;gt;: B3LYP&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;Basis set&amp;lt;/b&amp;gt;: 6-31G(d,p) &lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Summary table&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
[[file:Hyc116_bh3_631g_opt_summarytable.png]]&lt;br /&gt;
&lt;br /&gt;
The above summary table was obtained after the 2nd optimisation of BH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt; (after the initial optimisation using the 3-21G basis set). Notice how the symmetry is incorrect and shown as Cs. This is because the symmetry was manually broken at the beginning by changing the bond length of B-H bonds. The point group was manually adjusted and the molecule was optimised again before the frequency analysis and the new summary table is attached below.&lt;br /&gt;
&lt;br /&gt;
[[file:Hyc116_bh3_correctsummarytable.png]]&lt;br /&gt;
&lt;br /&gt;
The above summary table was obtained from the optimisation after adjusting the symmetry. The point shown in this summary table is D&amp;lt;sub&amp;gt;3h&amp;lt;/sub&amp;gt;, which is the correct for BH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;. &lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Items table&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
Below is the items table taken from the optimisation with the correct point group.&lt;br /&gt;
&lt;br /&gt;
&amp;lt;pre&amp;gt;&lt;br /&gt;
Item               Value     Threshold  Converged?&lt;br /&gt;
 Maximum Force            0.000015     0.000450     YES&lt;br /&gt;
 RMS     Force            0.000010     0.000300     YES&lt;br /&gt;
 Maximum Displacement     0.000058     0.001800     YES&lt;br /&gt;
 RMS     Displacement     0.000038     0.001200     YES&lt;br /&gt;
&amp;lt;/pre&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Frequency log file&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
[[Media:HYC116 BH3 FREQ.LOG]] &lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Frequencies&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;pre&amp;gt;&lt;br /&gt;
Low frequencies ---  -10.3498   -3.4492   -1.2454   -0.0055    0.4779    3.2165&lt;br /&gt;
Low frequencies --- 1162.9519 1213.1527 1213.1554&lt;br /&gt;
&amp;lt;/pre&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;jmol of BH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;&#039;&#039;&#039;&lt;br /&gt;
&amp;lt;jmol&amp;gt;&amp;lt;jmolApplet&amp;gt;&lt;br /&gt;
  &amp;lt;title&amp;gt;optimised BH3&amp;lt;/title&amp;gt;&lt;br /&gt;
  &amp;lt;color&amp;gt;black&amp;lt;/color&amp;gt;&lt;br /&gt;
  &amp;lt;size&amp;gt;200&amp;lt;/size&amp;gt;&lt;br /&gt;
  &amp;lt;uploadedFileContents&amp;gt;HYC116_BH3_FREQ.LOG&amp;lt;/uploadedFileContents&amp;gt;&lt;br /&gt;
&amp;lt;/jmolApplet&amp;gt;&amp;lt;/jmol&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
===Vibrational spectrum===&lt;br /&gt;
&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot;&lt;br /&gt;
!wavenumber (cm&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;)&lt;br /&gt;
!Intensity (arbitrary units)&lt;br /&gt;
!symmetry&lt;br /&gt;
!IR active?&lt;br /&gt;
!type&lt;br /&gt;
|-&lt;br /&gt;
|1163&lt;br /&gt;
|93&lt;br /&gt;
|A&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;&#039; &#039;&lt;br /&gt;
|Yes&lt;br /&gt;
|Out of plane bend&lt;br /&gt;
|-&lt;br /&gt;
|1213&lt;br /&gt;
|14&lt;br /&gt;
|E&#039;&lt;br /&gt;
|Very slight&lt;br /&gt;
|Bend&lt;br /&gt;
|-&lt;br /&gt;
|1213&lt;br /&gt;
|14&lt;br /&gt;
|E&#039;&lt;br /&gt;
|Very slight&lt;br /&gt;
|Bend&lt;br /&gt;
|-&lt;br /&gt;
|2582&lt;br /&gt;
|0&lt;br /&gt;
|A&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;&#039;&lt;br /&gt;
|No&lt;br /&gt;
|Symmetric stretch&lt;br /&gt;
|-&lt;br /&gt;
|2716&lt;br /&gt;
|126&lt;br /&gt;
|E&#039;&lt;br /&gt;
|Yes&lt;br /&gt;
|Asymmetric stretch&lt;br /&gt;
|-&lt;br /&gt;
|2716&lt;br /&gt;
|126&lt;br /&gt;
|E&#039;&lt;br /&gt;
|Yes&lt;br /&gt;
|Asymmetric stretch&lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;IR spectrum&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
[[file:Hyc116_ir_bh3.png|400*600]]&lt;br /&gt;
&lt;br /&gt;
There are only three peaks on the IR spectrum of BH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;, despite that there are 6 vibrational modes for the molecule. As shown in the table above, the symmetric stretching mode with A1 symmetry at 2582 cm&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt; is not IR active; naturally, that vibrational mode doesn’t give a peak on the IR spectrum. As shown from the table, two pairs of vibrational modes, the bond angle deformation/bend at 1213 cm&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt; and the asymmetric bond stretch at 2716 cm&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;, are degenerate with the symmetry label E. This means that they have the same energy, and hence give the same wavenumber on the IR spectrum. Each pair of degenerate vibrational modes give rise to one peak. This leaves three peaks, as confirmed by the IR spectrum above.&lt;br /&gt;
&lt;br /&gt;
===Molecular orbitals of BH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;===&lt;br /&gt;
&lt;br /&gt;
[[file:hyc116_bh3_MO_diagram.png]]&lt;br /&gt;
&lt;br /&gt;
The above molecular orbital diagram was taken from Dr Patricia Hunt&#039;s &amp;lt;i&amp;gt;Lecture 4 Tutorial Problem Model Answers&amp;lt;/i&amp;gt;.&amp;lt;ref&amp;gt;P. Hunt, &amp;quot;Lecture 4 Tutorial Problem Model Answers&amp;quot;, 2 (2018)&amp;lt;/ref&amp;gt; Diagrams of the &amp;quot;real&amp;quot; MOs were obtained from Gaussian.&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
There is no significant difference between the LCAO MOs and the real ones. Features such as orbital phases are shown clearly on both the LCAO MOs and the real MOs, illustrating the bonding/anti-bonding characters of the molecular orbitals. This suggests that the the qualitative MO theory is highly accurate and useful when studying the molecular orbitals of molecules.&lt;br /&gt;
&lt;br /&gt;
==Associated energies: ammonium borane==&lt;br /&gt;
&lt;br /&gt;
===NH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;===&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;Calculation type&amp;lt;/b&amp;gt;: Optimisation&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;Calculation Method&amp;lt;/b&amp;gt;: B3LYP&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;Basis set&amp;lt;/b&amp;gt;: 6-31G(d,p) &lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Summary table&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
[[file:Hyc116_nh3_631g_summarytable.png]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Items table&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;pre&amp;gt;&lt;br /&gt;
Item               Value     Threshold  Converged?&lt;br /&gt;
 Maximum Force            0.000006     0.000450     YES&lt;br /&gt;
 RMS     Force            0.000004     0.000300     YES&lt;br /&gt;
 Maximum Displacement     0.000012     0.001800     YES&lt;br /&gt;
 RMS     Displacement     0.000008     0.001200     YES&lt;br /&gt;
&amp;lt;/pre&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Frequency log file&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
[[Media:HYC116_NH3_FREQ.LOG]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Frequencies&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;pre&amp;gt;&lt;br /&gt;
Low frequencies ---   -8.5646   -8.5588   -0.0047    0.0454    0.1784   26.4183&lt;br /&gt;
Low frequencies --- 1089.7603 1694.1865 1694.1865&lt;br /&gt;
&amp;lt;/pre&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;jmol of NH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;&#039;&#039;&#039;&lt;br /&gt;
&amp;lt;jmol&amp;gt;&amp;lt;jmolApplet&amp;gt;&lt;br /&gt;
  &amp;lt;title&amp;gt;optimised NH3&amp;lt;/title&amp;gt;&lt;br /&gt;
  &amp;lt;color&amp;gt;black&amp;lt;/color&amp;gt;&lt;br /&gt;
  &amp;lt;size&amp;gt;200&amp;lt;/size&amp;gt;&lt;br /&gt;
  &amp;lt;uploadedFileContents&amp;gt;HYC116_NH3_FREQ.LOG&amp;lt;/uploadedFileContents&amp;gt;&lt;br /&gt;
&amp;lt;/jmolApplet&amp;gt;&amp;lt;/jmol&amp;gt;&lt;br /&gt;
&lt;br /&gt;
===NH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;BH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;===&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;Calculation type&amp;lt;/b&amp;gt;: Optimisation&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;Calculation Method&amp;lt;/b&amp;gt;: B3LYP&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;Basis set&amp;lt;/b&amp;gt;: 6-31G(d,p) &lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Summary table&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
[[file:Hyc116_nh3bh3_631g_summarytable1.png]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Items table&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;pre&amp;gt;&lt;br /&gt;
Item               Value     Threshold  Converged?&lt;br /&gt;
 Maximum Force            0.000121     0.000450     YES&lt;br /&gt;
 RMS     Force            0.000057     0.000300     YES&lt;br /&gt;
 Maximum Displacement     0.000501     0.001800     YES&lt;br /&gt;
 RMS     Displacement     0.000293     0.001200     YES&lt;br /&gt;
&amp;lt;/pre&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Frequency log file&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
[[Media:HYC116_NH3BH3_FREQ1.LOG]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Frequencies&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;pre&amp;gt;&lt;br /&gt;
Low frequencies ---   -0.0574   -0.0501   -0.0074   21.6276   21.6377   40.3839&lt;br /&gt;
Low frequencies ---  265.9973  632.3725  640.1275&lt;br /&gt;
&amp;lt;/pre&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;jmol of NH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;BH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;&#039;&#039;&#039;&lt;br /&gt;
&amp;lt;jmol&amp;gt;&amp;lt;jmolApplet&amp;gt;&lt;br /&gt;
  &amp;lt;title&amp;gt;optimised NH3BH3&amp;lt;/title&amp;gt;&lt;br /&gt;
  &amp;lt;color&amp;gt;black&amp;lt;/color&amp;gt;&lt;br /&gt;
  &amp;lt;size&amp;gt;200&amp;lt;/size&amp;gt;&lt;br /&gt;
  &amp;lt;uploadedFileContents&amp;gt;HYC116_NH3BH3_FREQ.LOG&amp;lt;/uploadedFileContents&amp;gt;&lt;br /&gt;
&amp;lt;/jmolApplet&amp;gt;&amp;lt;/jmol&amp;gt;&lt;br /&gt;
&lt;br /&gt;
===Association energy===&lt;br /&gt;
&lt;br /&gt;
E(BH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;) (using the optimisation with the correct symmetry) = -26.61532363 a.u. = &amp;lt;b&amp;gt;-26.61532 a.u. (5 d.p.)&amp;lt;/b&amp;gt;&lt;br /&gt;
&lt;br /&gt;
E(NH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;) = -56.55776873 a.u. = &amp;lt;b&amp;gt;-56.55777 a.u. (5 d.p.)&amp;lt;/b&amp;gt;&lt;br /&gt;
&lt;br /&gt;
E(NH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;BH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;) = -83.22468892 a.u. = &amp;lt;b&amp;gt;-83.22469 a.u. (5 d.p.)&amp;lt;/b&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
Carrying out calculations using numbers which has already been rounded up can possibly result in errors in the last digit. Hence, here the calculations were carried out using the numbers provided from the optimisations (i.e. with more decimal places than necessary); the answer was then rounded up to the desired accuracy. &lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
ΔE = E(NH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;BH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;)-[E(NH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;)+E(BH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;)]&lt;br /&gt;
&lt;br /&gt;
ΔE = -83.22468892 - (-56.55776873 + -26.61532363) = -0.05159656 a.u. &lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;ΔE = -0.05160 a.u. (5 d.p.)&amp;lt;/b&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Converting energy from a.u. to kJ/mol&#039;&#039;&#039;&lt;br /&gt;
An atomic unit for energy is Hartree, which is equal to 2625.5 kJ/mol.&lt;br /&gt;
&amp;lt;ref&amp;gt;https://cccbdb.nist.gov/hartree.asp (Accessed: 22.05.2018)&amp;lt;/ref&amp;gt;&lt;br /&gt;
 &lt;br /&gt;
&lt;br /&gt;
So ΔE in kJ/mol = -0.05159657 * 2625.5 = -135.46676828 kJ/mol&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;ΔE = -135 kJ/mol (nearest integer)&amp;lt;/b&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
The energy difference calculated above comes from the formation of the B-N dative bond. It is a relatively weak bond. According to a bond energy data sheet provided by the University of California,&amp;lt;ref&amp;gt;https://labs.chem.ucsb.edu/zakarian/armen/11---bonddissociationenergy.pdf (Accessed: 24.05.2018)&amp;lt;/ref&amp;gt;  the bond energy of the C-C bond of an ethane molecule is 368 kJ/mol. This is a fair comparison to the NH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;BH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt; molecule as the two molecules have the same structure, only with the carbon atoms on ethane swapped for Boron and Nitrogen in NH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;BH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;&lt;br /&gt;
&lt;br /&gt;
==Using a mixture of basis-sets and pseudo-potentials==&lt;br /&gt;
&lt;br /&gt;
===BBr&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;===&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;Calculation type&amp;lt;/b&amp;gt;: Optimisation&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;Calculation Method&amp;lt;/b&amp;gt;: B3LYP&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;Basis set&amp;lt;/b&amp;gt;: Boron: 6-31G(d,p) ; Br: LANL2DZ&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
Larger calculations are often sent to a web-server to run on a high-performance computer instead of a desktop. In order to experience and learn to use a web-server, the optimisation and the frequency analysis for BBr&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt; were both sent and done on a server instead of the desktop. The calculation results were downloaded from the web-server once they were finished.   &lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Summary table&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
[[file:Hyc116_bbr3_opt_summarytable.png]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Items table&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;pre&amp;gt;&lt;br /&gt;
Item               Value     Threshold  Converged?&lt;br /&gt;
 Maximum Force            0.000008     0.000450     YES&lt;br /&gt;
 RMS     Force            0.000005     0.000300     YES&lt;br /&gt;
 Maximum Displacement     0.000036     0.001800     YES&lt;br /&gt;
 RMS     Displacement     0.000023     0.001200     YES&lt;br /&gt;
&amp;lt;/pre&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Frequency log file&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
[[Media:Hyc116_bbr3_freq.log]]&lt;br /&gt;
&lt;br /&gt;
Attached above is the frequency file saved onto the computer from the SCAN server portal. The frequency file was also published on the chemistry database DSpace. {{DOI|10042/202442}}&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Frequencies&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;pre&amp;gt;&lt;br /&gt;
Low frequencies ---   -0.0137   -0.0064   -0.0046    2.4315    2.4315    4.8421&lt;br /&gt;
Low frequencies ---  155.9631  155.9651  267.7052&lt;br /&gt;
&amp;lt;/pre&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;jmol of BBr&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;&#039;&#039;&#039;&lt;br /&gt;
&amp;lt;jmol&amp;gt;&amp;lt;jmolApplet&amp;gt;&lt;br /&gt;
  &amp;lt;title&amp;gt;optimised BBr3&amp;lt;/title&amp;gt;&lt;br /&gt;
  &amp;lt;color&amp;gt;black&amp;lt;/color&amp;gt;&lt;br /&gt;
  &amp;lt;size&amp;gt;200&amp;lt;/size&amp;gt;&lt;br /&gt;
  &amp;lt;uploadedFileContents&amp;gt;Hyc116_bbr3_freq.log&amp;lt;/uploadedFileContents&amp;gt;&lt;br /&gt;
&amp;lt;/jmolApplet&amp;gt;&amp;lt;/jmol&amp;gt;&lt;br /&gt;
&lt;br /&gt;
==Mini project: Aromaticity==&lt;br /&gt;
&lt;br /&gt;
===Benzene===&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;Calculation type&amp;lt;/b&amp;gt;: Optimisation&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;Calculation Method&amp;lt;/b&amp;gt;: B3LYP&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;Basis set&amp;lt;/b&amp;gt;: 6-31G(d,p) &lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Summary table&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
[[file:Hyc116_c6h6_summarytable.png]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Items table&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;pre&amp;gt;&lt;br /&gt;
Item               Value     Threshold  Converged?&lt;br /&gt;
 Maximum Force            0.000193     0.000450     YES&lt;br /&gt;
 RMS     Force            0.000079     0.000300     YES&lt;br /&gt;
 Maximum Displacement     0.000830     0.001800     YES&lt;br /&gt;
 RMS     Displacement     0.000294     0.001200     YES&lt;br /&gt;
&amp;lt;/pre&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Frequency log file&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
[[Media:HYC116_C6H6_FREQ.LOG]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Frequencies&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;pre&amp;gt;&lt;br /&gt;
Low frequencies ---   -3.5606   -3.5606   -0.0089   -0.0043   -0.0043   10.0905&lt;br /&gt;
Low frequencies ---  413.9582  413.9582  621.1416&lt;br /&gt;
&amp;lt;/pre&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;jmol of C&amp;lt;sub&amp;gt;6&amp;lt;/sub&amp;gt;H&amp;lt;sub&amp;gt;6&amp;lt;/sub&amp;gt;&#039;&#039;&#039;&lt;br /&gt;
&amp;lt;jmol&amp;gt;&amp;lt;jmolApplet&amp;gt;&lt;br /&gt;
  &amp;lt;title&amp;gt;optimised Benzene&amp;lt;/title&amp;gt;&lt;br /&gt;
  &amp;lt;color&amp;gt;black&amp;lt;/color&amp;gt;&lt;br /&gt;
  &amp;lt;size&amp;gt;200&amp;lt;/size&amp;gt;&lt;br /&gt;
  &amp;lt;uploadedFileContents&amp;gt;HYC116_C6H6_FREQ.LOG&amp;lt;/uploadedFileContents&amp;gt;&lt;br /&gt;
&amp;lt;/jmolApplet&amp;gt;&amp;lt;/jmol&amp;gt;&lt;br /&gt;
&lt;br /&gt;
===Borazine===&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;Calculation type&amp;lt;/b&amp;gt;: Optimisation&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;Calculation Method&amp;lt;/b&amp;gt;: B3LYP&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;Basis set&amp;lt;/b&amp;gt;: 6-31G(d,p) &lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Summary table&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
[[file:Hyc116_borazine_summarytable.png]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Items table&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;pre&amp;gt;&lt;br /&gt;
Item               Value     Threshold  Converged?&lt;br /&gt;
 Maximum Force            0.000085     0.000450     YES&lt;br /&gt;
 RMS     Force            0.000033     0.000300     YES&lt;br /&gt;
 Maximum Displacement     0.000250     0.001800     YES&lt;br /&gt;
 RMS     Displacement     0.000074     0.001200     YES&lt;br /&gt;
&amp;lt;/pre&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Frequency log file&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
[[Media:HYC116_BORAZINE_FREQ.LOG]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Frequencies&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;pre&amp;gt;&lt;br /&gt;
Low frequencies ---  -12.6626  -12.6626   -8.9272   -0.0211   -0.0104   -0.0104&lt;br /&gt;
Low frequencies ---  289.1112  289.1112  403.8613&lt;br /&gt;
&amp;lt;/pre&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;jmol of Borazine&#039;&#039;&#039;&lt;br /&gt;
&amp;lt;jmol&amp;gt;&amp;lt;jmolApplet&amp;gt;&lt;br /&gt;
  &amp;lt;title&amp;gt;optimised Borazine&amp;lt;/title&amp;gt;&lt;br /&gt;
  &amp;lt;color&amp;gt;black&amp;lt;/color&amp;gt;&lt;br /&gt;
  &amp;lt;size&amp;gt;200&amp;lt;/size&amp;gt;&lt;br /&gt;
  &amp;lt;uploadedFileContents&amp;gt;HYC116_BORAZINE_FREQ.LOG&amp;lt;/uploadedFileContents&amp;gt;&lt;br /&gt;
&amp;lt;/jmolApplet&amp;gt;&amp;lt;/jmol&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
===Charge distribution===&lt;br /&gt;
&lt;br /&gt;
An NBO charge analysis was carried out on both the optimised benzene and borazine. Visualisations of the charge distribution are shown in the table below, with the colour range going from -1.102 to 1.102 for both molecule. This large scale was chosen as it allows direct comparison of the charge on any atoms in these two molecules and shows the relative magnitude of charges on all these atoms. Negative charges are shown in red, and positive charges are shown in green. A neutral charge is displayed in black, so the smaller a charge is (positive or negative), the darker its colour representation is. Larger charges are shown in brighter colours. The charges are also displayed on the atoms as numbers with a neutral charge being zero. Negative charges are shown as negative number and positive charges are shown as positive numbers. &lt;br /&gt;
&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot;&lt;br /&gt;
!&lt;br /&gt;
!Benzene&lt;br /&gt;
!Borazine&lt;br /&gt;
|-&lt;br /&gt;
!Visualisation of charge distribution&lt;br /&gt;
|[[File:Hyc116_benzene_charge_distribution1.png|500x500px|thumb|centre|Charge distribution of Benzene visualisation]]&lt;br /&gt;
|[[File:Hyc116_borazine_charge_distribution1.png|500x500px|thumb|centre|Charge distribution of Borazine visualisation]]&lt;br /&gt;
|-&lt;br /&gt;
!Charge &lt;br /&gt;
|Carbon: -0.239&lt;br /&gt;
&lt;br /&gt;
Hydrogen: 0.239&lt;br /&gt;
|Nitrogen: -1.102 &lt;br /&gt;
&lt;br /&gt;
Boron: 0.747&lt;br /&gt;
&lt;br /&gt;
Hydrogen (bonded to N): 0.432&lt;br /&gt;
&lt;br /&gt;
Hydrogen (bonded to B): -0.077&lt;br /&gt;
|-&lt;br /&gt;
!Discussion&lt;br /&gt;
|From the visualisation, it is shown that there is a slightly negative charge on the carbon atoms, and a positive charge of the same magnitude on the hydrogen atoms. All the carbon atoms have the same charge as they are in identical environments. The same applies to all the hydrogen atoms. This is due to the highly symmetrical structure of benzene. Since the same colour scale was used for both benzene and borazine, and the charges are much smaller in magnitude on atoms in benzene than atoms on borazine, the colours on the charge distribution visualisation is much darker. &lt;br /&gt;
|Polar bonds between nitrogen and boron are demonstration from the above visualisation. From the colours displayed on the charge distribution visualisation as well as the charge values, it is shown that nitrogen has a relatively large negative charge, while boron has a positive charge. This is due to the difference in electrogenativity between these atoms: nitrogen atoms are more electronegative than boron and tends to attract electrons towards themselves. It is worth noting that the hydrogen atoms do not all have the same charge. The hydrogen atoms bonded to boron have a slightly negative charge, and the ones bonded to nitrogen have a small positive charge. &lt;br /&gt;
&lt;br /&gt;
The fact that the same colour scale was used for both molecules comes in helpful here. It allows the charges on atoms to be compared directly. For example, just from looking at the colours, one can tell that or example, even though both carbon and nitrogen are electronegative, nitrogen is much more electronegative, which is quantitatively shown by Pauling&#039;s electronegativity scale.&amp;lt;ref&amp;gt;http://www.tutor-homework.com/Chemistry_Help/electronegativity_table/electronegativity.html (Accessed: 24.0502018&amp;lt;/ref&amp;gt;&lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
===Comparative MOs of Benzene and Borazine===&lt;br /&gt;
&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot;&lt;br /&gt;
!&lt;br /&gt;
!Benzene&lt;br /&gt;
!Borazine&lt;br /&gt;
!Comparison and Discussion&lt;br /&gt;
|-&lt;br /&gt;
!1st comparative pair&lt;br /&gt;
|[[File:Hyc116_benzene_1st_MO_pair_7.png|200x200px|centre]]&lt;br /&gt;
|[[File:Hyc116_borazine_1st_MO_pair_level9.png|200x200px|centre]]&lt;br /&gt;
|MO 9 of both benzene and borazine are comparable. They both show delocalised molecular orbital with an overall bonding character. There is a nodal plane across the molecular orbitals for both benzene and borazine. For benzene, there is contribution from all the carbon and hydrogen s orbitals. Moreover, the molecular orbitals are symmetric to their counterpart of opposite phase, giving an E&amp;lt;sub&amp;gt;1g&amp;lt;/sub&amp;gt; MO. That is not the case for borazine; they are less symmetric in borazine. This MO of borazine has an E&#039; symmetry. Nitrogen atoms are more electronegative than boron atoms and pull electron density towards themselves, resulting in a larger lobe. There is contribution from all the boron and nitrogen s orbitals, and three of the hydrogen s orbitals, though not all of them. &lt;br /&gt;
|-&lt;br /&gt;
!2nd comparative pair&lt;br /&gt;
|[[File:Hyc116_benzene_2nd_MO_pair_10.png|200x200px|centre]]&lt;br /&gt;
|[[File:Hyc116_borazine_2nd_MO_pair_level11.png|200x200px|centre]]&lt;br /&gt;
|MO 10 of benzene and MO 11 of borazine are comparable. Here shows a pair of rather delocalised molecular orbitals with slightly more antibonding character than the first pair shown above. On both MOs, there is no contribution from one pair of opposite hydrogen atoms, but contribution from s orbitals of all other atoms on both molecule. The benzene MO has an E&amp;lt;sub&amp;gt;2g&amp;lt;/sub&amp;gt; symmetry. In borazine, the lobes are in different sizes due to the higher electronegativity of nitrogen. The lobes at the nitrogen atoms are larger as they attract electrons towards themselves more so than boron atoms do. This borazine MO has an E&#039; symmetry. &lt;br /&gt;
|-&lt;br /&gt;
!3rd comparative pair&lt;br /&gt;
|[[File:Hyc116_benzene_3rd_MO_pair_21.png|200x200px|centre]]&lt;br /&gt;
|[[File:Hyc116_borazine_3rd_MO_pair_level21.png|200x200px|centre]]&lt;br /&gt;
|The HOMO (MO 21) of benzene and the HOMO (MO 21) of borazine are comparable. They are both made of p orbitals of all carbon atoms (or all boron and nitrogen atoms in the case of borazine); there is no contribution from hydrogen atoms as they do not have p orbitals. There is a nodal plan perpendicular to the z axis (highest rotational axis) and one parallel to the z axis. On benzene, the MO is very symmetric and has an E&amp;lt;sub&amp;gt;1g&amp;lt;/sub&amp;gt; symmetry; the lobes of the MO are the same in size. On borazine, the lobe where there are two nitrogen atoms is bigger in size, again due to the higher electronegtivity of nitrogen compared to boron. The borazine MO has an E&#039; &#039; symmetry.&lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
===Aromaticity: some theories===&lt;br /&gt;
&lt;br /&gt;
Aromatic compounds display properties such as their high stability and bond lengths between typical single and double bonds. A simple understanding of aromaticity involves the overlap of p orbitals perpendicular to the cyclic plane; the delocalisation of electrons on the pi system is identified to be responsible of the stability of aromatic systems. Aromatic compounds can be identified by the Huckel’s rule, which states that conjugated planar cyclic molecules with (4n +2) π electrons are aromatic. Both benzene and borazine obey the Huckel’s rule and fit the conventional description of aromaticity. &lt;br /&gt;
&lt;br /&gt;
However, it is proved in recent years that the conventional criteria do not necessarily have to be obeyed for a compound to be aromatic. For instance, there has been shown that some non-planar compounds display aromaticity. This suggests that the criteria for aromaticity is not simply structural, and these advances give rise to concepts such as quasiaromaticity and pseudoaromaticity. Recent advances show that there are quantum mechanics basis on the idea of aromaticity. &lt;br /&gt;
In conclusion, while the overlap of pi orbitals provides a simple understanding for aromaticity, it is not a sufficient description for aromaticity.&lt;br /&gt;
&lt;br /&gt;
==References==&lt;br /&gt;
{{reflist}}&lt;/div&gt;</summary>
		<author><name>Hyc116</name></author>
	</entry>
	<entry>
		<id>https://chemwiki.ch.ic.ac.uk/index.php?title=MO_hyc116&amp;diff=732326</id>
		<title>MO hyc116</title>
		<link rel="alternate" type="text/html" href="https://chemwiki.ch.ic.ac.uk/index.php?title=MO_hyc116&amp;diff=732326"/>
		<updated>2018-05-25T14:57:11Z</updated>

		<summary type="html">&lt;p&gt;Hyc116: &lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;==BH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;==&lt;br /&gt;
&lt;br /&gt;
===standard information===&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;Calculation type&amp;lt;/b&amp;gt;: Optimisation&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;Calculation Method&amp;lt;/b&amp;gt;: B3LYP&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;Basis set&amp;lt;/b&amp;gt;: 6-31G(d,p) &lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Summary table&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
[[file:Hyc116_bh3_631g_opt_summarytable.png]]&lt;br /&gt;
&lt;br /&gt;
The above summary table was obtained after the 2nd optimisation of BH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt; (after the initial optimisation using the 3-21G basis set). Notice how the symmetry is incorrect and shown as Cs. This is because the symmetry was manually broken at the beginning by changing the bond length of B-H bonds. The point group was manually adjusted and the molecule was optimised again before the frequency analysis and the new summary table is attached below.&lt;br /&gt;
&lt;br /&gt;
[[file:Hyc116_bh3_correctsummarytable.png]]&lt;br /&gt;
&lt;br /&gt;
The above summary table was obtained from the optimisation after adjusting the symmetry. The point shown in this summary table is D&amp;lt;sub&amp;gt;3h&amp;lt;/sub&amp;gt;, which is the correct for BH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;. &lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Items table&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
Below is the items table taken from the optimisation with the correct point group.&lt;br /&gt;
&lt;br /&gt;
&amp;lt;pre&amp;gt;&lt;br /&gt;
Item               Value     Threshold  Converged?&lt;br /&gt;
 Maximum Force            0.000015     0.000450     YES&lt;br /&gt;
 RMS     Force            0.000010     0.000300     YES&lt;br /&gt;
 Maximum Displacement     0.000058     0.001800     YES&lt;br /&gt;
 RMS     Displacement     0.000038     0.001200     YES&lt;br /&gt;
&amp;lt;/pre&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Frequency log file&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
[[Media:HYC116 BH3 FREQ.LOG]] &lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Frequencies&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;pre&amp;gt;&lt;br /&gt;
Low frequencies ---  -10.3498   -3.4492   -1.2454   -0.0055    0.4779    3.2165&lt;br /&gt;
Low frequencies --- 1162.9519 1213.1527 1213.1554&lt;br /&gt;
&amp;lt;/pre&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;jmol of BH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;&#039;&#039;&#039;&lt;br /&gt;
&amp;lt;jmol&amp;gt;&amp;lt;jmolApplet&amp;gt;&lt;br /&gt;
  &amp;lt;title&amp;gt;optimised BH3&amp;lt;/title&amp;gt;&lt;br /&gt;
  &amp;lt;color&amp;gt;black&amp;lt;/color&amp;gt;&lt;br /&gt;
  &amp;lt;size&amp;gt;200&amp;lt;/size&amp;gt;&lt;br /&gt;
  &amp;lt;uploadedFileContents&amp;gt;HYC116_BH3_FREQ.LOG&amp;lt;/uploadedFileContents&amp;gt;&lt;br /&gt;
&amp;lt;/jmolApplet&amp;gt;&amp;lt;/jmol&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
===Vibrational spectrum===&lt;br /&gt;
&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot;&lt;br /&gt;
!wavenumber (cm&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;)&lt;br /&gt;
!Intensity (arbitrary units)&lt;br /&gt;
!symmetry&lt;br /&gt;
!IR active?&lt;br /&gt;
!type&lt;br /&gt;
|-&lt;br /&gt;
|1163&lt;br /&gt;
|93&lt;br /&gt;
|A&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;&#039; &#039;&lt;br /&gt;
|Yes&lt;br /&gt;
|Out of plane bend&lt;br /&gt;
|-&lt;br /&gt;
|1213&lt;br /&gt;
|14&lt;br /&gt;
|E&#039;&lt;br /&gt;
|Very slight&lt;br /&gt;
|Bend&lt;br /&gt;
|-&lt;br /&gt;
|1213&lt;br /&gt;
|14&lt;br /&gt;
|E&#039;&lt;br /&gt;
|Very slight&lt;br /&gt;
|Bend&lt;br /&gt;
|-&lt;br /&gt;
|2582&lt;br /&gt;
|0&lt;br /&gt;
|A&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;&#039;&lt;br /&gt;
|No&lt;br /&gt;
|Symmetric stretch&lt;br /&gt;
|-&lt;br /&gt;
|2716&lt;br /&gt;
|126&lt;br /&gt;
|E&#039;&lt;br /&gt;
|Yes&lt;br /&gt;
|Asymmetric stretch&lt;br /&gt;
|-&lt;br /&gt;
|2716&lt;br /&gt;
|126&lt;br /&gt;
|E&#039;&lt;br /&gt;
|Yes&lt;br /&gt;
|Asymmetric stretch&lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;IR spectrum&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
[[file:Hyc116_ir_bh3.png|400*600]]&lt;br /&gt;
&lt;br /&gt;
There are only three peaks on the IR spectrum of BH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;, despite that there are 6 vibrational modes for the molecule. As shown in the table above, the symmetric stretching mode with A1 symmetry at 2582 cm&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt; is not IR active; naturally, that vibrational mode doesn’t give a peak on the IR spectrum. As shown from the table, two pairs of vibrational modes, the bond angle deformation/bend at 1213 cm&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt; and the asymmetric bond stretch at 2716 cm&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;, are degenerate with the symmetry label E. This means that they have the same energy, and hence give the same wavenumber on the IR spectrum. Each pair of degenerate vibrational modes give rise to one peak. This leaves three peaks, as confirmed by the IR spectrum above.&lt;br /&gt;
&lt;br /&gt;
===Molecular orbitals of BH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;===&lt;br /&gt;
&lt;br /&gt;
[[file:hyc116_bh3_MO_diagram.png]]&lt;br /&gt;
&lt;br /&gt;
The above molecular orbital diagram was taken from Dr Patricia Hunt&#039;s &amp;lt;i&amp;gt;Lecture 4 Tutorial Problem Model Answers&amp;lt;/i&amp;gt;.&amp;lt;ref&amp;gt;P. Hunt, &amp;quot;Lecture 4 Tutorial Problem Model Answers&amp;quot;, 2 (2018)&amp;lt;/ref&amp;gt; Diagrams of the &amp;quot;real&amp;quot; MOs were obtained from Gaussian.&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
There is no significant difference between the LCAO MOs and the real ones. Features such as orbital phases are shown clearly on both the LCAO MOs and the real MOs, illustrating the bonding/anti-bonding characters of the molecular orbitals. This suggests that the the qualitative MO theory is highly accurate and useful when studying the molecular orbitals of molecules.&lt;br /&gt;
&lt;br /&gt;
==Associated energies: ammonium borane==&lt;br /&gt;
&lt;br /&gt;
===NH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;===&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;Calculation type&amp;lt;/b&amp;gt;: Optimisation&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;Calculation Method&amp;lt;/b&amp;gt;: B3LYP&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;Basis set&amp;lt;/b&amp;gt;: 6-31G(d,p) &lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Summary table&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
[[file:Hyc116_nh3_631g_summarytable.png]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Items table&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;pre&amp;gt;&lt;br /&gt;
Item               Value     Threshold  Converged?&lt;br /&gt;
 Maximum Force            0.000006     0.000450     YES&lt;br /&gt;
 RMS     Force            0.000004     0.000300     YES&lt;br /&gt;
 Maximum Displacement     0.000012     0.001800     YES&lt;br /&gt;
 RMS     Displacement     0.000008     0.001200     YES&lt;br /&gt;
&amp;lt;/pre&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Frequency log file&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
[[Media:HYC116_NH3_FREQ.LOG]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Frequencies&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;pre&amp;gt;&lt;br /&gt;
Low frequencies ---   -8.5646   -8.5588   -0.0047    0.0454    0.1784   26.4183&lt;br /&gt;
Low frequencies --- 1089.7603 1694.1865 1694.1865&lt;br /&gt;
&amp;lt;/pre&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;jmol of NH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;&#039;&#039;&#039;&lt;br /&gt;
&amp;lt;jmol&amp;gt;&amp;lt;jmolApplet&amp;gt;&lt;br /&gt;
  &amp;lt;title&amp;gt;optimised NH3&amp;lt;/title&amp;gt;&lt;br /&gt;
  &amp;lt;color&amp;gt;black&amp;lt;/color&amp;gt;&lt;br /&gt;
  &amp;lt;size&amp;gt;200&amp;lt;/size&amp;gt;&lt;br /&gt;
  &amp;lt;uploadedFileContents&amp;gt;HYC116_NH3_FREQ.LOG&amp;lt;/uploadedFileContents&amp;gt;&lt;br /&gt;
&amp;lt;/jmolApplet&amp;gt;&amp;lt;/jmol&amp;gt;&lt;br /&gt;
&lt;br /&gt;
===NH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;BH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;===&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;Calculation type&amp;lt;/b&amp;gt;: Optimisation&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;Calculation Method&amp;lt;/b&amp;gt;: B3LYP&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;Basis set&amp;lt;/b&amp;gt;: 6-31G(d,p) &lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Summary table&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
[[file:Hyc116_nh3bh3_631g_summarytable1.png]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Items table&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;pre&amp;gt;&lt;br /&gt;
Item               Value     Threshold  Converged?&lt;br /&gt;
 Maximum Force            0.000121     0.000450     YES&lt;br /&gt;
 RMS     Force            0.000057     0.000300     YES&lt;br /&gt;
 Maximum Displacement     0.000501     0.001800     YES&lt;br /&gt;
 RMS     Displacement     0.000293     0.001200     YES&lt;br /&gt;
&amp;lt;/pre&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Frequency log file&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
[[Media:HYC116_NH3BH3_FREQ1.LOG]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Frequencies&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;pre&amp;gt;&lt;br /&gt;
Low frequencies ---   -0.0574   -0.0501   -0.0074   21.6276   21.6377   40.3839&lt;br /&gt;
Low frequencies ---  265.9973  632.3725  640.1275&lt;br /&gt;
&amp;lt;/pre&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;jmol of NH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;BH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;&#039;&#039;&#039;&lt;br /&gt;
&amp;lt;jmol&amp;gt;&amp;lt;jmolApplet&amp;gt;&lt;br /&gt;
  &amp;lt;title&amp;gt;optimised NH3BH3&amp;lt;/title&amp;gt;&lt;br /&gt;
  &amp;lt;color&amp;gt;black&amp;lt;/color&amp;gt;&lt;br /&gt;
  &amp;lt;size&amp;gt;200&amp;lt;/size&amp;gt;&lt;br /&gt;
  &amp;lt;uploadedFileContents&amp;gt;HYC116_NH3BH3_FREQ.LOG&amp;lt;/uploadedFileContents&amp;gt;&lt;br /&gt;
&amp;lt;/jmolApplet&amp;gt;&amp;lt;/jmol&amp;gt;&lt;br /&gt;
&lt;br /&gt;
===Association energy===&lt;br /&gt;
&lt;br /&gt;
E(BH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;) (using the optimisation with the correct symmetry) = -26.61532363 a.u. = &amp;lt;b&amp;gt;-26.61532 a.u. (5 d.p.)&amp;lt;/b&amp;gt;&lt;br /&gt;
&lt;br /&gt;
E(NH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;) = -56.55776873 a.u. = &amp;lt;b&amp;gt;-56.55777 a.u. (5 d.p.)&amp;lt;/b&amp;gt;&lt;br /&gt;
&lt;br /&gt;
E(NH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;BH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;) = -83.22468892 a.u. = &amp;lt;b&amp;gt;-83.22469 a.u. (5 d.p.)&amp;lt;/b&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
Carrying out calculations using numbers which has already been rounded up can possibly result in errors in the last digit. Hence, here the calculations were carried out using the numbers provided from the optimisations (i.e. with more decimal places than necessary); the answer was then rounded up to the desired accuracy. &lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
ΔE = E(NH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;BH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;)-[E(NH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;)+E(BH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;)]&lt;br /&gt;
&lt;br /&gt;
ΔE = -83.22468892 - (-56.55776873 + -26.61532363) = -0.05159656 a.u. &lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;ΔE = -0.05160 a.u. (5 d.p.)&amp;lt;/b&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Converting energy from a.u. to kJ/mol&#039;&#039;&#039;&lt;br /&gt;
An atomic unit for energy is Hartree, which is equal to 2625.5 kJ/mol.&lt;br /&gt;
&amp;lt;ref&amp;gt;https://cccbdb.nist.gov/hartree.asp (Accessed: 22.05.2018)&amp;lt;/ref&amp;gt;&lt;br /&gt;
 &lt;br /&gt;
&lt;br /&gt;
So ΔE in kJ/mol = -0.05159657 * 2625.5 = -135.46676828 kJ/mol&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;ΔE = -135 kJ/mol (nearest integer)&amp;lt;/b&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
The energy difference calculated above comes from the formation of the B-N dative bond. It is a relatively weak bond. According to a bond energy data sheet provided by the University of California,&amp;lt;ref&amp;gt;https://labs.chem.ucsb.edu/zakarian/armen/11---bonddissociationenergy.pdf (Accessed: 24.05.2018)&amp;lt;/ref&amp;gt;  the bond energy of the C-C bond of an ethane molecule is 368 kJ/mol. This is a fair comparison to the NH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;BH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt; molecule as the two molecules have the same structure, only with the carbon atoms on ethane swapped for Boron and Nitrogen in NH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;BH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;&lt;br /&gt;
&lt;br /&gt;
==Using a mixture of basis-sets and pseudo-potentials==&lt;br /&gt;
&lt;br /&gt;
===BBr&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;===&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;Calculation type&amp;lt;/b&amp;gt;: Optimisation&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;Calculation Method&amp;lt;/b&amp;gt;: B3LYP&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;Basis set&amp;lt;/b&amp;gt;: Boron: 6-31G(d,p) ; Br: LANL2DZ&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
Larger calculations are often sent to a web-server to run on a high-performance computer instead of a desktop. In order to experience and learn to use a web-server, the optimisation and the frequency analysis for BBr&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt; were both sent and done on a server instead of the desktop. The calculation results were downloaded from the web-server once they were finished.   &lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Summary table&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
[[file:Hyc116_bbr3_opt_summarytable.png]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Items table&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;pre&amp;gt;&lt;br /&gt;
Item               Value     Threshold  Converged?&lt;br /&gt;
 Maximum Force            0.000008     0.000450     YES&lt;br /&gt;
 RMS     Force            0.000005     0.000300     YES&lt;br /&gt;
 Maximum Displacement     0.000036     0.001800     YES&lt;br /&gt;
 RMS     Displacement     0.000023     0.001200     YES&lt;br /&gt;
&amp;lt;/pre&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Frequency log file&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
[[Media:Hyc116_bbr3_freq.log]]&lt;br /&gt;
&lt;br /&gt;
Attached above is the frequency file saved onto the computer from the SCAN server portal. The frequency file was also published on the chemistry database DSpace. {{DOI|10042/202442}}&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Frequencies&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;pre&amp;gt;&lt;br /&gt;
Low frequencies ---   -0.0137   -0.0064   -0.0046    2.4315    2.4315    4.8421&lt;br /&gt;
Low frequencies ---  155.9631  155.9651  267.7052&lt;br /&gt;
&amp;lt;/pre&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;jmol of BBr&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;&#039;&#039;&#039;&lt;br /&gt;
&amp;lt;jmol&amp;gt;&amp;lt;jmolApplet&amp;gt;&lt;br /&gt;
  &amp;lt;title&amp;gt;optimised BBr3&amp;lt;/title&amp;gt;&lt;br /&gt;
  &amp;lt;color&amp;gt;black&amp;lt;/color&amp;gt;&lt;br /&gt;
  &amp;lt;size&amp;gt;200&amp;lt;/size&amp;gt;&lt;br /&gt;
  &amp;lt;uploadedFileContents&amp;gt;Hyc116_bbr3_freq.log&amp;lt;/uploadedFileContents&amp;gt;&lt;br /&gt;
&amp;lt;/jmolApplet&amp;gt;&amp;lt;/jmol&amp;gt;&lt;br /&gt;
&lt;br /&gt;
==Aromaticity==&lt;br /&gt;
&lt;br /&gt;
===Benzene===&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;Calculation type&amp;lt;/b&amp;gt;: Optimisation&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;Calculation Method&amp;lt;/b&amp;gt;: B3LYP&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;Basis set&amp;lt;/b&amp;gt;: 6-31G(d,p) &lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Summary table&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
[[file:Hyc116_c6h6_summarytable.png]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Items table&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;pre&amp;gt;&lt;br /&gt;
Item               Value     Threshold  Converged?&lt;br /&gt;
 Maximum Force            0.000193     0.000450     YES&lt;br /&gt;
 RMS     Force            0.000079     0.000300     YES&lt;br /&gt;
 Maximum Displacement     0.000830     0.001800     YES&lt;br /&gt;
 RMS     Displacement     0.000294     0.001200     YES&lt;br /&gt;
&amp;lt;/pre&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Frequency log file&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
[[Media:HYC116_C6H6_FREQ.LOG]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Frequencies&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;pre&amp;gt;&lt;br /&gt;
Low frequencies ---   -3.5606   -3.5606   -0.0089   -0.0043   -0.0043   10.0905&lt;br /&gt;
Low frequencies ---  413.9582  413.9582  621.1416&lt;br /&gt;
&amp;lt;/pre&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;jmol of C&amp;lt;sub&amp;gt;6&amp;lt;/sub&amp;gt;H&amp;lt;sub&amp;gt;6&amp;lt;/sub&amp;gt;&#039;&#039;&#039;&lt;br /&gt;
&amp;lt;jmol&amp;gt;&amp;lt;jmolApplet&amp;gt;&lt;br /&gt;
  &amp;lt;title&amp;gt;optimised Benzene&amp;lt;/title&amp;gt;&lt;br /&gt;
  &amp;lt;color&amp;gt;black&amp;lt;/color&amp;gt;&lt;br /&gt;
  &amp;lt;size&amp;gt;200&amp;lt;/size&amp;gt;&lt;br /&gt;
  &amp;lt;uploadedFileContents&amp;gt;HYC116_C6H6_FREQ.LOG&amp;lt;/uploadedFileContents&amp;gt;&lt;br /&gt;
&amp;lt;/jmolApplet&amp;gt;&amp;lt;/jmol&amp;gt;&lt;br /&gt;
&lt;br /&gt;
===Borazine===&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;Calculation type&amp;lt;/b&amp;gt;: Optimisation&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;Calculation Method&amp;lt;/b&amp;gt;: B3LYP&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;Basis set&amp;lt;/b&amp;gt;: 6-31G(d,p) &lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Summary table&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
[[file:Hyc116_borazine_summarytable.png]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Items table&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;pre&amp;gt;&lt;br /&gt;
Item               Value     Threshold  Converged?&lt;br /&gt;
 Maximum Force            0.000085     0.000450     YES&lt;br /&gt;
 RMS     Force            0.000033     0.000300     YES&lt;br /&gt;
 Maximum Displacement     0.000250     0.001800     YES&lt;br /&gt;
 RMS     Displacement     0.000074     0.001200     YES&lt;br /&gt;
&amp;lt;/pre&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Frequency log file&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
[[Media:HYC116_BORAZINE_FREQ.LOG]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Frequencies&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;pre&amp;gt;&lt;br /&gt;
Low frequencies ---  -12.6626  -12.6626   -8.9272   -0.0211   -0.0104   -0.0104&lt;br /&gt;
Low frequencies ---  289.1112  289.1112  403.8613&lt;br /&gt;
&amp;lt;/pre&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;jmol of Borazine&#039;&#039;&#039;&lt;br /&gt;
&amp;lt;jmol&amp;gt;&amp;lt;jmolApplet&amp;gt;&lt;br /&gt;
  &amp;lt;title&amp;gt;optimised Borazine&amp;lt;/title&amp;gt;&lt;br /&gt;
  &amp;lt;color&amp;gt;black&amp;lt;/color&amp;gt;&lt;br /&gt;
  &amp;lt;size&amp;gt;200&amp;lt;/size&amp;gt;&lt;br /&gt;
  &amp;lt;uploadedFileContents&amp;gt;HYC116_BORAZINE_FREQ.LOG&amp;lt;/uploadedFileContents&amp;gt;&lt;br /&gt;
&amp;lt;/jmolApplet&amp;gt;&amp;lt;/jmol&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
===Charge distribution===&lt;br /&gt;
&lt;br /&gt;
An NBO charge analysis was carried out on both the optimised benzene and borazine. Visualisations of the charge distribution are shown in the table below, with the colour range going from -1.102 to 1.102 for both molecule. This large scale was chosen as it allows direct comparison of the charge on any atoms in these two molecules and shows the relative magnitude of charges on all these atoms. Negative charges are shown in red, and positive charges are shown in green. A neutral charge is displayed in black, so the smaller a charge is (positive or negative), the darker its colour representation is. Larger charges are shown in brighter colours. The charges are also displayed on the atoms as numbers with a neutral charge being zero. Negative charges are shown as negative number and positive charges are shown as positive numbers. &lt;br /&gt;
&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot;&lt;br /&gt;
!&lt;br /&gt;
!Benzene&lt;br /&gt;
!Borazine&lt;br /&gt;
|-&lt;br /&gt;
!Visualisation of charge distribution&lt;br /&gt;
|[[File:Hyc116_benzene_charge_distribution1.png|500x500px|thumb|centre|Charge distribution of Benzene visualisation]]&lt;br /&gt;
|[[File:Hyc116_borazine_charge_distribution1.png|500x500px|thumb|centre|Charge distribution of Borazine visualisation]]&lt;br /&gt;
|-&lt;br /&gt;
!Charge &lt;br /&gt;
|Carbon: -0.239&lt;br /&gt;
&lt;br /&gt;
Hydrogen: 0.239&lt;br /&gt;
|Nitrogen: -1.102 &lt;br /&gt;
&lt;br /&gt;
Boron: 0.747&lt;br /&gt;
&lt;br /&gt;
Hydrogen (bonded to N): 0.432&lt;br /&gt;
&lt;br /&gt;
Hydrogen (bonded to B): -0.077&lt;br /&gt;
|-&lt;br /&gt;
!Discussion&lt;br /&gt;
|From the visualisation, it is shown that there is a slightly negative charge on the carbon atoms, and a positive charge of the same magnitude on the hydrogen atoms. All the carbon atoms have the same charge as they are in identical environments. The same applies to all the hydrogen atoms. This is due to the highly symmetrical structure of benzene. Since the same colour scale was used for both benzene and borazine, and the charges are much smaller in magnitude on atoms in benzene than atoms on borazine, the colours on the charge distribution visualisation is much darker. &lt;br /&gt;
|Polar bonds between nitrogen and boron are demonstration from the above visualisation. From the colours displayed on the charge distribution visualisation as well as the charge values, it is shown that nitrogen has a relatively large negative charge, while boron has a positive charge. This is due to the difference in electrogenativity between these atoms: nitrogen atoms are more electronegative than boron and tends to attract electrons towards themselves. It is worth noting that the hydrogen atoms do not all have the same charge. The hydrogen atoms bonded to boron have a slightly negative charge, and the ones bonded to nitrogen have a small positive charge. &lt;br /&gt;
&lt;br /&gt;
The fact that the same colour scale was used for both molecules comes in helpful here. It allows the charges on atoms to be compared directly. For example, just from looking at the colours, one can tell that or example, even though both carbon and nitrogen are electronegative, nitrogen is much more electronegative, which is quantitatively shown by Pauling&#039;s electronegativity scale.&amp;lt;ref&amp;gt;http://www.tutor-homework.com/Chemistry_Help/electronegativity_table/electronegativity.html (Accessed: 24.0502018&amp;lt;/ref&amp;gt;&lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
===Comparative MOs of Benzene and Borazine===&lt;br /&gt;
&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot;&lt;br /&gt;
!&lt;br /&gt;
!Benzene&lt;br /&gt;
!Borazine&lt;br /&gt;
!Comparison and Discussion&lt;br /&gt;
|-&lt;br /&gt;
!1st comparative pair&lt;br /&gt;
|[[File:Hyc116_benzene_1st_MO_pair_7.png|200x200px|centre]]&lt;br /&gt;
|[[File:Hyc116_borazine_1st_MO_pair_level9.png|200x200px|centre]]&lt;br /&gt;
|MO 9 of both benzene and borazine are comparable. They both show delocalised molecular orbital with an overall bonding character. There is a nodal plane across the molecular orbitals for both benzene and borazine. For benzene, there is contribution from all the carbon and hydrogen s orbitals. Moreover, the molecular orbitals are symmetric to their counterpart of opposite phase, giving an E&amp;lt;sub&amp;gt;1g&amp;lt;/sub&amp;gt; MO. That is not the case for borazine; they are less symmetric in borazine. This MO of borazine has an E&#039; symmetry. Nitrogen atoms are more electronegative than boron atoms and pull electron density towards themselves, resulting in a larger lobe. There is contribution from all the boron and nitrogen s orbitals, and three of the hydrogen s orbitals, though not all of them. &lt;br /&gt;
|-&lt;br /&gt;
!2nd comparative pair&lt;br /&gt;
|[[File:Hyc116_benzene_2nd_MO_pair_10.png|200x200px|centre]]&lt;br /&gt;
|[[File:Hyc116_borazine_2nd_MO_pair_level11.png|200x200px|centre]]&lt;br /&gt;
|MO 10 of benzene and MO 11 of borazine are comparable. Here shows a pair of rather delocalised molecular orbitals with slightly more antibonding character than the first pair shown above. On both MOs, there is no contribution from one pair of opposite hydrogen atoms, but contribution from s orbitals of all other atoms on both molecule. The benzene MO has an E&amp;lt;sub&amp;gt;2g&amp;lt;/sub&amp;gt; symmetry. In borazine, the lobes are in different sizes due to the higher electronegativity of nitrogen. The lobes at the nitrogen atoms are larger as they attract electrons towards themselves more so than boron atoms do. This borazine MO has an E&#039; symmetry. &lt;br /&gt;
|-&lt;br /&gt;
!3rd comparative pair&lt;br /&gt;
|[[File:Hyc116_benzene_3rd_MO_pair_21.png|200x200px|centre]]&lt;br /&gt;
|[[File:Hyc116_borazine_3rd_MO_pair_level21.png|200x200px|centre]]&lt;br /&gt;
|The HOMO (MO 21) of benzene and the HOMO (MO 21) of borazine are comparable. They are both made of p orbitals of all carbon atoms (or all boron and nitrogen atoms in the case of borazine); there is no contribution from hydrogen atoms as they do not have p orbitals. There is a nodal plan perpendicular to the z axis (highest rotational axis) and one parallel to the z axis. On benzene, the MO is very symmetric and has an E&amp;lt;sub&amp;gt;1g&amp;lt;/sub&amp;gt; symmetry; the lobes of the MO are the same in size. On borazine, the lobe where there are two nitrogen atoms is bigger in size, again due to the higher electronegtivity of nitrogen compared to boron. The borazine MO has an E&#039; &#039; symmetry.&lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
===Aromaticity: some theories===&lt;br /&gt;
&lt;br /&gt;
Aromatic compounds display properties such as their high stability and bond lengths between typical single and double bonds. A simple understanding of aromaticity involves the overlap of p orbitals perpendicular to the cyclic plane; the delocalisation of electrons on the pi system is identified to be responsible of the stability of aromatic systems. Aromatic compounds can be identified by the Huckel’s rule, which states that conjugated planar cyclic molecules with (4n +2) π electrons are aromatic. Both benzene and borazine obey the Huckel’s rule and fit the conventional description of aromaticity. &lt;br /&gt;
&lt;br /&gt;
However, it is proved in recent years that the conventional criteria do not necessarily have to be obeyed for a compound to be aromatic. For instance, there has been shown that some non-planar compounds display aromaticity. This suggests that the criteria for aromaticity is not simply structural, and these advances give rise to concepts such as quasiaromaticity and pseudoaromaticity. Recent advances show that there are quantum mechanics basis on the idea of aromaticity. &lt;br /&gt;
In conclusion, while the overlap of pi orbitals provides a simple understanding for aromaticity, it is not a sufficient description for aromaticity.&lt;br /&gt;
&lt;br /&gt;
==References==&lt;br /&gt;
{{reflist}}&lt;/div&gt;</summary>
		<author><name>Hyc116</name></author>
	</entry>
	<entry>
		<id>https://chemwiki.ch.ic.ac.uk/index.php?title=MO_hyc116&amp;diff=732322</id>
		<title>MO hyc116</title>
		<link rel="alternate" type="text/html" href="https://chemwiki.ch.ic.ac.uk/index.php?title=MO_hyc116&amp;diff=732322"/>
		<updated>2018-05-25T14:56:47Z</updated>

		<summary type="html">&lt;p&gt;Hyc116: &lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;=BH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;=&lt;br /&gt;
&lt;br /&gt;
===standard information===&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;Calculation type&amp;lt;/b&amp;gt;: Optimisation&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;Calculation Method&amp;lt;/b&amp;gt;: B3LYP&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;Basis set&amp;lt;/b&amp;gt;: 6-31G(d,p) &lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Summary table&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
[[file:Hyc116_bh3_631g_opt_summarytable.png]]&lt;br /&gt;
&lt;br /&gt;
The above summary table was obtained after the 2nd optimisation of BH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt; (after the initial optimisation using the 3-21G basis set). Notice how the symmetry is incorrect and shown as Cs. This is because the symmetry was manually broken at the beginning by changing the bond length of B-H bonds. The point group was manually adjusted and the molecule was optimised again before the frequency analysis and the new summary table is attached below.&lt;br /&gt;
&lt;br /&gt;
[[file:Hyc116_bh3_correctsummarytable.png]]&lt;br /&gt;
&lt;br /&gt;
The above summary table was obtained from the optimisation after adjusting the symmetry. The point shown in this summary table is D&amp;lt;sub&amp;gt;3h&amp;lt;/sub&amp;gt;, which is the correct for BH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;. &lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Items table&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
Below is the items table taken from the optimisation with the correct point group.&lt;br /&gt;
&lt;br /&gt;
&amp;lt;pre&amp;gt;&lt;br /&gt;
Item               Value     Threshold  Converged?&lt;br /&gt;
 Maximum Force            0.000015     0.000450     YES&lt;br /&gt;
 RMS     Force            0.000010     0.000300     YES&lt;br /&gt;
 Maximum Displacement     0.000058     0.001800     YES&lt;br /&gt;
 RMS     Displacement     0.000038     0.001200     YES&lt;br /&gt;
&amp;lt;/pre&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Frequency log file&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
[[Media:HYC116 BH3 FREQ.LOG]] &lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Frequencies&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;pre&amp;gt;&lt;br /&gt;
Low frequencies ---  -10.3498   -3.4492   -1.2454   -0.0055    0.4779    3.2165&lt;br /&gt;
Low frequencies --- 1162.9519 1213.1527 1213.1554&lt;br /&gt;
&amp;lt;/pre&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;jmol of BH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;&#039;&#039;&#039;&lt;br /&gt;
&amp;lt;jmol&amp;gt;&amp;lt;jmolApplet&amp;gt;&lt;br /&gt;
  &amp;lt;title&amp;gt;optimised BH3&amp;lt;/title&amp;gt;&lt;br /&gt;
  &amp;lt;color&amp;gt;black&amp;lt;/color&amp;gt;&lt;br /&gt;
  &amp;lt;size&amp;gt;200&amp;lt;/size&amp;gt;&lt;br /&gt;
  &amp;lt;uploadedFileContents&amp;gt;HYC116_BH3_FREQ.LOG&amp;lt;/uploadedFileContents&amp;gt;&lt;br /&gt;
&amp;lt;/jmolApplet&amp;gt;&amp;lt;/jmol&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
===Vibrational spectrum===&lt;br /&gt;
&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot;&lt;br /&gt;
!wavenumber (cm&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;)&lt;br /&gt;
!Intensity (arbitrary units)&lt;br /&gt;
!symmetry&lt;br /&gt;
!IR active?&lt;br /&gt;
!type&lt;br /&gt;
|-&lt;br /&gt;
|1163&lt;br /&gt;
|93&lt;br /&gt;
|A&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;&#039; &#039;&lt;br /&gt;
|Yes&lt;br /&gt;
|Out of plane bend&lt;br /&gt;
|-&lt;br /&gt;
|1213&lt;br /&gt;
|14&lt;br /&gt;
|E&#039;&lt;br /&gt;
|Very slight&lt;br /&gt;
|Bend&lt;br /&gt;
|-&lt;br /&gt;
|1213&lt;br /&gt;
|14&lt;br /&gt;
|E&#039;&lt;br /&gt;
|Very slight&lt;br /&gt;
|Bend&lt;br /&gt;
|-&lt;br /&gt;
|2582&lt;br /&gt;
|0&lt;br /&gt;
|A&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;&#039;&lt;br /&gt;
|No&lt;br /&gt;
|Symmetric stretch&lt;br /&gt;
|-&lt;br /&gt;
|2716&lt;br /&gt;
|126&lt;br /&gt;
|E&#039;&lt;br /&gt;
|Yes&lt;br /&gt;
|Asymmetric stretch&lt;br /&gt;
|-&lt;br /&gt;
|2716&lt;br /&gt;
|126&lt;br /&gt;
|E&#039;&lt;br /&gt;
|Yes&lt;br /&gt;
|Asymmetric stretch&lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;IR spectrum&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
[[file:Hyc116_ir_bh3.png|400*600]]&lt;br /&gt;
&lt;br /&gt;
There are only three peaks on the IR spectrum of BH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;, despite that there are 6 vibrational modes for the molecule. As shown in the table above, the symmetric stretching mode with A1 symmetry at 2582 cm&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt; is not IR active; naturally, that vibrational mode doesn’t give a peak on the IR spectrum. As shown from the table, two pairs of vibrational modes, the bond angle deformation/bend at 1213 cm&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt; and the asymmetric bond stretch at 2716 cm&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;, are degenerate with the symmetry label E. This means that they have the same energy, and hence give the same wavenumber on the IR spectrum. Each pair of degenerate vibrational modes give rise to one peak. This leaves three peaks, as confirmed by the IR spectrum above.&lt;br /&gt;
&lt;br /&gt;
===Molecular orbitals of BH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;===&lt;br /&gt;
&lt;br /&gt;
[[file:hyc116_bh3_MO_diagram.png]]&lt;br /&gt;
&lt;br /&gt;
The above molecular orbital diagram was taken from Dr Patricia Hunt&#039;s &amp;lt;i&amp;gt;Lecture 4 Tutorial Problem Model Answers&amp;lt;/i&amp;gt;.&amp;lt;ref&amp;gt;P. Hunt, &amp;quot;Lecture 4 Tutorial Problem Model Answers&amp;quot;, 2 (2018)&amp;lt;/ref&amp;gt; Diagrams of the &amp;quot;real&amp;quot; MOs were obtained from Gaussian.&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
There is no significant difference between the LCAO MOs and the real ones. Features such as orbital phases are shown clearly on both the LCAO MOs and the real MOs, illustrating the bonding/anti-bonding characters of the molecular orbitals. This suggests that the the qualitative MO theory is highly accurate and useful when studying the molecular orbitals of molecules.&lt;br /&gt;
&lt;br /&gt;
==Associated energies: ammonium borane==&lt;br /&gt;
&lt;br /&gt;
===NH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;===&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;Calculation type&amp;lt;/b&amp;gt;: Optimisation&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;Calculation Method&amp;lt;/b&amp;gt;: B3LYP&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;Basis set&amp;lt;/b&amp;gt;: 6-31G(d,p) &lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Summary table&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
[[file:Hyc116_nh3_631g_summarytable.png]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Items table&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;pre&amp;gt;&lt;br /&gt;
Item               Value     Threshold  Converged?&lt;br /&gt;
 Maximum Force            0.000006     0.000450     YES&lt;br /&gt;
 RMS     Force            0.000004     0.000300     YES&lt;br /&gt;
 Maximum Displacement     0.000012     0.001800     YES&lt;br /&gt;
 RMS     Displacement     0.000008     0.001200     YES&lt;br /&gt;
&amp;lt;/pre&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Frequency log file&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
[[Media:HYC116_NH3_FREQ.LOG]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Frequencies&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;pre&amp;gt;&lt;br /&gt;
Low frequencies ---   -8.5646   -8.5588   -0.0047    0.0454    0.1784   26.4183&lt;br /&gt;
Low frequencies --- 1089.7603 1694.1865 1694.1865&lt;br /&gt;
&amp;lt;/pre&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;jmol of NH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;&#039;&#039;&#039;&lt;br /&gt;
&amp;lt;jmol&amp;gt;&amp;lt;jmolApplet&amp;gt;&lt;br /&gt;
  &amp;lt;title&amp;gt;optimised NH3&amp;lt;/title&amp;gt;&lt;br /&gt;
  &amp;lt;color&amp;gt;black&amp;lt;/color&amp;gt;&lt;br /&gt;
  &amp;lt;size&amp;gt;200&amp;lt;/size&amp;gt;&lt;br /&gt;
  &amp;lt;uploadedFileContents&amp;gt;HYC116_NH3_FREQ.LOG&amp;lt;/uploadedFileContents&amp;gt;&lt;br /&gt;
&amp;lt;/jmolApplet&amp;gt;&amp;lt;/jmol&amp;gt;&lt;br /&gt;
&lt;br /&gt;
===NH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;BH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;===&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;Calculation type&amp;lt;/b&amp;gt;: Optimisation&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;Calculation Method&amp;lt;/b&amp;gt;: B3LYP&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;Basis set&amp;lt;/b&amp;gt;: 6-31G(d,p) &lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Summary table&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
[[file:Hyc116_nh3bh3_631g_summarytable1.png]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Items table&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;pre&amp;gt;&lt;br /&gt;
Item               Value     Threshold  Converged?&lt;br /&gt;
 Maximum Force            0.000121     0.000450     YES&lt;br /&gt;
 RMS     Force            0.000057     0.000300     YES&lt;br /&gt;
 Maximum Displacement     0.000501     0.001800     YES&lt;br /&gt;
 RMS     Displacement     0.000293     0.001200     YES&lt;br /&gt;
&amp;lt;/pre&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Frequency log file&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
[[Media:HYC116_NH3BH3_FREQ1.LOG]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Frequencies&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;pre&amp;gt;&lt;br /&gt;
Low frequencies ---   -0.0574   -0.0501   -0.0074   21.6276   21.6377   40.3839&lt;br /&gt;
Low frequencies ---  265.9973  632.3725  640.1275&lt;br /&gt;
&amp;lt;/pre&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;jmol of NH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;BH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;&#039;&#039;&#039;&lt;br /&gt;
&amp;lt;jmol&amp;gt;&amp;lt;jmolApplet&amp;gt;&lt;br /&gt;
  &amp;lt;title&amp;gt;optimised NH3BH3&amp;lt;/title&amp;gt;&lt;br /&gt;
  &amp;lt;color&amp;gt;black&amp;lt;/color&amp;gt;&lt;br /&gt;
  &amp;lt;size&amp;gt;200&amp;lt;/size&amp;gt;&lt;br /&gt;
  &amp;lt;uploadedFileContents&amp;gt;HYC116_NH3BH3_FREQ.LOG&amp;lt;/uploadedFileContents&amp;gt;&lt;br /&gt;
&amp;lt;/jmolApplet&amp;gt;&amp;lt;/jmol&amp;gt;&lt;br /&gt;
&lt;br /&gt;
===Association energy===&lt;br /&gt;
&lt;br /&gt;
E(BH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;) (using the optimisation with the correct symmetry) = -26.61532363 a.u. = &amp;lt;b&amp;gt;-26.61532 a.u. (5 d.p.)&amp;lt;/b&amp;gt;&lt;br /&gt;
&lt;br /&gt;
E(NH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;) = -56.55776873 a.u. = &amp;lt;b&amp;gt;-56.55777 a.u. (5 d.p.)&amp;lt;/b&amp;gt;&lt;br /&gt;
&lt;br /&gt;
E(NH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;BH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;) = -83.22468892 a.u. = &amp;lt;b&amp;gt;-83.22469 a.u. (5 d.p.)&amp;lt;/b&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
Carrying out calculations using numbers which has already been rounded up can possibly result in errors in the last digit. Hence, here the calculations were carried out using the numbers provided from the optimisations (i.e. with more decimal places than necessary); the answer was then rounded up to the desired accuracy. &lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
ΔE = E(NH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;BH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;)-[E(NH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;)+E(BH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;)]&lt;br /&gt;
&lt;br /&gt;
ΔE = -83.22468892 - (-56.55776873 + -26.61532363) = -0.05159656 a.u. &lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;ΔE = -0.05160 a.u. (5 d.p.)&amp;lt;/b&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Converting energy from a.u. to kJ/mol&#039;&#039;&#039;&lt;br /&gt;
An atomic unit for energy is Hartree, which is equal to 2625.5 kJ/mol.&lt;br /&gt;
&amp;lt;ref&amp;gt;https://cccbdb.nist.gov/hartree.asp (Accessed: 22.05.2018)&amp;lt;/ref&amp;gt;&lt;br /&gt;
 &lt;br /&gt;
&lt;br /&gt;
So ΔE in kJ/mol = -0.05159657 * 2625.5 = -135.46676828 kJ/mol&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;ΔE = -135 kJ/mol (nearest integer)&amp;lt;/b&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
The energy difference calculated above comes from the formation of the B-N dative bond. It is a relatively weak bond. According to a bond energy data sheet provided by the University of California,&amp;lt;ref&amp;gt;https://labs.chem.ucsb.edu/zakarian/armen/11---bonddissociationenergy.pdf (Accessed: 24.05.2018)&amp;lt;/ref&amp;gt;  the bond energy of the C-C bond of an ethane molecule is 368 kJ/mol. This is a fair comparison to the NH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;BH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt; molecule as the two molecules have the same structure, only with the carbon atoms on ethane swapped for Boron and Nitrogen in NH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;BH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;&lt;br /&gt;
&lt;br /&gt;
==Using a mixture of basis-sets and pseudo-potentials==&lt;br /&gt;
&lt;br /&gt;
===BBr&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;===&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;Calculation type&amp;lt;/b&amp;gt;: Optimisation&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;Calculation Method&amp;lt;/b&amp;gt;: B3LYP&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;Basis set&amp;lt;/b&amp;gt;: Boron: 6-31G(d,p) ; Br: LANL2DZ&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
Larger calculations are often sent to a web-server to run on a high-performance computer instead of a desktop. In order to experience and learn to use a web-server, the optimisation and the frequency analysis for BBr&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt; were both sent and done on a server instead of the desktop. The calculation results were downloaded from the web-server once they were finished.   &lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Summary table&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
[[file:Hyc116_bbr3_opt_summarytable.png]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Items table&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;pre&amp;gt;&lt;br /&gt;
Item               Value     Threshold  Converged?&lt;br /&gt;
 Maximum Force            0.000008     0.000450     YES&lt;br /&gt;
 RMS     Force            0.000005     0.000300     YES&lt;br /&gt;
 Maximum Displacement     0.000036     0.001800     YES&lt;br /&gt;
 RMS     Displacement     0.000023     0.001200     YES&lt;br /&gt;
&amp;lt;/pre&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Frequency log file&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
[[Media:Hyc116_bbr3_freq.log]]&lt;br /&gt;
&lt;br /&gt;
Attached above is the frequency file saved onto the computer from the SCAN server portal. The frequency file was also published on the chemistry database DSpace. {{DOI|10042/202442}}&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Frequencies&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;pre&amp;gt;&lt;br /&gt;
Low frequencies ---   -0.0137   -0.0064   -0.0046    2.4315    2.4315    4.8421&lt;br /&gt;
Low frequencies ---  155.9631  155.9651  267.7052&lt;br /&gt;
&amp;lt;/pre&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;jmol of BBr&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;&#039;&#039;&#039;&lt;br /&gt;
&amp;lt;jmol&amp;gt;&amp;lt;jmolApplet&amp;gt;&lt;br /&gt;
  &amp;lt;title&amp;gt;optimised BBr3&amp;lt;/title&amp;gt;&lt;br /&gt;
  &amp;lt;color&amp;gt;black&amp;lt;/color&amp;gt;&lt;br /&gt;
  &amp;lt;size&amp;gt;200&amp;lt;/size&amp;gt;&lt;br /&gt;
  &amp;lt;uploadedFileContents&amp;gt;Hyc116_bbr3_freq.log&amp;lt;/uploadedFileContents&amp;gt;&lt;br /&gt;
&amp;lt;/jmolApplet&amp;gt;&amp;lt;/jmol&amp;gt;&lt;br /&gt;
&lt;br /&gt;
==Aromaticity==&lt;br /&gt;
&lt;br /&gt;
===Benzene===&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;Calculation type&amp;lt;/b&amp;gt;: Optimisation&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;Calculation Method&amp;lt;/b&amp;gt;: B3LYP&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;Basis set&amp;lt;/b&amp;gt;: 6-31G(d,p) &lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Summary table&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
[[file:Hyc116_c6h6_summarytable.png]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Items table&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;pre&amp;gt;&lt;br /&gt;
Item               Value     Threshold  Converged?&lt;br /&gt;
 Maximum Force            0.000193     0.000450     YES&lt;br /&gt;
 RMS     Force            0.000079     0.000300     YES&lt;br /&gt;
 Maximum Displacement     0.000830     0.001800     YES&lt;br /&gt;
 RMS     Displacement     0.000294     0.001200     YES&lt;br /&gt;
&amp;lt;/pre&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Frequency log file&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
[[Media:HYC116_C6H6_FREQ.LOG]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Frequencies&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;pre&amp;gt;&lt;br /&gt;
Low frequencies ---   -3.5606   -3.5606   -0.0089   -0.0043   -0.0043   10.0905&lt;br /&gt;
Low frequencies ---  413.9582  413.9582  621.1416&lt;br /&gt;
&amp;lt;/pre&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;jmol of C&amp;lt;sub&amp;gt;6&amp;lt;/sub&amp;gt;H&amp;lt;sub&amp;gt;6&amp;lt;/sub&amp;gt;&#039;&#039;&#039;&lt;br /&gt;
&amp;lt;jmol&amp;gt;&amp;lt;jmolApplet&amp;gt;&lt;br /&gt;
  &amp;lt;title&amp;gt;optimised Benzene&amp;lt;/title&amp;gt;&lt;br /&gt;
  &amp;lt;color&amp;gt;black&amp;lt;/color&amp;gt;&lt;br /&gt;
  &amp;lt;size&amp;gt;200&amp;lt;/size&amp;gt;&lt;br /&gt;
  &amp;lt;uploadedFileContents&amp;gt;HYC116_C6H6_FREQ.LOG&amp;lt;/uploadedFileContents&amp;gt;&lt;br /&gt;
&amp;lt;/jmolApplet&amp;gt;&amp;lt;/jmol&amp;gt;&lt;br /&gt;
&lt;br /&gt;
===Borazine===&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;Calculation type&amp;lt;/b&amp;gt;: Optimisation&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;Calculation Method&amp;lt;/b&amp;gt;: B3LYP&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;Basis set&amp;lt;/b&amp;gt;: 6-31G(d,p) &lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Summary table&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
[[file:Hyc116_borazine_summarytable.png]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Items table&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;pre&amp;gt;&lt;br /&gt;
Item               Value     Threshold  Converged?&lt;br /&gt;
 Maximum Force            0.000085     0.000450     YES&lt;br /&gt;
 RMS     Force            0.000033     0.000300     YES&lt;br /&gt;
 Maximum Displacement     0.000250     0.001800     YES&lt;br /&gt;
 RMS     Displacement     0.000074     0.001200     YES&lt;br /&gt;
&amp;lt;/pre&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Frequency log file&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
[[Media:HYC116_BORAZINE_FREQ.LOG]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Frequencies&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;pre&amp;gt;&lt;br /&gt;
Low frequencies ---  -12.6626  -12.6626   -8.9272   -0.0211   -0.0104   -0.0104&lt;br /&gt;
Low frequencies ---  289.1112  289.1112  403.8613&lt;br /&gt;
&amp;lt;/pre&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;jmol of Borazine&#039;&#039;&#039;&lt;br /&gt;
&amp;lt;jmol&amp;gt;&amp;lt;jmolApplet&amp;gt;&lt;br /&gt;
  &amp;lt;title&amp;gt;optimised Borazine&amp;lt;/title&amp;gt;&lt;br /&gt;
  &amp;lt;color&amp;gt;black&amp;lt;/color&amp;gt;&lt;br /&gt;
  &amp;lt;size&amp;gt;200&amp;lt;/size&amp;gt;&lt;br /&gt;
  &amp;lt;uploadedFileContents&amp;gt;HYC116_BORAZINE_FREQ.LOG&amp;lt;/uploadedFileContents&amp;gt;&lt;br /&gt;
&amp;lt;/jmolApplet&amp;gt;&amp;lt;/jmol&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
===Charge distribution===&lt;br /&gt;
&lt;br /&gt;
An NBO charge analysis was carried out on both the optimised benzene and borazine. Visualisations of the charge distribution are shown in the table below, with the colour range going from -1.102 to 1.102 for both molecule. This large scale was chosen as it allows direct comparison of the charge on any atoms in these two molecules and shows the relative magnitude of charges on all these atoms. Negative charges are shown in red, and positive charges are shown in green. A neutral charge is displayed in black, so the smaller a charge is (positive or negative), the darker its colour representation is. Larger charges are shown in brighter colours. The charges are also displayed on the atoms as numbers with a neutral charge being zero. Negative charges are shown as negative number and positive charges are shown as positive numbers. &lt;br /&gt;
&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot;&lt;br /&gt;
!&lt;br /&gt;
!Benzene&lt;br /&gt;
!Borazine&lt;br /&gt;
|-&lt;br /&gt;
!Visualisation of charge distribution&lt;br /&gt;
|[[File:Hyc116_benzene_charge_distribution1.png|500x500px|thumb|centre|Charge distribution of Benzene visualisation]]&lt;br /&gt;
|[[File:Hyc116_borazine_charge_distribution1.png|500x500px|thumb|centre|Charge distribution of Borazine visualisation]]&lt;br /&gt;
|-&lt;br /&gt;
!Charge &lt;br /&gt;
|Carbon: -0.239&lt;br /&gt;
&lt;br /&gt;
Hydrogen: 0.239&lt;br /&gt;
|Nitrogen: -1.102 &lt;br /&gt;
&lt;br /&gt;
Boron: 0.747&lt;br /&gt;
&lt;br /&gt;
Hydrogen (bonded to N): 0.432&lt;br /&gt;
&lt;br /&gt;
Hydrogen (bonded to B): -0.077&lt;br /&gt;
|-&lt;br /&gt;
!Discussion&lt;br /&gt;
|From the visualisation, it is shown that there is a slightly negative charge on the carbon atoms, and a positive charge of the same magnitude on the hydrogen atoms. All the carbon atoms have the same charge as they are in identical environments. The same applies to all the hydrogen atoms. This is due to the highly symmetrical structure of benzene. Since the same colour scale was used for both benzene and borazine, and the charges are much smaller in magnitude on atoms in benzene than atoms on borazine, the colours on the charge distribution visualisation is much darker. &lt;br /&gt;
|Polar bonds between nitrogen and boron are demonstration from the above visualisation. From the colours displayed on the charge distribution visualisation as well as the charge values, it is shown that nitrogen has a relatively large negative charge, while boron has a positive charge. This is due to the difference in electrogenativity between these atoms: nitrogen atoms are more electronegative than boron and tends to attract electrons towards themselves. It is worth noting that the hydrogen atoms do not all have the same charge. The hydrogen atoms bonded to boron have a slightly negative charge, and the ones bonded to nitrogen have a small positive charge. &lt;br /&gt;
&lt;br /&gt;
The fact that the same colour scale was used for both molecules comes in helpful here. It allows the charges on atoms to be compared directly. For example, just from looking at the colours, one can tell that or example, even though both carbon and nitrogen are electronegative, nitrogen is much more electronegative, which is quantitatively shown by Pauling&#039;s electronegativity scale.&amp;lt;ref&amp;gt;http://www.tutor-homework.com/Chemistry_Help/electronegativity_table/electronegativity.html (Accessed: 24.0502018&amp;lt;/ref&amp;gt;&lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
===Comparative MOs of Benzene and Borazine===&lt;br /&gt;
&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot;&lt;br /&gt;
!&lt;br /&gt;
!Benzene&lt;br /&gt;
!Borazine&lt;br /&gt;
!Comparison and Discussion&lt;br /&gt;
|-&lt;br /&gt;
!1st comparative pair&lt;br /&gt;
|[[File:Hyc116_benzene_1st_MO_pair_7.png|200x200px|centre]]&lt;br /&gt;
|[[File:Hyc116_borazine_1st_MO_pair_level9.png|200x200px|centre]]&lt;br /&gt;
|MO 9 of both benzene and borazine are comparable. They both show delocalised molecular orbital with an overall bonding character. There is a nodal plane across the molecular orbitals for both benzene and borazine. For benzene, there is contribution from all the carbon and hydrogen s orbitals. Moreover, the molecular orbitals are symmetric to their counterpart of opposite phase, giving an E&amp;lt;sub&amp;gt;1g&amp;lt;/sub&amp;gt; MO. That is not the case for borazine; they are less symmetric in borazine. This MO of borazine has an E&#039; symmetry. Nitrogen atoms are more electronegative than boron atoms and pull electron density towards themselves, resulting in a larger lobe. There is contribution from all the boron and nitrogen s orbitals, and three of the hydrogen s orbitals, though not all of them. &lt;br /&gt;
|-&lt;br /&gt;
!2nd comparative pair&lt;br /&gt;
|[[File:Hyc116_benzene_2nd_MO_pair_10.png|200x200px|centre]]&lt;br /&gt;
|[[File:Hyc116_borazine_2nd_MO_pair_level11.png|200x200px|centre]]&lt;br /&gt;
|MO 10 of benzene and MO 11 of borazine are comparable. Here shows a pair of rather delocalised molecular orbitals with slightly more antibonding character than the first pair shown above. On both MOs, there is no contribution from one pair of opposite hydrogen atoms, but contribution from s orbitals of all other atoms on both molecule. The benzene MO has an E&amp;lt;sub&amp;gt;2g&amp;lt;/sub&amp;gt; symmetry. In borazine, the lobes are in different sizes due to the higher electronegativity of nitrogen. The lobes at the nitrogen atoms are larger as they attract electrons towards themselves more so than boron atoms do. This borazine MO has an E&#039; symmetry. &lt;br /&gt;
|-&lt;br /&gt;
!3rd comparative pair&lt;br /&gt;
|[[File:Hyc116_benzene_3rd_MO_pair_21.png|200x200px|centre]]&lt;br /&gt;
|[[File:Hyc116_borazine_3rd_MO_pair_level21.png|200x200px|centre]]&lt;br /&gt;
|The HOMO (MO 21) of benzene and the HOMO (MO 21) of borazine are comparable. They are both made of p orbitals of all carbon atoms (or all boron and nitrogen atoms in the case of borazine); there is no contribution from hydrogen atoms as they do not have p orbitals. There is a nodal plan perpendicular to the z axis (highest rotational axis) and one parallel to the z axis. On benzene, the MO is very symmetric and has an E&amp;lt;sub&amp;gt;1g&amp;lt;/sub&amp;gt; symmetry; the lobes of the MO are the same in size. On borazine, the lobe where there are two nitrogen atoms is bigger in size, again due to the higher electronegtivity of nitrogen compared to boron. The borazine MO has an E&#039; &#039; symmetry.&lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
===Aromaticity: some theories===&lt;br /&gt;
&lt;br /&gt;
Aromatic compounds display properties such as their high stability and bond lengths between typical single and double bonds. A simple understanding of aromaticity involves the overlap of p orbitals perpendicular to the cyclic plane; the delocalisation of electrons on the pi system is identified to be responsible of the stability of aromatic systems. Aromatic compounds can be identified by the Huckel’s rule, which states that conjugated planar cyclic molecules with (4n +2) π electrons are aromatic. Both benzene and borazine obey the Huckel’s rule and fit the conventional description of aromaticity. &lt;br /&gt;
&lt;br /&gt;
However, it is proved in recent years that the conventional criteria do not necessarily have to be obeyed for a compound to be aromatic. For instance, there has been shown that some non-planar compounds display aromaticity. This suggests that the criteria for aromaticity is not simply structural, and these advances give rise to concepts such as quasiaromaticity and pseudoaromaticity. Recent advances show that there are quantum mechanics basis on the idea of aromaticity. &lt;br /&gt;
In conclusion, while the overlap of pi orbitals provides a simple understanding for aromaticity, it is not a sufficient description for aromaticity.&lt;br /&gt;
&lt;br /&gt;
==References==&lt;br /&gt;
{{reflist}}&lt;/div&gt;</summary>
		<author><name>Hyc116</name></author>
	</entry>
	<entry>
		<id>https://chemwiki.ch.ic.ac.uk/index.php?title=MO_hyc116&amp;diff=732317</id>
		<title>MO hyc116</title>
		<link rel="alternate" type="text/html" href="https://chemwiki.ch.ic.ac.uk/index.php?title=MO_hyc116&amp;diff=732317"/>
		<updated>2018-05-25T14:56:19Z</updated>

		<summary type="html">&lt;p&gt;Hyc116: /* Using a mixture of basis-sets and pseudo-potentials */&lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;==BH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;==&lt;br /&gt;
&lt;br /&gt;
===standard information===&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;Calculation type&amp;lt;/b&amp;gt;: Optimisation&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;Calculation Method&amp;lt;/b&amp;gt;: B3LYP&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;Basis set&amp;lt;/b&amp;gt;: 6-31G(d,p) &lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Summary table&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
[[file:Hyc116_bh3_631g_opt_summarytable.png]]&lt;br /&gt;
&lt;br /&gt;
The above summary table was obtained after the 2nd optimisation of BH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt; (after the initial optimisation using the 3-21G basis set). Notice how the symmetry is incorrect and shown as Cs. This is because the symmetry was manually broken at the beginning by changing the bond length of B-H bonds. The point group was manually adjusted and the molecule was optimised again before the frequency analysis and the new summary table is attached below.&lt;br /&gt;
&lt;br /&gt;
[[file:Hyc116_bh3_correctsummarytable.png]]&lt;br /&gt;
&lt;br /&gt;
The above summary table was obtained from the optimisation after adjusting the symmetry. The point shown in this summary table is D&amp;lt;sub&amp;gt;3h&amp;lt;/sub&amp;gt;, which is the correct for BH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;. &lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Items table&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
Below is the items table taken from the optimisation with the correct point group.&lt;br /&gt;
&lt;br /&gt;
&amp;lt;pre&amp;gt;&lt;br /&gt;
Item               Value     Threshold  Converged?&lt;br /&gt;
 Maximum Force            0.000015     0.000450     YES&lt;br /&gt;
 RMS     Force            0.000010     0.000300     YES&lt;br /&gt;
 Maximum Displacement     0.000058     0.001800     YES&lt;br /&gt;
 RMS     Displacement     0.000038     0.001200     YES&lt;br /&gt;
&amp;lt;/pre&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Frequency log file&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
[[Media:HYC116 BH3 FREQ.LOG]] &lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Frequencies&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;pre&amp;gt;&lt;br /&gt;
Low frequencies ---  -10.3498   -3.4492   -1.2454   -0.0055    0.4779    3.2165&lt;br /&gt;
Low frequencies --- 1162.9519 1213.1527 1213.1554&lt;br /&gt;
&amp;lt;/pre&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;jmol of BH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;&#039;&#039;&#039;&lt;br /&gt;
&amp;lt;jmol&amp;gt;&amp;lt;jmolApplet&amp;gt;&lt;br /&gt;
  &amp;lt;title&amp;gt;optimised BH3&amp;lt;/title&amp;gt;&lt;br /&gt;
  &amp;lt;color&amp;gt;black&amp;lt;/color&amp;gt;&lt;br /&gt;
  &amp;lt;size&amp;gt;200&amp;lt;/size&amp;gt;&lt;br /&gt;
  &amp;lt;uploadedFileContents&amp;gt;HYC116_BH3_FREQ.LOG&amp;lt;/uploadedFileContents&amp;gt;&lt;br /&gt;
&amp;lt;/jmolApplet&amp;gt;&amp;lt;/jmol&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
===Vibrational spectrum===&lt;br /&gt;
&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot;&lt;br /&gt;
!wavenumber (cm&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;)&lt;br /&gt;
!Intensity (arbitrary units)&lt;br /&gt;
!symmetry&lt;br /&gt;
!IR active?&lt;br /&gt;
!type&lt;br /&gt;
|-&lt;br /&gt;
|1163&lt;br /&gt;
|93&lt;br /&gt;
|A&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;&#039; &#039;&lt;br /&gt;
|Yes&lt;br /&gt;
|Out of plane bend&lt;br /&gt;
|-&lt;br /&gt;
|1213&lt;br /&gt;
|14&lt;br /&gt;
|E&#039;&lt;br /&gt;
|Very slight&lt;br /&gt;
|Bend&lt;br /&gt;
|-&lt;br /&gt;
|1213&lt;br /&gt;
|14&lt;br /&gt;
|E&#039;&lt;br /&gt;
|Very slight&lt;br /&gt;
|Bend&lt;br /&gt;
|-&lt;br /&gt;
|2582&lt;br /&gt;
|0&lt;br /&gt;
|A&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;&#039;&lt;br /&gt;
|No&lt;br /&gt;
|Symmetric stretch&lt;br /&gt;
|-&lt;br /&gt;
|2716&lt;br /&gt;
|126&lt;br /&gt;
|E&#039;&lt;br /&gt;
|Yes&lt;br /&gt;
|Asymmetric stretch&lt;br /&gt;
|-&lt;br /&gt;
|2716&lt;br /&gt;
|126&lt;br /&gt;
|E&#039;&lt;br /&gt;
|Yes&lt;br /&gt;
|Asymmetric stretch&lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;IR spectrum&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
[[file:Hyc116_ir_bh3.png|400*600]]&lt;br /&gt;
&lt;br /&gt;
There are only three peaks on the IR spectrum of BH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;, despite that there are 6 vibrational modes for the molecule. As shown in the table above, the symmetric stretching mode with A1 symmetry at 2582 cm&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt; is not IR active; naturally, that vibrational mode doesn’t give a peak on the IR spectrum. As shown from the table, two pairs of vibrational modes, the bond angle deformation/bend at 1213 cm&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt; and the asymmetric bond stretch at 2716 cm&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;, are degenerate with the symmetry label E. This means that they have the same energy, and hence give the same wavenumber on the IR spectrum. Each pair of degenerate vibrational modes give rise to one peak. This leaves three peaks, as confirmed by the IR spectrum above.&lt;br /&gt;
&lt;br /&gt;
===Molecular orbitals of BH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;===&lt;br /&gt;
&lt;br /&gt;
[[file:hyc116_bh3_MO_diagram.png]]&lt;br /&gt;
&lt;br /&gt;
The above molecular orbital diagram was taken from Dr Patricia Hunt&#039;s &amp;lt;i&amp;gt;Lecture 4 Tutorial Problem Model Answers&amp;lt;/i&amp;gt;.&amp;lt;ref&amp;gt;P. Hunt, &amp;quot;Lecture 4 Tutorial Problem Model Answers&amp;quot;, 2 (2018)&amp;lt;/ref&amp;gt; Diagrams of the &amp;quot;real&amp;quot; MOs were obtained from Gaussian.&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
There is no significant difference between the LCAO MOs and the real ones. Features such as orbital phases are shown clearly on both the LCAO MOs and the real MOs, illustrating the bonding/anti-bonding characters of the molecular orbitals. This suggests that the the qualitative MO theory is highly accurate and useful when studying the molecular orbitals of molecules.&lt;br /&gt;
&lt;br /&gt;
==Associated energies: ammonium borane==&lt;br /&gt;
&lt;br /&gt;
===NH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;===&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;Calculation type&amp;lt;/b&amp;gt;: Optimisation&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;Calculation Method&amp;lt;/b&amp;gt;: B3LYP&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;Basis set&amp;lt;/b&amp;gt;: 6-31G(d,p) &lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Summary table&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
[[file:Hyc116_nh3_631g_summarytable.png]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Items table&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;pre&amp;gt;&lt;br /&gt;
Item               Value     Threshold  Converged?&lt;br /&gt;
 Maximum Force            0.000006     0.000450     YES&lt;br /&gt;
 RMS     Force            0.000004     0.000300     YES&lt;br /&gt;
 Maximum Displacement     0.000012     0.001800     YES&lt;br /&gt;
 RMS     Displacement     0.000008     0.001200     YES&lt;br /&gt;
&amp;lt;/pre&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Frequency log file&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
[[Media:HYC116_NH3_FREQ.LOG]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Frequencies&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;pre&amp;gt;&lt;br /&gt;
Low frequencies ---   -8.5646   -8.5588   -0.0047    0.0454    0.1784   26.4183&lt;br /&gt;
Low frequencies --- 1089.7603 1694.1865 1694.1865&lt;br /&gt;
&amp;lt;/pre&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;jmol of NH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;&#039;&#039;&#039;&lt;br /&gt;
&amp;lt;jmol&amp;gt;&amp;lt;jmolApplet&amp;gt;&lt;br /&gt;
  &amp;lt;title&amp;gt;optimised NH3&amp;lt;/title&amp;gt;&lt;br /&gt;
  &amp;lt;color&amp;gt;black&amp;lt;/color&amp;gt;&lt;br /&gt;
  &amp;lt;size&amp;gt;200&amp;lt;/size&amp;gt;&lt;br /&gt;
  &amp;lt;uploadedFileContents&amp;gt;HYC116_NH3_FREQ.LOG&amp;lt;/uploadedFileContents&amp;gt;&lt;br /&gt;
&amp;lt;/jmolApplet&amp;gt;&amp;lt;/jmol&amp;gt;&lt;br /&gt;
&lt;br /&gt;
===NH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;BH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;===&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;Calculation type&amp;lt;/b&amp;gt;: Optimisation&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;Calculation Method&amp;lt;/b&amp;gt;: B3LYP&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;Basis set&amp;lt;/b&amp;gt;: 6-31G(d,p) &lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Summary table&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
[[file:Hyc116_nh3bh3_631g_summarytable1.png]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Items table&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;pre&amp;gt;&lt;br /&gt;
Item               Value     Threshold  Converged?&lt;br /&gt;
 Maximum Force            0.000121     0.000450     YES&lt;br /&gt;
 RMS     Force            0.000057     0.000300     YES&lt;br /&gt;
 Maximum Displacement     0.000501     0.001800     YES&lt;br /&gt;
 RMS     Displacement     0.000293     0.001200     YES&lt;br /&gt;
&amp;lt;/pre&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Frequency log file&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
[[Media:HYC116_NH3BH3_FREQ1.LOG]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Frequencies&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;pre&amp;gt;&lt;br /&gt;
Low frequencies ---   -0.0574   -0.0501   -0.0074   21.6276   21.6377   40.3839&lt;br /&gt;
Low frequencies ---  265.9973  632.3725  640.1275&lt;br /&gt;
&amp;lt;/pre&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;jmol of NH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;BH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;&#039;&#039;&#039;&lt;br /&gt;
&amp;lt;jmol&amp;gt;&amp;lt;jmolApplet&amp;gt;&lt;br /&gt;
  &amp;lt;title&amp;gt;optimised NH3BH3&amp;lt;/title&amp;gt;&lt;br /&gt;
  &amp;lt;color&amp;gt;black&amp;lt;/color&amp;gt;&lt;br /&gt;
  &amp;lt;size&amp;gt;200&amp;lt;/size&amp;gt;&lt;br /&gt;
  &amp;lt;uploadedFileContents&amp;gt;HYC116_NH3BH3_FREQ.LOG&amp;lt;/uploadedFileContents&amp;gt;&lt;br /&gt;
&amp;lt;/jmolApplet&amp;gt;&amp;lt;/jmol&amp;gt;&lt;br /&gt;
&lt;br /&gt;
===Association energy===&lt;br /&gt;
&lt;br /&gt;
E(BH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;) (using the optimisation with the correct symmetry) = -26.61532363 a.u. = &amp;lt;b&amp;gt;-26.61532 a.u. (5 d.p.)&amp;lt;/b&amp;gt;&lt;br /&gt;
&lt;br /&gt;
E(NH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;) = -56.55776873 a.u. = &amp;lt;b&amp;gt;-56.55777 a.u. (5 d.p.)&amp;lt;/b&amp;gt;&lt;br /&gt;
&lt;br /&gt;
E(NH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;BH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;) = -83.22468892 a.u. = &amp;lt;b&amp;gt;-83.22469 a.u. (5 d.p.)&amp;lt;/b&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
Carrying out calculations using numbers which has already been rounded up can possibly result in errors in the last digit. Hence, here the calculations were carried out using the numbers provided from the optimisations (i.e. with more decimal places than necessary); the answer was then rounded up to the desired accuracy. &lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
ΔE = E(NH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;BH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;)-[E(NH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;)+E(BH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;)]&lt;br /&gt;
&lt;br /&gt;
ΔE = -83.22468892 - (-56.55776873 + -26.61532363) = -0.05159656 a.u. &lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;ΔE = -0.05160 a.u. (5 d.p.)&amp;lt;/b&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Converting energy from a.u. to kJ/mol&#039;&#039;&#039;&lt;br /&gt;
An atomic unit for energy is Hartree, which is equal to 2625.5 kJ/mol.&lt;br /&gt;
&amp;lt;ref&amp;gt;https://cccbdb.nist.gov/hartree.asp (Accessed: 22.05.2018)&amp;lt;/ref&amp;gt;&lt;br /&gt;
 &lt;br /&gt;
&lt;br /&gt;
So ΔE in kJ/mol = -0.05159657 * 2625.5 = -135.46676828 kJ/mol&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;ΔE = -135 kJ/mol (nearest integer)&amp;lt;/b&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
The energy difference calculated above comes from the formation of the B-N dative bond. It is a relatively weak bond. According to a bond energy data sheet provided by the University of California,&amp;lt;ref&amp;gt;https://labs.chem.ucsb.edu/zakarian/armen/11---bonddissociationenergy.pdf (Accessed: 24.05.2018)&amp;lt;/ref&amp;gt;  the bond energy of the C-C bond of an ethane molecule is 368 kJ/mol. This is a fair comparison to the NH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;BH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt; molecule as the two molecules have the same structure, only with the carbon atoms on ethane swapped for Boron and Nitrogen in NH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;BH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;&lt;br /&gt;
&lt;br /&gt;
==Using a mixture of basis-sets and pseudo-potentials==&lt;br /&gt;
&lt;br /&gt;
===BBr&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;===&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;Calculation type&amp;lt;/b&amp;gt;: Optimisation&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;Calculation Method&amp;lt;/b&amp;gt;: B3LYP&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;Basis set&amp;lt;/b&amp;gt;: Boron: 6-31G(d,p) ; Br: LANL2DZ&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
Larger calculations are often sent to a web-server to run on a high-performance computer instead of a desktop. In order to experience and learn to use a web-server, the optimisation and the frequency analysis for BBr&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt; were both sent and done on a server instead of the desktop. The calculation results were downloaded from the web-server once they were finished.   &lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Summary table&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
[[file:Hyc116_bbr3_opt_summarytable.png]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Items table&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;pre&amp;gt;&lt;br /&gt;
Item               Value     Threshold  Converged?&lt;br /&gt;
 Maximum Force            0.000008     0.000450     YES&lt;br /&gt;
 RMS     Force            0.000005     0.000300     YES&lt;br /&gt;
 Maximum Displacement     0.000036     0.001800     YES&lt;br /&gt;
 RMS     Displacement     0.000023     0.001200     YES&lt;br /&gt;
&amp;lt;/pre&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Frequency log file&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
[[Media:Hyc116_bbr3_freq.log]]&lt;br /&gt;
&lt;br /&gt;
Attached above is the frequency file saved onto the computer from the SCAN server portal. The frequency file was also published on the chemistry database DSpace. {{DOI|10042/202442}}&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Frequencies&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;pre&amp;gt;&lt;br /&gt;
Low frequencies ---   -0.0137   -0.0064   -0.0046    2.4315    2.4315    4.8421&lt;br /&gt;
Low frequencies ---  155.9631  155.9651  267.7052&lt;br /&gt;
&amp;lt;/pre&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;jmol of BBr&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;&#039;&#039;&#039;&lt;br /&gt;
&amp;lt;jmol&amp;gt;&amp;lt;jmolApplet&amp;gt;&lt;br /&gt;
  &amp;lt;title&amp;gt;optimised BBr3&amp;lt;/title&amp;gt;&lt;br /&gt;
  &amp;lt;color&amp;gt;black&amp;lt;/color&amp;gt;&lt;br /&gt;
  &amp;lt;size&amp;gt;200&amp;lt;/size&amp;gt;&lt;br /&gt;
  &amp;lt;uploadedFileContents&amp;gt;Hyc116_bbr3_freq.log&amp;lt;/uploadedFileContents&amp;gt;&lt;br /&gt;
&amp;lt;/jmolApplet&amp;gt;&amp;lt;/jmol&amp;gt;&lt;br /&gt;
&lt;br /&gt;
==Aromaticity==&lt;br /&gt;
&lt;br /&gt;
===Benzene===&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;Calculation type&amp;lt;/b&amp;gt;: Optimisation&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;Calculation Method&amp;lt;/b&amp;gt;: B3LYP&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;Basis set&amp;lt;/b&amp;gt;: 6-31G(d,p) &lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Summary table&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
[[file:Hyc116_c6h6_summarytable.png]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Items table&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;pre&amp;gt;&lt;br /&gt;
Item               Value     Threshold  Converged?&lt;br /&gt;
 Maximum Force            0.000193     0.000450     YES&lt;br /&gt;
 RMS     Force            0.000079     0.000300     YES&lt;br /&gt;
 Maximum Displacement     0.000830     0.001800     YES&lt;br /&gt;
 RMS     Displacement     0.000294     0.001200     YES&lt;br /&gt;
&amp;lt;/pre&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Frequency log file&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
[[Media:HYC116_C6H6_FREQ.LOG]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Frequencies&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;pre&amp;gt;&lt;br /&gt;
Low frequencies ---   -3.5606   -3.5606   -0.0089   -0.0043   -0.0043   10.0905&lt;br /&gt;
Low frequencies ---  413.9582  413.9582  621.1416&lt;br /&gt;
&amp;lt;/pre&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;jmol of C&amp;lt;sub&amp;gt;6&amp;lt;/sub&amp;gt;H&amp;lt;sub&amp;gt;6&amp;lt;/sub&amp;gt;&#039;&#039;&#039;&lt;br /&gt;
&amp;lt;jmol&amp;gt;&amp;lt;jmolApplet&amp;gt;&lt;br /&gt;
  &amp;lt;title&amp;gt;optimised Benzene&amp;lt;/title&amp;gt;&lt;br /&gt;
  &amp;lt;color&amp;gt;black&amp;lt;/color&amp;gt;&lt;br /&gt;
  &amp;lt;size&amp;gt;200&amp;lt;/size&amp;gt;&lt;br /&gt;
  &amp;lt;uploadedFileContents&amp;gt;HYC116_C6H6_FREQ.LOG&amp;lt;/uploadedFileContents&amp;gt;&lt;br /&gt;
&amp;lt;/jmolApplet&amp;gt;&amp;lt;/jmol&amp;gt;&lt;br /&gt;
&lt;br /&gt;
===Borazine===&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;Calculation type&amp;lt;/b&amp;gt;: Optimisation&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;Calculation Method&amp;lt;/b&amp;gt;: B3LYP&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;Basis set&amp;lt;/b&amp;gt;: 6-31G(d,p) &lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Summary table&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
[[file:Hyc116_borazine_summarytable.png]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Items table&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;pre&amp;gt;&lt;br /&gt;
Item               Value     Threshold  Converged?&lt;br /&gt;
 Maximum Force            0.000085     0.000450     YES&lt;br /&gt;
 RMS     Force            0.000033     0.000300     YES&lt;br /&gt;
 Maximum Displacement     0.000250     0.001800     YES&lt;br /&gt;
 RMS     Displacement     0.000074     0.001200     YES&lt;br /&gt;
&amp;lt;/pre&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Frequency log file&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
[[Media:HYC116_BORAZINE_FREQ.LOG]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Frequencies&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;pre&amp;gt;&lt;br /&gt;
Low frequencies ---  -12.6626  -12.6626   -8.9272   -0.0211   -0.0104   -0.0104&lt;br /&gt;
Low frequencies ---  289.1112  289.1112  403.8613&lt;br /&gt;
&amp;lt;/pre&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;jmol of Borazine&#039;&#039;&#039;&lt;br /&gt;
&amp;lt;jmol&amp;gt;&amp;lt;jmolApplet&amp;gt;&lt;br /&gt;
  &amp;lt;title&amp;gt;optimised Borazine&amp;lt;/title&amp;gt;&lt;br /&gt;
  &amp;lt;color&amp;gt;black&amp;lt;/color&amp;gt;&lt;br /&gt;
  &amp;lt;size&amp;gt;200&amp;lt;/size&amp;gt;&lt;br /&gt;
  &amp;lt;uploadedFileContents&amp;gt;HYC116_BORAZINE_FREQ.LOG&amp;lt;/uploadedFileContents&amp;gt;&lt;br /&gt;
&amp;lt;/jmolApplet&amp;gt;&amp;lt;/jmol&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
===Charge distribution===&lt;br /&gt;
&lt;br /&gt;
An NBO charge analysis was carried out on both the optimised benzene and borazine. Visualisations of the charge distribution are shown in the table below, with the colour range going from -1.102 to 1.102 for both molecule. This large scale was chosen as it allows direct comparison of the charge on any atoms in these two molecules and shows the relative magnitude of charges on all these atoms. Negative charges are shown in red, and positive charges are shown in green. A neutral charge is displayed in black, so the smaller a charge is (positive or negative), the darker its colour representation is. Larger charges are shown in brighter colours. The charges are also displayed on the atoms as numbers with a neutral charge being zero. Negative charges are shown as negative number and positive charges are shown as positive numbers. &lt;br /&gt;
&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot;&lt;br /&gt;
!&lt;br /&gt;
!Benzene&lt;br /&gt;
!Borazine&lt;br /&gt;
|-&lt;br /&gt;
!Visualisation of charge distribution&lt;br /&gt;
|[[File:Hyc116_benzene_charge_distribution1.png|500x500px|thumb|centre|Charge distribution of Benzene visualisation]]&lt;br /&gt;
|[[File:Hyc116_borazine_charge_distribution1.png|500x500px|thumb|centre|Charge distribution of Borazine visualisation]]&lt;br /&gt;
|-&lt;br /&gt;
!Charge &lt;br /&gt;
|Carbon: -0.239&lt;br /&gt;
&lt;br /&gt;
Hydrogen: 0.239&lt;br /&gt;
|Nitrogen: -1.102 &lt;br /&gt;
&lt;br /&gt;
Boron: 0.747&lt;br /&gt;
&lt;br /&gt;
Hydrogen (bonded to N): 0.432&lt;br /&gt;
&lt;br /&gt;
Hydrogen (bonded to B): -0.077&lt;br /&gt;
|-&lt;br /&gt;
!Discussion&lt;br /&gt;
|From the visualisation, it is shown that there is a slightly negative charge on the carbon atoms, and a positive charge of the same magnitude on the hydrogen atoms. All the carbon atoms have the same charge as they are in identical environments. The same applies to all the hydrogen atoms. This is due to the highly symmetrical structure of benzene. Since the same colour scale was used for both benzene and borazine, and the charges are much smaller in magnitude on atoms in benzene than atoms on borazine, the colours on the charge distribution visualisation is much darker. &lt;br /&gt;
|Polar bonds between nitrogen and boron are demonstration from the above visualisation. From the colours displayed on the charge distribution visualisation as well as the charge values, it is shown that nitrogen has a relatively large negative charge, while boron has a positive charge. This is due to the difference in electrogenativity between these atoms: nitrogen atoms are more electronegative than boron and tends to attract electrons towards themselves. It is worth noting that the hydrogen atoms do not all have the same charge. The hydrogen atoms bonded to boron have a slightly negative charge, and the ones bonded to nitrogen have a small positive charge. &lt;br /&gt;
&lt;br /&gt;
The fact that the same colour scale was used for both molecules comes in helpful here. It allows the charges on atoms to be compared directly. For example, just from looking at the colours, one can tell that or example, even though both carbon and nitrogen are electronegative, nitrogen is much more electronegative, which is quantitatively shown by Pauling&#039;s electronegativity scale.&amp;lt;ref&amp;gt;http://www.tutor-homework.com/Chemistry_Help/electronegativity_table/electronegativity.html (Accessed: 24.0502018&amp;lt;/ref&amp;gt;&lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
===Comparative MOs of Benzene and Borazine===&lt;br /&gt;
&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot;&lt;br /&gt;
!&lt;br /&gt;
!Benzene&lt;br /&gt;
!Borazine&lt;br /&gt;
!Comparison and Discussion&lt;br /&gt;
|-&lt;br /&gt;
!1st comparative pair&lt;br /&gt;
|[[File:Hyc116_benzene_1st_MO_pair_7.png|200x200px|centre]]&lt;br /&gt;
|[[File:Hyc116_borazine_1st_MO_pair_level9.png|200x200px|centre]]&lt;br /&gt;
|MO 9 of both benzene and borazine are comparable. They both show delocalised molecular orbital with an overall bonding character. There is a nodal plane across the molecular orbitals for both benzene and borazine. For benzene, there is contribution from all the carbon and hydrogen s orbitals. Moreover, the molecular orbitals are symmetric to their counterpart of opposite phase, giving an E&amp;lt;sub&amp;gt;1g&amp;lt;/sub&amp;gt; MO. That is not the case for borazine; they are less symmetric in borazine. This MO of borazine has an E&#039; symmetry. Nitrogen atoms are more electronegative than boron atoms and pull electron density towards themselves, resulting in a larger lobe. There is contribution from all the boron and nitrogen s orbitals, and three of the hydrogen s orbitals, though not all of them. &lt;br /&gt;
|-&lt;br /&gt;
!2nd comparative pair&lt;br /&gt;
|[[File:Hyc116_benzene_2nd_MO_pair_10.png|200x200px|centre]]&lt;br /&gt;
|[[File:Hyc116_borazine_2nd_MO_pair_level11.png|200x200px|centre]]&lt;br /&gt;
|MO 10 of benzene and MO 11 of borazine are comparable. Here shows a pair of rather delocalised molecular orbitals with slightly more antibonding character than the first pair shown above. On both MOs, there is no contribution from one pair of opposite hydrogen atoms, but contribution from s orbitals of all other atoms on both molecule. The benzene MO has an E&amp;lt;sub&amp;gt;2g&amp;lt;/sub&amp;gt; symmetry. In borazine, the lobes are in different sizes due to the higher electronegativity of nitrogen. The lobes at the nitrogen atoms are larger as they attract electrons towards themselves more so than boron atoms do. This borazine MO has an E&#039; symmetry. &lt;br /&gt;
|-&lt;br /&gt;
!3rd comparative pair&lt;br /&gt;
|[[File:Hyc116_benzene_3rd_MO_pair_21.png|200x200px|centre]]&lt;br /&gt;
|[[File:Hyc116_borazine_3rd_MO_pair_level21.png|200x200px|centre]]&lt;br /&gt;
|The HOMO (MO 21) of benzene and the HOMO (MO 21) of borazine are comparable. They are both made of p orbitals of all carbon atoms (or all boron and nitrogen atoms in the case of borazine); there is no contribution from hydrogen atoms as they do not have p orbitals. There is a nodal plan perpendicular to the z axis (highest rotational axis) and one parallel to the z axis. On benzene, the MO is very symmetric and has an E&amp;lt;sub&amp;gt;1g&amp;lt;/sub&amp;gt; symmetry; the lobes of the MO are the same in size. On borazine, the lobe where there are two nitrogen atoms is bigger in size, again due to the higher electronegtivity of nitrogen compared to boron. The borazine MO has an E&#039; &#039; symmetry.&lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
===Aromaticity: some theories===&lt;br /&gt;
&lt;br /&gt;
Aromatic compounds display properties such as their high stability and bond lengths between typical single and double bonds. A simple understanding of aromaticity involves the overlap of p orbitals perpendicular to the cyclic plane; the delocalisation of electrons on the pi system is identified to be responsible of the stability of aromatic systems. Aromatic compounds can be identified by the Huckel’s rule, which states that conjugated planar cyclic molecules with (4n +2) π electrons are aromatic. Both benzene and borazine obey the Huckel’s rule and fit the conventional description of aromaticity. &lt;br /&gt;
&lt;br /&gt;
However, it is proved in recent years that the conventional criteria do not necessarily have to be obeyed for a compound to be aromatic. For instance, there has been shown that some non-planar compounds display aromaticity. This suggests that the criteria for aromaticity is not simply structural, and these advances give rise to concepts such as quasiaromaticity and pseudoaromaticity. Recent advances show that there are quantum mechanics basis on the idea of aromaticity. &lt;br /&gt;
In conclusion, while the overlap of pi orbitals provides a simple understanding for aromaticity, it is not a sufficient description for aromaticity.&lt;br /&gt;
&lt;br /&gt;
==References==&lt;br /&gt;
{{reflist}}&lt;/div&gt;</summary>
		<author><name>Hyc116</name></author>
	</entry>
	<entry>
		<id>https://chemwiki.ch.ic.ac.uk/index.php?title=MO_hyc116&amp;diff=732308</id>
		<title>MO hyc116</title>
		<link rel="alternate" type="text/html" href="https://chemwiki.ch.ic.ac.uk/index.php?title=MO_hyc116&amp;diff=732308"/>
		<updated>2018-05-25T14:55:32Z</updated>

		<summary type="html">&lt;p&gt;Hyc116: /* BH3 */&lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;==BH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;==&lt;br /&gt;
&lt;br /&gt;
===standard information===&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;Calculation type&amp;lt;/b&amp;gt;: Optimisation&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;Calculation Method&amp;lt;/b&amp;gt;: B3LYP&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;Basis set&amp;lt;/b&amp;gt;: 6-31G(d,p) &lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Summary table&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
[[file:Hyc116_bh3_631g_opt_summarytable.png]]&lt;br /&gt;
&lt;br /&gt;
The above summary table was obtained after the 2nd optimisation of BH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt; (after the initial optimisation using the 3-21G basis set). Notice how the symmetry is incorrect and shown as Cs. This is because the symmetry was manually broken at the beginning by changing the bond length of B-H bonds. The point group was manually adjusted and the molecule was optimised again before the frequency analysis and the new summary table is attached below.&lt;br /&gt;
&lt;br /&gt;
[[file:Hyc116_bh3_correctsummarytable.png]]&lt;br /&gt;
&lt;br /&gt;
The above summary table was obtained from the optimisation after adjusting the symmetry. The point shown in this summary table is D&amp;lt;sub&amp;gt;3h&amp;lt;/sub&amp;gt;, which is the correct for BH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;. &lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Items table&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
Below is the items table taken from the optimisation with the correct point group.&lt;br /&gt;
&lt;br /&gt;
&amp;lt;pre&amp;gt;&lt;br /&gt;
Item               Value     Threshold  Converged?&lt;br /&gt;
 Maximum Force            0.000015     0.000450     YES&lt;br /&gt;
 RMS     Force            0.000010     0.000300     YES&lt;br /&gt;
 Maximum Displacement     0.000058     0.001800     YES&lt;br /&gt;
 RMS     Displacement     0.000038     0.001200     YES&lt;br /&gt;
&amp;lt;/pre&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Frequency log file&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
[[Media:HYC116 BH3 FREQ.LOG]] &lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Frequencies&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;pre&amp;gt;&lt;br /&gt;
Low frequencies ---  -10.3498   -3.4492   -1.2454   -0.0055    0.4779    3.2165&lt;br /&gt;
Low frequencies --- 1162.9519 1213.1527 1213.1554&lt;br /&gt;
&amp;lt;/pre&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;jmol of BH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;&#039;&#039;&#039;&lt;br /&gt;
&amp;lt;jmol&amp;gt;&amp;lt;jmolApplet&amp;gt;&lt;br /&gt;
  &amp;lt;title&amp;gt;optimised BH3&amp;lt;/title&amp;gt;&lt;br /&gt;
  &amp;lt;color&amp;gt;black&amp;lt;/color&amp;gt;&lt;br /&gt;
  &amp;lt;size&amp;gt;200&amp;lt;/size&amp;gt;&lt;br /&gt;
  &amp;lt;uploadedFileContents&amp;gt;HYC116_BH3_FREQ.LOG&amp;lt;/uploadedFileContents&amp;gt;&lt;br /&gt;
&amp;lt;/jmolApplet&amp;gt;&amp;lt;/jmol&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
===Vibrational spectrum===&lt;br /&gt;
&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot;&lt;br /&gt;
!wavenumber (cm&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;)&lt;br /&gt;
!Intensity (arbitrary units)&lt;br /&gt;
!symmetry&lt;br /&gt;
!IR active?&lt;br /&gt;
!type&lt;br /&gt;
|-&lt;br /&gt;
|1163&lt;br /&gt;
|93&lt;br /&gt;
|A&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;&#039; &#039;&lt;br /&gt;
|Yes&lt;br /&gt;
|Out of plane bend&lt;br /&gt;
|-&lt;br /&gt;
|1213&lt;br /&gt;
|14&lt;br /&gt;
|E&#039;&lt;br /&gt;
|Very slight&lt;br /&gt;
|Bend&lt;br /&gt;
|-&lt;br /&gt;
|1213&lt;br /&gt;
|14&lt;br /&gt;
|E&#039;&lt;br /&gt;
|Very slight&lt;br /&gt;
|Bend&lt;br /&gt;
|-&lt;br /&gt;
|2582&lt;br /&gt;
|0&lt;br /&gt;
|A&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;&#039;&lt;br /&gt;
|No&lt;br /&gt;
|Symmetric stretch&lt;br /&gt;
|-&lt;br /&gt;
|2716&lt;br /&gt;
|126&lt;br /&gt;
|E&#039;&lt;br /&gt;
|Yes&lt;br /&gt;
|Asymmetric stretch&lt;br /&gt;
|-&lt;br /&gt;
|2716&lt;br /&gt;
|126&lt;br /&gt;
|E&#039;&lt;br /&gt;
|Yes&lt;br /&gt;
|Asymmetric stretch&lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;IR spectrum&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
[[file:Hyc116_ir_bh3.png|400*600]]&lt;br /&gt;
&lt;br /&gt;
There are only three peaks on the IR spectrum of BH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;, despite that there are 6 vibrational modes for the molecule. As shown in the table above, the symmetric stretching mode with A1 symmetry at 2582 cm&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt; is not IR active; naturally, that vibrational mode doesn’t give a peak on the IR spectrum. As shown from the table, two pairs of vibrational modes, the bond angle deformation/bend at 1213 cm&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt; and the asymmetric bond stretch at 2716 cm&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;, are degenerate with the symmetry label E. This means that they have the same energy, and hence give the same wavenumber on the IR spectrum. Each pair of degenerate vibrational modes give rise to one peak. This leaves three peaks, as confirmed by the IR spectrum above.&lt;br /&gt;
&lt;br /&gt;
===Molecular orbitals of BH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;===&lt;br /&gt;
&lt;br /&gt;
[[file:hyc116_bh3_MO_diagram.png]]&lt;br /&gt;
&lt;br /&gt;
The above molecular orbital diagram was taken from Dr Patricia Hunt&#039;s &amp;lt;i&amp;gt;Lecture 4 Tutorial Problem Model Answers&amp;lt;/i&amp;gt;.&amp;lt;ref&amp;gt;P. Hunt, &amp;quot;Lecture 4 Tutorial Problem Model Answers&amp;quot;, 2 (2018)&amp;lt;/ref&amp;gt; Diagrams of the &amp;quot;real&amp;quot; MOs were obtained from Gaussian.&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
There is no significant difference between the LCAO MOs and the real ones. Features such as orbital phases are shown clearly on both the LCAO MOs and the real MOs, illustrating the bonding/anti-bonding characters of the molecular orbitals. This suggests that the the qualitative MO theory is highly accurate and useful when studying the molecular orbitals of molecules.&lt;br /&gt;
&lt;br /&gt;
==Associated energies: ammonium borane==&lt;br /&gt;
&lt;br /&gt;
===NH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;===&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;Calculation type&amp;lt;/b&amp;gt;: Optimisation&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;Calculation Method&amp;lt;/b&amp;gt;: B3LYP&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;Basis set&amp;lt;/b&amp;gt;: 6-31G(d,p) &lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Summary table&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
[[file:Hyc116_nh3_631g_summarytable.png]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Items table&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;pre&amp;gt;&lt;br /&gt;
Item               Value     Threshold  Converged?&lt;br /&gt;
 Maximum Force            0.000006     0.000450     YES&lt;br /&gt;
 RMS     Force            0.000004     0.000300     YES&lt;br /&gt;
 Maximum Displacement     0.000012     0.001800     YES&lt;br /&gt;
 RMS     Displacement     0.000008     0.001200     YES&lt;br /&gt;
&amp;lt;/pre&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Frequency log file&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
[[Media:HYC116_NH3_FREQ.LOG]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Frequencies&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;pre&amp;gt;&lt;br /&gt;
Low frequencies ---   -8.5646   -8.5588   -0.0047    0.0454    0.1784   26.4183&lt;br /&gt;
Low frequencies --- 1089.7603 1694.1865 1694.1865&lt;br /&gt;
&amp;lt;/pre&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;jmol of NH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;&#039;&#039;&#039;&lt;br /&gt;
&amp;lt;jmol&amp;gt;&amp;lt;jmolApplet&amp;gt;&lt;br /&gt;
  &amp;lt;title&amp;gt;optimised NH3&amp;lt;/title&amp;gt;&lt;br /&gt;
  &amp;lt;color&amp;gt;black&amp;lt;/color&amp;gt;&lt;br /&gt;
  &amp;lt;size&amp;gt;200&amp;lt;/size&amp;gt;&lt;br /&gt;
  &amp;lt;uploadedFileContents&amp;gt;HYC116_NH3_FREQ.LOG&amp;lt;/uploadedFileContents&amp;gt;&lt;br /&gt;
&amp;lt;/jmolApplet&amp;gt;&amp;lt;/jmol&amp;gt;&lt;br /&gt;
&lt;br /&gt;
===NH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;BH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;===&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;Calculation type&amp;lt;/b&amp;gt;: Optimisation&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;Calculation Method&amp;lt;/b&amp;gt;: B3LYP&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;Basis set&amp;lt;/b&amp;gt;: 6-31G(d,p) &lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Summary table&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
[[file:Hyc116_nh3bh3_631g_summarytable1.png]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Items table&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;pre&amp;gt;&lt;br /&gt;
Item               Value     Threshold  Converged?&lt;br /&gt;
 Maximum Force            0.000121     0.000450     YES&lt;br /&gt;
 RMS     Force            0.000057     0.000300     YES&lt;br /&gt;
 Maximum Displacement     0.000501     0.001800     YES&lt;br /&gt;
 RMS     Displacement     0.000293     0.001200     YES&lt;br /&gt;
&amp;lt;/pre&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Frequency log file&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
[[Media:HYC116_NH3BH3_FREQ1.LOG]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Frequencies&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;pre&amp;gt;&lt;br /&gt;
Low frequencies ---   -0.0574   -0.0501   -0.0074   21.6276   21.6377   40.3839&lt;br /&gt;
Low frequencies ---  265.9973  632.3725  640.1275&lt;br /&gt;
&amp;lt;/pre&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;jmol of NH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;BH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;&#039;&#039;&#039;&lt;br /&gt;
&amp;lt;jmol&amp;gt;&amp;lt;jmolApplet&amp;gt;&lt;br /&gt;
  &amp;lt;title&amp;gt;optimised NH3BH3&amp;lt;/title&amp;gt;&lt;br /&gt;
  &amp;lt;color&amp;gt;black&amp;lt;/color&amp;gt;&lt;br /&gt;
  &amp;lt;size&amp;gt;200&amp;lt;/size&amp;gt;&lt;br /&gt;
  &amp;lt;uploadedFileContents&amp;gt;HYC116_NH3BH3_FREQ.LOG&amp;lt;/uploadedFileContents&amp;gt;&lt;br /&gt;
&amp;lt;/jmolApplet&amp;gt;&amp;lt;/jmol&amp;gt;&lt;br /&gt;
&lt;br /&gt;
===Association energy===&lt;br /&gt;
&lt;br /&gt;
E(BH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;) (using the optimisation with the correct symmetry) = -26.61532363 a.u. = &amp;lt;b&amp;gt;-26.61532 a.u. (5 d.p.)&amp;lt;/b&amp;gt;&lt;br /&gt;
&lt;br /&gt;
E(NH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;) = -56.55776873 a.u. = &amp;lt;b&amp;gt;-56.55777 a.u. (5 d.p.)&amp;lt;/b&amp;gt;&lt;br /&gt;
&lt;br /&gt;
E(NH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;BH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;) = -83.22468892 a.u. = &amp;lt;b&amp;gt;-83.22469 a.u. (5 d.p.)&amp;lt;/b&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
Carrying out calculations using numbers which has already been rounded up can possibly result in errors in the last digit. Hence, here the calculations were carried out using the numbers provided from the optimisations (i.e. with more decimal places than necessary); the answer was then rounded up to the desired accuracy. &lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
ΔE = E(NH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;BH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;)-[E(NH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;)+E(BH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;)]&lt;br /&gt;
&lt;br /&gt;
ΔE = -83.22468892 - (-56.55776873 + -26.61532363) = -0.05159656 a.u. &lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;ΔE = -0.05160 a.u. (5 d.p.)&amp;lt;/b&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Converting energy from a.u. to kJ/mol&#039;&#039;&#039;&lt;br /&gt;
An atomic unit for energy is Hartree, which is equal to 2625.5 kJ/mol.&lt;br /&gt;
&amp;lt;ref&amp;gt;https://cccbdb.nist.gov/hartree.asp (Accessed: 22.05.2018)&amp;lt;/ref&amp;gt;&lt;br /&gt;
 &lt;br /&gt;
&lt;br /&gt;
So ΔE in kJ/mol = -0.05159657 * 2625.5 = -135.46676828 kJ/mol&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;ΔE = -135 kJ/mol (nearest integer)&amp;lt;/b&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
The energy difference calculated above comes from the formation of the B-N dative bond. It is a relatively weak bond. According to a bond energy data sheet provided by the University of California,&amp;lt;ref&amp;gt;https://labs.chem.ucsb.edu/zakarian/armen/11---bonddissociationenergy.pdf (Accessed: 24.05.2018)&amp;lt;/ref&amp;gt;  the bond energy of the C-C bond of an ethane molecule is 368 kJ/mol. This is a fair comparison to the NH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;BH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt; molecule as the two molecules have the same structure, only with the carbon atoms on ethane swapped for Boron and Nitrogen in NH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;BH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;&lt;br /&gt;
&lt;br /&gt;
==Using a mixture of basis-sets and pseudo-potentials==&lt;br /&gt;
&lt;br /&gt;
===BBr&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;===&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;Calculation type&amp;lt;/b&amp;gt;: Optimisation&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;Calculation Method&amp;lt;/b&amp;gt;: B3LYP&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;Basis set&amp;lt;/b&amp;gt;: Boron: 6-31G(d,p) ; Br: LANL2DZ&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
Larger calculations are often sent to a web-server to run on a high-performance computer instead of a desktop. In order to experience and learn to use a web-server, the optimisation and the frequency analysis for BBr&amp;lt;sub&amp;gt;3&amp;lt;/sub were both sent and done on a server instead of the desktop. The calculation results were downloaded from the web-server once they were finished.   &lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Summary table&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
[[file:Hyc116_bbr3_opt_summarytable.png]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Items table&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;pre&amp;gt;&lt;br /&gt;
Item               Value     Threshold  Converged?&lt;br /&gt;
 Maximum Force            0.000008     0.000450     YES&lt;br /&gt;
 RMS     Force            0.000005     0.000300     YES&lt;br /&gt;
 Maximum Displacement     0.000036     0.001800     YES&lt;br /&gt;
 RMS     Displacement     0.000023     0.001200     YES&lt;br /&gt;
&amp;lt;/pre&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Frequency log file&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
[[Media:Hyc116_bbr3_freq.log]]&lt;br /&gt;
&lt;br /&gt;
Attached above is the frequency file saved onto the computer from the SCAN server portal. The frequency file was also published on the chemistry database DSpace. {{DOI|10042/202442}}&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Frequencies&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;pre&amp;gt;&lt;br /&gt;
Low frequencies ---   -0.0137   -0.0064   -0.0046    2.4315    2.4315    4.8421&lt;br /&gt;
Low frequencies ---  155.9631  155.9651  267.7052&lt;br /&gt;
&amp;lt;/pre&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;jmol of BBr&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;&#039;&#039;&#039;&lt;br /&gt;
&amp;lt;jmol&amp;gt;&amp;lt;jmolApplet&amp;gt;&lt;br /&gt;
  &amp;lt;title&amp;gt;optimised BBr3&amp;lt;/title&amp;gt;&lt;br /&gt;
  &amp;lt;color&amp;gt;black&amp;lt;/color&amp;gt;&lt;br /&gt;
  &amp;lt;size&amp;gt;200&amp;lt;/size&amp;gt;&lt;br /&gt;
  &amp;lt;uploadedFileContents&amp;gt;Hyc116_bbr3_freq.log&amp;lt;/uploadedFileContents&amp;gt;&lt;br /&gt;
&amp;lt;/jmolApplet&amp;gt;&amp;lt;/jmol&amp;gt;&lt;br /&gt;
&lt;br /&gt;
==Aromaticity==&lt;br /&gt;
&lt;br /&gt;
===Benzene===&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;Calculation type&amp;lt;/b&amp;gt;: Optimisation&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;Calculation Method&amp;lt;/b&amp;gt;: B3LYP&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;Basis set&amp;lt;/b&amp;gt;: 6-31G(d,p) &lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Summary table&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
[[file:Hyc116_c6h6_summarytable.png]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Items table&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;pre&amp;gt;&lt;br /&gt;
Item               Value     Threshold  Converged?&lt;br /&gt;
 Maximum Force            0.000193     0.000450     YES&lt;br /&gt;
 RMS     Force            0.000079     0.000300     YES&lt;br /&gt;
 Maximum Displacement     0.000830     0.001800     YES&lt;br /&gt;
 RMS     Displacement     0.000294     0.001200     YES&lt;br /&gt;
&amp;lt;/pre&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Frequency log file&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
[[Media:HYC116_C6H6_FREQ.LOG]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Frequencies&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;pre&amp;gt;&lt;br /&gt;
Low frequencies ---   -3.5606   -3.5606   -0.0089   -0.0043   -0.0043   10.0905&lt;br /&gt;
Low frequencies ---  413.9582  413.9582  621.1416&lt;br /&gt;
&amp;lt;/pre&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;jmol of C&amp;lt;sub&amp;gt;6&amp;lt;/sub&amp;gt;H&amp;lt;sub&amp;gt;6&amp;lt;/sub&amp;gt;&#039;&#039;&#039;&lt;br /&gt;
&amp;lt;jmol&amp;gt;&amp;lt;jmolApplet&amp;gt;&lt;br /&gt;
  &amp;lt;title&amp;gt;optimised Benzene&amp;lt;/title&amp;gt;&lt;br /&gt;
  &amp;lt;color&amp;gt;black&amp;lt;/color&amp;gt;&lt;br /&gt;
  &amp;lt;size&amp;gt;200&amp;lt;/size&amp;gt;&lt;br /&gt;
  &amp;lt;uploadedFileContents&amp;gt;HYC116_C6H6_FREQ.LOG&amp;lt;/uploadedFileContents&amp;gt;&lt;br /&gt;
&amp;lt;/jmolApplet&amp;gt;&amp;lt;/jmol&amp;gt;&lt;br /&gt;
&lt;br /&gt;
===Borazine===&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;Calculation type&amp;lt;/b&amp;gt;: Optimisation&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;Calculation Method&amp;lt;/b&amp;gt;: B3LYP&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;Basis set&amp;lt;/b&amp;gt;: 6-31G(d,p) &lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Summary table&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
[[file:Hyc116_borazine_summarytable.png]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Items table&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;pre&amp;gt;&lt;br /&gt;
Item               Value     Threshold  Converged?&lt;br /&gt;
 Maximum Force            0.000085     0.000450     YES&lt;br /&gt;
 RMS     Force            0.000033     0.000300     YES&lt;br /&gt;
 Maximum Displacement     0.000250     0.001800     YES&lt;br /&gt;
 RMS     Displacement     0.000074     0.001200     YES&lt;br /&gt;
&amp;lt;/pre&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Frequency log file&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
[[Media:HYC116_BORAZINE_FREQ.LOG]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Frequencies&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;pre&amp;gt;&lt;br /&gt;
Low frequencies ---  -12.6626  -12.6626   -8.9272   -0.0211   -0.0104   -0.0104&lt;br /&gt;
Low frequencies ---  289.1112  289.1112  403.8613&lt;br /&gt;
&amp;lt;/pre&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;jmol of Borazine&#039;&#039;&#039;&lt;br /&gt;
&amp;lt;jmol&amp;gt;&amp;lt;jmolApplet&amp;gt;&lt;br /&gt;
  &amp;lt;title&amp;gt;optimised Borazine&amp;lt;/title&amp;gt;&lt;br /&gt;
  &amp;lt;color&amp;gt;black&amp;lt;/color&amp;gt;&lt;br /&gt;
  &amp;lt;size&amp;gt;200&amp;lt;/size&amp;gt;&lt;br /&gt;
  &amp;lt;uploadedFileContents&amp;gt;HYC116_BORAZINE_FREQ.LOG&amp;lt;/uploadedFileContents&amp;gt;&lt;br /&gt;
&amp;lt;/jmolApplet&amp;gt;&amp;lt;/jmol&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
===Charge distribution===&lt;br /&gt;
&lt;br /&gt;
An NBO charge analysis was carried out on both the optimised benzene and borazine. Visualisations of the charge distribution are shown in the table below, with the colour range going from -1.102 to 1.102 for both molecule. This large scale was chosen as it allows direct comparison of the charge on any atoms in these two molecules and shows the relative magnitude of charges on all these atoms. Negative charges are shown in red, and positive charges are shown in green. A neutral charge is displayed in black, so the smaller a charge is (positive or negative), the darker its colour representation is. Larger charges are shown in brighter colours. The charges are also displayed on the atoms as numbers with a neutral charge being zero. Negative charges are shown as negative number and positive charges are shown as positive numbers. &lt;br /&gt;
&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot;&lt;br /&gt;
!&lt;br /&gt;
!Benzene&lt;br /&gt;
!Borazine&lt;br /&gt;
|-&lt;br /&gt;
!Visualisation of charge distribution&lt;br /&gt;
|[[File:Hyc116_benzene_charge_distribution1.png|500x500px|thumb|centre|Charge distribution of Benzene visualisation]]&lt;br /&gt;
|[[File:Hyc116_borazine_charge_distribution1.png|500x500px|thumb|centre|Charge distribution of Borazine visualisation]]&lt;br /&gt;
|-&lt;br /&gt;
!Charge &lt;br /&gt;
|Carbon: -0.239&lt;br /&gt;
&lt;br /&gt;
Hydrogen: 0.239&lt;br /&gt;
|Nitrogen: -1.102 &lt;br /&gt;
&lt;br /&gt;
Boron: 0.747&lt;br /&gt;
&lt;br /&gt;
Hydrogen (bonded to N): 0.432&lt;br /&gt;
&lt;br /&gt;
Hydrogen (bonded to B): -0.077&lt;br /&gt;
|-&lt;br /&gt;
!Discussion&lt;br /&gt;
|From the visualisation, it is shown that there is a slightly negative charge on the carbon atoms, and a positive charge of the same magnitude on the hydrogen atoms. All the carbon atoms have the same charge as they are in identical environments. The same applies to all the hydrogen atoms. This is due to the highly symmetrical structure of benzene. Since the same colour scale was used for both benzene and borazine, and the charges are much smaller in magnitude on atoms in benzene than atoms on borazine, the colours on the charge distribution visualisation is much darker. &lt;br /&gt;
|Polar bonds between nitrogen and boron are demonstration from the above visualisation. From the colours displayed on the charge distribution visualisation as well as the charge values, it is shown that nitrogen has a relatively large negative charge, while boron has a positive charge. This is due to the difference in electrogenativity between these atoms: nitrogen atoms are more electronegative than boron and tends to attract electrons towards themselves. It is worth noting that the hydrogen atoms do not all have the same charge. The hydrogen atoms bonded to boron have a slightly negative charge, and the ones bonded to nitrogen have a small positive charge. &lt;br /&gt;
&lt;br /&gt;
The fact that the same colour scale was used for both molecules comes in helpful here. It allows the charges on atoms to be compared directly. For example, just from looking at the colours, one can tell that or example, even though both carbon and nitrogen are electronegative, nitrogen is much more electronegative, which is quantitatively shown by Pauling&#039;s electronegativity scale.&amp;lt;ref&amp;gt;http://www.tutor-homework.com/Chemistry_Help/electronegativity_table/electronegativity.html (Accessed: 24.0502018&amp;lt;/ref&amp;gt;&lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
===Comparative MOs of Benzene and Borazine===&lt;br /&gt;
&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot;&lt;br /&gt;
!&lt;br /&gt;
!Benzene&lt;br /&gt;
!Borazine&lt;br /&gt;
!Comparison and Discussion&lt;br /&gt;
|-&lt;br /&gt;
!1st comparative pair&lt;br /&gt;
|[[File:Hyc116_benzene_1st_MO_pair_7.png|200x200px|centre]]&lt;br /&gt;
|[[File:Hyc116_borazine_1st_MO_pair_level9.png|200x200px|centre]]&lt;br /&gt;
|MO 9 of both benzene and borazine are comparable. They both show delocalised molecular orbital with an overall bonding character. There is a nodal plane across the molecular orbitals for both benzene and borazine. For benzene, there is contribution from all the carbon and hydrogen s orbitals. Moreover, the molecular orbitals are symmetric to their counterpart of opposite phase, giving an E&amp;lt;sub&amp;gt;1g&amp;lt;/sub&amp;gt; MO. That is not the case for borazine; they are less symmetric in borazine. This MO of borazine has an E&#039; symmetry. Nitrogen atoms are more electronegative than boron atoms and pull electron density towards themselves, resulting in a larger lobe. There is contribution from all the boron and nitrogen s orbitals, and three of the hydrogen s orbitals, though not all of them. &lt;br /&gt;
|-&lt;br /&gt;
!2nd comparative pair&lt;br /&gt;
|[[File:Hyc116_benzene_2nd_MO_pair_10.png|200x200px|centre]]&lt;br /&gt;
|[[File:Hyc116_borazine_2nd_MO_pair_level11.png|200x200px|centre]]&lt;br /&gt;
|MO 10 of benzene and MO 11 of borazine are comparable. Here shows a pair of rather delocalised molecular orbitals with slightly more antibonding character than the first pair shown above. On both MOs, there is no contribution from one pair of opposite hydrogen atoms, but contribution from s orbitals of all other atoms on both molecule. The benzene MO has an E&amp;lt;sub&amp;gt;2g&amp;lt;/sub&amp;gt; symmetry. In borazine, the lobes are in different sizes due to the higher electronegativity of nitrogen. The lobes at the nitrogen atoms are larger as they attract electrons towards themselves more so than boron atoms do. This borazine MO has an E&#039; symmetry. &lt;br /&gt;
|-&lt;br /&gt;
!3rd comparative pair&lt;br /&gt;
|[[File:Hyc116_benzene_3rd_MO_pair_21.png|200x200px|centre]]&lt;br /&gt;
|[[File:Hyc116_borazine_3rd_MO_pair_level21.png|200x200px|centre]]&lt;br /&gt;
|The HOMO (MO 21) of benzene and the HOMO (MO 21) of borazine are comparable. They are both made of p orbitals of all carbon atoms (or all boron and nitrogen atoms in the case of borazine); there is no contribution from hydrogen atoms as they do not have p orbitals. There is a nodal plan perpendicular to the z axis (highest rotational axis) and one parallel to the z axis. On benzene, the MO is very symmetric and has an E&amp;lt;sub&amp;gt;1g&amp;lt;/sub&amp;gt; symmetry; the lobes of the MO are the same in size. On borazine, the lobe where there are two nitrogen atoms is bigger in size, again due to the higher electronegtivity of nitrogen compared to boron. The borazine MO has an E&#039; &#039; symmetry.&lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
===Aromaticity: some theories===&lt;br /&gt;
&lt;br /&gt;
Aromatic compounds display properties such as their high stability and bond lengths between typical single and double bonds. A simple understanding of aromaticity involves the overlap of p orbitals perpendicular to the cyclic plane; the delocalisation of electrons on the pi system is identified to be responsible of the stability of aromatic systems. Aromatic compounds can be identified by the Huckel’s rule, which states that conjugated planar cyclic molecules with (4n +2) π electrons are aromatic. Both benzene and borazine obey the Huckel’s rule and fit the conventional description of aromaticity. &lt;br /&gt;
&lt;br /&gt;
However, it is proved in recent years that the conventional criteria do not necessarily have to be obeyed for a compound to be aromatic. For instance, there has been shown that some non-planar compounds display aromaticity. This suggests that the criteria for aromaticity is not simply structural, and these advances give rise to concepts such as quasiaromaticity and pseudoaromaticity. Recent advances show that there are quantum mechanics basis on the idea of aromaticity. &lt;br /&gt;
In conclusion, while the overlap of pi orbitals provides a simple understanding for aromaticity, it is not a sufficient description for aromaticity.&lt;br /&gt;
&lt;br /&gt;
==References==&lt;br /&gt;
{{reflist}}&lt;/div&gt;</summary>
		<author><name>Hyc116</name></author>
	</entry>
	<entry>
		<id>https://chemwiki.ch.ic.ac.uk/index.php?title=MO_hyc116&amp;diff=732302</id>
		<title>MO hyc116</title>
		<link rel="alternate" type="text/html" href="https://chemwiki.ch.ic.ac.uk/index.php?title=MO_hyc116&amp;diff=732302"/>
		<updated>2018-05-25T14:53:27Z</updated>

		<summary type="html">&lt;p&gt;Hyc116: /* Comparative MOs of Benzene and Borazine */&lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;==BH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;==&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;Calculation type&amp;lt;/b&amp;gt;: Optimisation&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;Calculation Method&amp;lt;/b&amp;gt;: B3LYP&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;Basis set&amp;lt;/b&amp;gt;: 6-31G(d,p) &lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Summary table&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
[[file:Hyc116_bh3_631g_opt_summarytable.png]]&lt;br /&gt;
&lt;br /&gt;
The above summary table was obtained after the 2nd optimisation of BH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt; (after the initial optimisation using the 3-21G basis set). Notice how the symmetry is incorrect and shown as Cs. This is because the symmetry was manually broken at the beginning by changing the bond length of B-H bonds. The point group was manually adjusted and the molecule was optimised again before the frequency analysis and the new summary table is attached below.&lt;br /&gt;
&lt;br /&gt;
[[file:Hyc116_bh3_correctsummarytable.png]]&lt;br /&gt;
&lt;br /&gt;
The above summary table was obtained from the optimisation after adjusting the symmetry. The point shown in this summary table is D&amp;lt;sub&amp;gt;3h&amp;lt;/sub&amp;gt;, which is the correct for BH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;. &lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Items table&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
Below is the items table taken from the optimisation with the correct point group.&lt;br /&gt;
&lt;br /&gt;
&amp;lt;pre&amp;gt;&lt;br /&gt;
Item               Value     Threshold  Converged?&lt;br /&gt;
 Maximum Force            0.000015     0.000450     YES&lt;br /&gt;
 RMS     Force            0.000010     0.000300     YES&lt;br /&gt;
 Maximum Displacement     0.000058     0.001800     YES&lt;br /&gt;
 RMS     Displacement     0.000038     0.001200     YES&lt;br /&gt;
&amp;lt;/pre&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Frequency log file&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
[[Media:HYC116 BH3 FREQ.LOG]] &lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Frequencies&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;pre&amp;gt;&lt;br /&gt;
Low frequencies ---  -10.3498   -3.4492   -1.2454   -0.0055    0.4779    3.2165&lt;br /&gt;
Low frequencies --- 1162.9519 1213.1527 1213.1554&lt;br /&gt;
&amp;lt;/pre&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;jmol of BH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;&#039;&#039;&#039;&lt;br /&gt;
&amp;lt;jmol&amp;gt;&amp;lt;jmolApplet&amp;gt;&lt;br /&gt;
  &amp;lt;title&amp;gt;optimised BH3&amp;lt;/title&amp;gt;&lt;br /&gt;
  &amp;lt;color&amp;gt;black&amp;lt;/color&amp;gt;&lt;br /&gt;
  &amp;lt;size&amp;gt;200&amp;lt;/size&amp;gt;&lt;br /&gt;
  &amp;lt;uploadedFileContents&amp;gt;HYC116_BH3_FREQ.LOG&amp;lt;/uploadedFileContents&amp;gt;&lt;br /&gt;
&amp;lt;/jmolApplet&amp;gt;&amp;lt;/jmol&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
===Vibrational spectrum===&lt;br /&gt;
&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot;&lt;br /&gt;
!wavenumber (cm&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;)&lt;br /&gt;
!Intensity (arbitrary units)&lt;br /&gt;
!symmetry&lt;br /&gt;
!IR active?&lt;br /&gt;
!type&lt;br /&gt;
|-&lt;br /&gt;
|1163&lt;br /&gt;
|93&lt;br /&gt;
|A&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;&#039; &#039;&lt;br /&gt;
|Yes&lt;br /&gt;
|Out of plane bend&lt;br /&gt;
|-&lt;br /&gt;
|1213&lt;br /&gt;
|14&lt;br /&gt;
|E&#039;&lt;br /&gt;
|Very slight&lt;br /&gt;
|Bend&lt;br /&gt;
|-&lt;br /&gt;
|1213&lt;br /&gt;
|14&lt;br /&gt;
|E&#039;&lt;br /&gt;
|Very slight&lt;br /&gt;
|Bend&lt;br /&gt;
|-&lt;br /&gt;
|2582&lt;br /&gt;
|0&lt;br /&gt;
|A&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;&#039;&lt;br /&gt;
|No&lt;br /&gt;
|Symmetric stretch&lt;br /&gt;
|-&lt;br /&gt;
|2716&lt;br /&gt;
|126&lt;br /&gt;
|E&#039;&lt;br /&gt;
|Yes&lt;br /&gt;
|Asymmetric stretch&lt;br /&gt;
|-&lt;br /&gt;
|2716&lt;br /&gt;
|126&lt;br /&gt;
|E&#039;&lt;br /&gt;
|Yes&lt;br /&gt;
|Asymmetric stretch&lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;IR spectrum&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
[[file:Hyc116_ir_bh3.png|400*600]]&lt;br /&gt;
&lt;br /&gt;
There are only three peaks on the IR spectrum of BH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;, despite that there are 6 vibrational modes for the molecule. As shown in the table above, the symmetric stretching mode with A1 symmetry at 2582 cm&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt; is not IR active; naturally, that vibrational mode doesn’t give a peak on the IR spectrum. As shown from the table, two pairs of vibrational modes, the bond angle deformation/bend at 1213 cm&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt; and the asymmetric bond stretch at 2716 cm&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;, are degenerate with the symmetry label E. This means that they have the same energy, and hence give the same wavenumber on the IR spectrum. Each pair of degenerate vibrational modes give rise to one peak. This leaves three peaks, as confirmed by the IR spectrum above.&lt;br /&gt;
&lt;br /&gt;
===Molecular orbitals of BH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;===&lt;br /&gt;
&lt;br /&gt;
[[file:hyc116_bh3_MO_diagram.png]]&lt;br /&gt;
&lt;br /&gt;
The above molecular orbital diagram was taken from Dr Patricia Hunt&#039;s &amp;lt;i&amp;gt;Lecture 4 Tutorial Problem Model Answers&amp;lt;/i&amp;gt;.&amp;lt;ref&amp;gt;P. Hunt, &amp;quot;Lecture 4 Tutorial Problem Model Answers&amp;quot;, 2 (2018)&amp;lt;/ref&amp;gt; Diagrams of the &amp;quot;real&amp;quot; MOs were obtained from Gaussian.&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
There is no significant difference between the LCAO MOs and the real ones. Features such as orbital phases are shown clearly on both the LCAO MOs and the real MOs, illustrating the bonding/anti-bonding characters of the molecular orbitals. This suggests that the the qualitative MO theory is highly accurate and useful when studying the molecular orbitals of molecules.&lt;br /&gt;
&lt;br /&gt;
==Associated energies: ammonium borane==&lt;br /&gt;
&lt;br /&gt;
===NH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;===&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;Calculation type&amp;lt;/b&amp;gt;: Optimisation&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;Calculation Method&amp;lt;/b&amp;gt;: B3LYP&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;Basis set&amp;lt;/b&amp;gt;: 6-31G(d,p) &lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Summary table&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
[[file:Hyc116_nh3_631g_summarytable.png]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Items table&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;pre&amp;gt;&lt;br /&gt;
Item               Value     Threshold  Converged?&lt;br /&gt;
 Maximum Force            0.000006     0.000450     YES&lt;br /&gt;
 RMS     Force            0.000004     0.000300     YES&lt;br /&gt;
 Maximum Displacement     0.000012     0.001800     YES&lt;br /&gt;
 RMS     Displacement     0.000008     0.001200     YES&lt;br /&gt;
&amp;lt;/pre&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Frequency log file&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
[[Media:HYC116_NH3_FREQ.LOG]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Frequencies&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;pre&amp;gt;&lt;br /&gt;
Low frequencies ---   -8.5646   -8.5588   -0.0047    0.0454    0.1784   26.4183&lt;br /&gt;
Low frequencies --- 1089.7603 1694.1865 1694.1865&lt;br /&gt;
&amp;lt;/pre&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;jmol of NH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;&#039;&#039;&#039;&lt;br /&gt;
&amp;lt;jmol&amp;gt;&amp;lt;jmolApplet&amp;gt;&lt;br /&gt;
  &amp;lt;title&amp;gt;optimised NH3&amp;lt;/title&amp;gt;&lt;br /&gt;
  &amp;lt;color&amp;gt;black&amp;lt;/color&amp;gt;&lt;br /&gt;
  &amp;lt;size&amp;gt;200&amp;lt;/size&amp;gt;&lt;br /&gt;
  &amp;lt;uploadedFileContents&amp;gt;HYC116_NH3_FREQ.LOG&amp;lt;/uploadedFileContents&amp;gt;&lt;br /&gt;
&amp;lt;/jmolApplet&amp;gt;&amp;lt;/jmol&amp;gt;&lt;br /&gt;
&lt;br /&gt;
===NH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;BH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;===&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;Calculation type&amp;lt;/b&amp;gt;: Optimisation&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;Calculation Method&amp;lt;/b&amp;gt;: B3LYP&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;Basis set&amp;lt;/b&amp;gt;: 6-31G(d,p) &lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Summary table&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
[[file:Hyc116_nh3bh3_631g_summarytable1.png]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Items table&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;pre&amp;gt;&lt;br /&gt;
Item               Value     Threshold  Converged?&lt;br /&gt;
 Maximum Force            0.000121     0.000450     YES&lt;br /&gt;
 RMS     Force            0.000057     0.000300     YES&lt;br /&gt;
 Maximum Displacement     0.000501     0.001800     YES&lt;br /&gt;
 RMS     Displacement     0.000293     0.001200     YES&lt;br /&gt;
&amp;lt;/pre&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Frequency log file&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
[[Media:HYC116_NH3BH3_FREQ1.LOG]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Frequencies&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;pre&amp;gt;&lt;br /&gt;
Low frequencies ---   -0.0574   -0.0501   -0.0074   21.6276   21.6377   40.3839&lt;br /&gt;
Low frequencies ---  265.9973  632.3725  640.1275&lt;br /&gt;
&amp;lt;/pre&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;jmol of NH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;BH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;&#039;&#039;&#039;&lt;br /&gt;
&amp;lt;jmol&amp;gt;&amp;lt;jmolApplet&amp;gt;&lt;br /&gt;
  &amp;lt;title&amp;gt;optimised NH3BH3&amp;lt;/title&amp;gt;&lt;br /&gt;
  &amp;lt;color&amp;gt;black&amp;lt;/color&amp;gt;&lt;br /&gt;
  &amp;lt;size&amp;gt;200&amp;lt;/size&amp;gt;&lt;br /&gt;
  &amp;lt;uploadedFileContents&amp;gt;HYC116_NH3BH3_FREQ.LOG&amp;lt;/uploadedFileContents&amp;gt;&lt;br /&gt;
&amp;lt;/jmolApplet&amp;gt;&amp;lt;/jmol&amp;gt;&lt;br /&gt;
&lt;br /&gt;
===Association energy===&lt;br /&gt;
&lt;br /&gt;
E(BH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;) (using the optimisation with the correct symmetry) = -26.61532363 a.u. = &amp;lt;b&amp;gt;-26.61532 a.u. (5 d.p.)&amp;lt;/b&amp;gt;&lt;br /&gt;
&lt;br /&gt;
E(NH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;) = -56.55776873 a.u. = &amp;lt;b&amp;gt;-56.55777 a.u. (5 d.p.)&amp;lt;/b&amp;gt;&lt;br /&gt;
&lt;br /&gt;
E(NH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;BH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;) = -83.22468892 a.u. = &amp;lt;b&amp;gt;-83.22469 a.u. (5 d.p.)&amp;lt;/b&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
Carrying out calculations using numbers which has already been rounded up can possibly result in errors in the last digit. Hence, here the calculations were carried out using the numbers provided from the optimisations (i.e. with more decimal places than necessary); the answer was then rounded up to the desired accuracy. &lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
ΔE = E(NH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;BH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;)-[E(NH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;)+E(BH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;)]&lt;br /&gt;
&lt;br /&gt;
ΔE = -83.22468892 - (-56.55776873 + -26.61532363) = -0.05159656 a.u. &lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;ΔE = -0.05160 a.u. (5 d.p.)&amp;lt;/b&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Converting energy from a.u. to kJ/mol&#039;&#039;&#039;&lt;br /&gt;
An atomic unit for energy is Hartree, which is equal to 2625.5 kJ/mol.&lt;br /&gt;
&amp;lt;ref&amp;gt;https://cccbdb.nist.gov/hartree.asp (Accessed: 22.05.2018)&amp;lt;/ref&amp;gt;&lt;br /&gt;
 &lt;br /&gt;
&lt;br /&gt;
So ΔE in kJ/mol = -0.05159657 * 2625.5 = -135.46676828 kJ/mol&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;ΔE = -135 kJ/mol (nearest integer)&amp;lt;/b&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
The energy difference calculated above comes from the formation of the B-N dative bond. It is a relatively weak bond. According to a bond energy data sheet provided by the University of California,&amp;lt;ref&amp;gt;https://labs.chem.ucsb.edu/zakarian/armen/11---bonddissociationenergy.pdf (Accessed: 24.05.2018)&amp;lt;/ref&amp;gt;  the bond energy of the C-C bond of an ethane molecule is 368 kJ/mol. This is a fair comparison to the NH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;BH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt; molecule as the two molecules have the same structure, only with the carbon atoms on ethane swapped for Boron and Nitrogen in NH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;BH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;&lt;br /&gt;
&lt;br /&gt;
==Using a mixture of basis-sets and pseudo-potentials==&lt;br /&gt;
&lt;br /&gt;
===BBr&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;===&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;Calculation type&amp;lt;/b&amp;gt;: Optimisation&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;Calculation Method&amp;lt;/b&amp;gt;: B3LYP&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;Basis set&amp;lt;/b&amp;gt;: Boron: 6-31G(d,p) ; Br: LANL2DZ&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
Larger calculations are often sent to a web-server to run on a high-performance computer instead of a desktop. In order to experience and learn to use a web-server, the optimisation and the frequency analysis for BBr&amp;lt;sub&amp;gt;3&amp;lt;/sub were both sent and done on a server instead of the desktop. The calculation results were downloaded from the web-server once they were finished.   &lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Summary table&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
[[file:Hyc116_bbr3_opt_summarytable.png]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Items table&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;pre&amp;gt;&lt;br /&gt;
Item               Value     Threshold  Converged?&lt;br /&gt;
 Maximum Force            0.000008     0.000450     YES&lt;br /&gt;
 RMS     Force            0.000005     0.000300     YES&lt;br /&gt;
 Maximum Displacement     0.000036     0.001800     YES&lt;br /&gt;
 RMS     Displacement     0.000023     0.001200     YES&lt;br /&gt;
&amp;lt;/pre&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Frequency log file&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
[[Media:Hyc116_bbr3_freq.log]]&lt;br /&gt;
&lt;br /&gt;
Attached above is the frequency file saved onto the computer from the SCAN server portal. The frequency file was also published on the chemistry database DSpace. {{DOI|10042/202442}}&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Frequencies&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;pre&amp;gt;&lt;br /&gt;
Low frequencies ---   -0.0137   -0.0064   -0.0046    2.4315    2.4315    4.8421&lt;br /&gt;
Low frequencies ---  155.9631  155.9651  267.7052&lt;br /&gt;
&amp;lt;/pre&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;jmol of BBr&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;&#039;&#039;&#039;&lt;br /&gt;
&amp;lt;jmol&amp;gt;&amp;lt;jmolApplet&amp;gt;&lt;br /&gt;
  &amp;lt;title&amp;gt;optimised BBr3&amp;lt;/title&amp;gt;&lt;br /&gt;
  &amp;lt;color&amp;gt;black&amp;lt;/color&amp;gt;&lt;br /&gt;
  &amp;lt;size&amp;gt;200&amp;lt;/size&amp;gt;&lt;br /&gt;
  &amp;lt;uploadedFileContents&amp;gt;Hyc116_bbr3_freq.log&amp;lt;/uploadedFileContents&amp;gt;&lt;br /&gt;
&amp;lt;/jmolApplet&amp;gt;&amp;lt;/jmol&amp;gt;&lt;br /&gt;
&lt;br /&gt;
==Aromaticity==&lt;br /&gt;
&lt;br /&gt;
===Benzene===&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;Calculation type&amp;lt;/b&amp;gt;: Optimisation&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;Calculation Method&amp;lt;/b&amp;gt;: B3LYP&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;Basis set&amp;lt;/b&amp;gt;: 6-31G(d,p) &lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Summary table&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
[[file:Hyc116_c6h6_summarytable.png]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Items table&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;pre&amp;gt;&lt;br /&gt;
Item               Value     Threshold  Converged?&lt;br /&gt;
 Maximum Force            0.000193     0.000450     YES&lt;br /&gt;
 RMS     Force            0.000079     0.000300     YES&lt;br /&gt;
 Maximum Displacement     0.000830     0.001800     YES&lt;br /&gt;
 RMS     Displacement     0.000294     0.001200     YES&lt;br /&gt;
&amp;lt;/pre&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Frequency log file&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
[[Media:HYC116_C6H6_FREQ.LOG]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Frequencies&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;pre&amp;gt;&lt;br /&gt;
Low frequencies ---   -3.5606   -3.5606   -0.0089   -0.0043   -0.0043   10.0905&lt;br /&gt;
Low frequencies ---  413.9582  413.9582  621.1416&lt;br /&gt;
&amp;lt;/pre&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;jmol of C&amp;lt;sub&amp;gt;6&amp;lt;/sub&amp;gt;H&amp;lt;sub&amp;gt;6&amp;lt;/sub&amp;gt;&#039;&#039;&#039;&lt;br /&gt;
&amp;lt;jmol&amp;gt;&amp;lt;jmolApplet&amp;gt;&lt;br /&gt;
  &amp;lt;title&amp;gt;optimised Benzene&amp;lt;/title&amp;gt;&lt;br /&gt;
  &amp;lt;color&amp;gt;black&amp;lt;/color&amp;gt;&lt;br /&gt;
  &amp;lt;size&amp;gt;200&amp;lt;/size&amp;gt;&lt;br /&gt;
  &amp;lt;uploadedFileContents&amp;gt;HYC116_C6H6_FREQ.LOG&amp;lt;/uploadedFileContents&amp;gt;&lt;br /&gt;
&amp;lt;/jmolApplet&amp;gt;&amp;lt;/jmol&amp;gt;&lt;br /&gt;
&lt;br /&gt;
===Borazine===&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;Calculation type&amp;lt;/b&amp;gt;: Optimisation&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;Calculation Method&amp;lt;/b&amp;gt;: B3LYP&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;Basis set&amp;lt;/b&amp;gt;: 6-31G(d,p) &lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Summary table&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
[[file:Hyc116_borazine_summarytable.png]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Items table&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;pre&amp;gt;&lt;br /&gt;
Item               Value     Threshold  Converged?&lt;br /&gt;
 Maximum Force            0.000085     0.000450     YES&lt;br /&gt;
 RMS     Force            0.000033     0.000300     YES&lt;br /&gt;
 Maximum Displacement     0.000250     0.001800     YES&lt;br /&gt;
 RMS     Displacement     0.000074     0.001200     YES&lt;br /&gt;
&amp;lt;/pre&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Frequency log file&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
[[Media:HYC116_BORAZINE_FREQ.LOG]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Frequencies&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;pre&amp;gt;&lt;br /&gt;
Low frequencies ---  -12.6626  -12.6626   -8.9272   -0.0211   -0.0104   -0.0104&lt;br /&gt;
Low frequencies ---  289.1112  289.1112  403.8613&lt;br /&gt;
&amp;lt;/pre&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;jmol of Borazine&#039;&#039;&#039;&lt;br /&gt;
&amp;lt;jmol&amp;gt;&amp;lt;jmolApplet&amp;gt;&lt;br /&gt;
  &amp;lt;title&amp;gt;optimised Borazine&amp;lt;/title&amp;gt;&lt;br /&gt;
  &amp;lt;color&amp;gt;black&amp;lt;/color&amp;gt;&lt;br /&gt;
  &amp;lt;size&amp;gt;200&amp;lt;/size&amp;gt;&lt;br /&gt;
  &amp;lt;uploadedFileContents&amp;gt;HYC116_BORAZINE_FREQ.LOG&amp;lt;/uploadedFileContents&amp;gt;&lt;br /&gt;
&amp;lt;/jmolApplet&amp;gt;&amp;lt;/jmol&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
===Charge distribution===&lt;br /&gt;
&lt;br /&gt;
An NBO charge analysis was carried out on both the optimised benzene and borazine. Visualisations of the charge distribution are shown in the table below, with the colour range going from -1.102 to 1.102 for both molecule. This large scale was chosen as it allows direct comparison of the charge on any atoms in these two molecules and shows the relative magnitude of charges on all these atoms. Negative charges are shown in red, and positive charges are shown in green. A neutral charge is displayed in black, so the smaller a charge is (positive or negative), the darker its colour representation is. Larger charges are shown in brighter colours. The charges are also displayed on the atoms as numbers with a neutral charge being zero. Negative charges are shown as negative number and positive charges are shown as positive numbers. &lt;br /&gt;
&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot;&lt;br /&gt;
!&lt;br /&gt;
!Benzene&lt;br /&gt;
!Borazine&lt;br /&gt;
|-&lt;br /&gt;
!Visualisation of charge distribution&lt;br /&gt;
|[[File:Hyc116_benzene_charge_distribution1.png|500x500px|thumb|centre|Charge distribution of Benzene visualisation]]&lt;br /&gt;
|[[File:Hyc116_borazine_charge_distribution1.png|500x500px|thumb|centre|Charge distribution of Borazine visualisation]]&lt;br /&gt;
|-&lt;br /&gt;
!Charge &lt;br /&gt;
|Carbon: -0.239&lt;br /&gt;
&lt;br /&gt;
Hydrogen: 0.239&lt;br /&gt;
|Nitrogen: -1.102 &lt;br /&gt;
&lt;br /&gt;
Boron: 0.747&lt;br /&gt;
&lt;br /&gt;
Hydrogen (bonded to N): 0.432&lt;br /&gt;
&lt;br /&gt;
Hydrogen (bonded to B): -0.077&lt;br /&gt;
|-&lt;br /&gt;
!Discussion&lt;br /&gt;
|From the visualisation, it is shown that there is a slightly negative charge on the carbon atoms, and a positive charge of the same magnitude on the hydrogen atoms. All the carbon atoms have the same charge as they are in identical environments. The same applies to all the hydrogen atoms. This is due to the highly symmetrical structure of benzene. Since the same colour scale was used for both benzene and borazine, and the charges are much smaller in magnitude on atoms in benzene than atoms on borazine, the colours on the charge distribution visualisation is much darker. &lt;br /&gt;
|Polar bonds between nitrogen and boron are demonstration from the above visualisation. From the colours displayed on the charge distribution visualisation as well as the charge values, it is shown that nitrogen has a relatively large negative charge, while boron has a positive charge. This is due to the difference in electrogenativity between these atoms: nitrogen atoms are more electronegative than boron and tends to attract electrons towards themselves. It is worth noting that the hydrogen atoms do not all have the same charge. The hydrogen atoms bonded to boron have a slightly negative charge, and the ones bonded to nitrogen have a small positive charge. &lt;br /&gt;
&lt;br /&gt;
The fact that the same colour scale was used for both molecules comes in helpful here. It allows the charges on atoms to be compared directly. For example, just from looking at the colours, one can tell that or example, even though both carbon and nitrogen are electronegative, nitrogen is much more electronegative, which is quantitatively shown by Pauling&#039;s electronegativity scale.&amp;lt;ref&amp;gt;http://www.tutor-homework.com/Chemistry_Help/electronegativity_table/electronegativity.html (Accessed: 24.0502018&amp;lt;/ref&amp;gt;&lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
===Comparative MOs of Benzene and Borazine===&lt;br /&gt;
&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot;&lt;br /&gt;
!&lt;br /&gt;
!Benzene&lt;br /&gt;
!Borazine&lt;br /&gt;
!Comparison and Discussion&lt;br /&gt;
|-&lt;br /&gt;
!1st comparative pair&lt;br /&gt;
|[[File:Hyc116_benzene_1st_MO_pair_7.png|200x200px|centre]]&lt;br /&gt;
|[[File:Hyc116_borazine_1st_MO_pair_level9.png|200x200px|centre]]&lt;br /&gt;
|MO 9 of both benzene and borazine are comparable. They both show delocalised molecular orbital with an overall bonding character. There is a nodal plane across the molecular orbitals for both benzene and borazine. For benzene, there is contribution from all the carbon and hydrogen s orbitals. Moreover, the molecular orbitals are symmetric to their counterpart of opposite phase, giving an E&amp;lt;sub&amp;gt;1g&amp;lt;/sub&amp;gt; MO. That is not the case for borazine; they are less symmetric in borazine. This MO of borazine has an E&#039; symmetry. Nitrogen atoms are more electronegative than boron atoms and pull electron density towards themselves, resulting in a larger lobe. There is contribution from all the boron and nitrogen s orbitals, and three of the hydrogen s orbitals, though not all of them. &lt;br /&gt;
|-&lt;br /&gt;
!2nd comparative pair&lt;br /&gt;
|[[File:Hyc116_benzene_2nd_MO_pair_10.png|200x200px|centre]]&lt;br /&gt;
|[[File:Hyc116_borazine_2nd_MO_pair_level11.png|200x200px|centre]]&lt;br /&gt;
|MO 10 of benzene and MO 11 of borazine are comparable. Here shows a pair of rather delocalised molecular orbitals with slightly more antibonding character than the first pair shown above. On both MOs, there is no contribution from one pair of opposite hydrogen atoms, but contribution from s orbitals of all other atoms on both molecule. The benzene MO has an E&amp;lt;sub&amp;gt;2g&amp;lt;/sub&amp;gt; symmetry. In borazine, the lobes are in different sizes due to the higher electronegativity of nitrogen. The lobes at the nitrogen atoms are larger as they attract electrons towards themselves more so than boron atoms do. This borazine MO has an E&#039; symmetry. &lt;br /&gt;
|-&lt;br /&gt;
!3rd comparative pair&lt;br /&gt;
|[[File:Hyc116_benzene_3rd_MO_pair_21.png|200x200px|centre]]&lt;br /&gt;
|[[File:Hyc116_borazine_3rd_MO_pair_level21.png|200x200px|centre]]&lt;br /&gt;
|The HOMO (MO 21) of benzene and the HOMO (MO 21) of borazine are comparable. They are both made of p orbitals of all carbon atoms (or all boron and nitrogen atoms in the case of borazine); there is no contribution from hydrogen atoms as they do not have p orbitals. There is a nodal plan perpendicular to the z axis (highest rotational axis) and one parallel to the z axis. On benzene, the MO is very symmetric and has an E&amp;lt;sub&amp;gt;1g&amp;lt;/sub&amp;gt; symmetry; the lobes of the MO are the same in size. On borazine, the lobe where there are two nitrogen atoms is bigger in size, again due to the higher electronegtivity of nitrogen compared to boron. The borazine MO has an E&#039; &#039; symmetry.&lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
===Aromaticity: some theories===&lt;br /&gt;
&lt;br /&gt;
Aromatic compounds display properties such as their high stability and bond lengths between typical single and double bonds. A simple understanding of aromaticity involves the overlap of p orbitals perpendicular to the cyclic plane; the delocalisation of electrons on the pi system is identified to be responsible of the stability of aromatic systems. Aromatic compounds can be identified by the Huckel’s rule, which states that conjugated planar cyclic molecules with (4n +2) π electrons are aromatic. Both benzene and borazine obey the Huckel’s rule and fit the conventional description of aromaticity. &lt;br /&gt;
&lt;br /&gt;
However, it is proved in recent years that the conventional criteria do not necessarily have to be obeyed for a compound to be aromatic. For instance, there has been shown that some non-planar compounds display aromaticity. This suggests that the criteria for aromaticity is not simply structural, and these advances give rise to concepts such as quasiaromaticity and pseudoaromaticity. Recent advances show that there are quantum mechanics basis on the idea of aromaticity. &lt;br /&gt;
In conclusion, while the overlap of pi orbitals provides a simple understanding for aromaticity, it is not a sufficient description for aromaticity.&lt;br /&gt;
&lt;br /&gt;
==References==&lt;br /&gt;
{{reflist}}&lt;/div&gt;</summary>
		<author><name>Hyc116</name></author>
	</entry>
	<entry>
		<id>https://chemwiki.ch.ic.ac.uk/index.php?title=MO_hyc116&amp;diff=732301</id>
		<title>MO hyc116</title>
		<link rel="alternate" type="text/html" href="https://chemwiki.ch.ic.ac.uk/index.php?title=MO_hyc116&amp;diff=732301"/>
		<updated>2018-05-25T14:53:10Z</updated>

		<summary type="html">&lt;p&gt;Hyc116: /* Comparative MOs of Benzene and Borazine */&lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;==BH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;==&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;Calculation type&amp;lt;/b&amp;gt;: Optimisation&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;Calculation Method&amp;lt;/b&amp;gt;: B3LYP&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;Basis set&amp;lt;/b&amp;gt;: 6-31G(d,p) &lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Summary table&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
[[file:Hyc116_bh3_631g_opt_summarytable.png]]&lt;br /&gt;
&lt;br /&gt;
The above summary table was obtained after the 2nd optimisation of BH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt; (after the initial optimisation using the 3-21G basis set). Notice how the symmetry is incorrect and shown as Cs. This is because the symmetry was manually broken at the beginning by changing the bond length of B-H bonds. The point group was manually adjusted and the molecule was optimised again before the frequency analysis and the new summary table is attached below.&lt;br /&gt;
&lt;br /&gt;
[[file:Hyc116_bh3_correctsummarytable.png]]&lt;br /&gt;
&lt;br /&gt;
The above summary table was obtained from the optimisation after adjusting the symmetry. The point shown in this summary table is D&amp;lt;sub&amp;gt;3h&amp;lt;/sub&amp;gt;, which is the correct for BH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;. &lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Items table&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
Below is the items table taken from the optimisation with the correct point group.&lt;br /&gt;
&lt;br /&gt;
&amp;lt;pre&amp;gt;&lt;br /&gt;
Item               Value     Threshold  Converged?&lt;br /&gt;
 Maximum Force            0.000015     0.000450     YES&lt;br /&gt;
 RMS     Force            0.000010     0.000300     YES&lt;br /&gt;
 Maximum Displacement     0.000058     0.001800     YES&lt;br /&gt;
 RMS     Displacement     0.000038     0.001200     YES&lt;br /&gt;
&amp;lt;/pre&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Frequency log file&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
[[Media:HYC116 BH3 FREQ.LOG]] &lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Frequencies&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;pre&amp;gt;&lt;br /&gt;
Low frequencies ---  -10.3498   -3.4492   -1.2454   -0.0055    0.4779    3.2165&lt;br /&gt;
Low frequencies --- 1162.9519 1213.1527 1213.1554&lt;br /&gt;
&amp;lt;/pre&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;jmol of BH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;&#039;&#039;&#039;&lt;br /&gt;
&amp;lt;jmol&amp;gt;&amp;lt;jmolApplet&amp;gt;&lt;br /&gt;
  &amp;lt;title&amp;gt;optimised BH3&amp;lt;/title&amp;gt;&lt;br /&gt;
  &amp;lt;color&amp;gt;black&amp;lt;/color&amp;gt;&lt;br /&gt;
  &amp;lt;size&amp;gt;200&amp;lt;/size&amp;gt;&lt;br /&gt;
  &amp;lt;uploadedFileContents&amp;gt;HYC116_BH3_FREQ.LOG&amp;lt;/uploadedFileContents&amp;gt;&lt;br /&gt;
&amp;lt;/jmolApplet&amp;gt;&amp;lt;/jmol&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
===Vibrational spectrum===&lt;br /&gt;
&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot;&lt;br /&gt;
!wavenumber (cm&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;)&lt;br /&gt;
!Intensity (arbitrary units)&lt;br /&gt;
!symmetry&lt;br /&gt;
!IR active?&lt;br /&gt;
!type&lt;br /&gt;
|-&lt;br /&gt;
|1163&lt;br /&gt;
|93&lt;br /&gt;
|A&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;&#039; &#039;&lt;br /&gt;
|Yes&lt;br /&gt;
|Out of plane bend&lt;br /&gt;
|-&lt;br /&gt;
|1213&lt;br /&gt;
|14&lt;br /&gt;
|E&#039;&lt;br /&gt;
|Very slight&lt;br /&gt;
|Bend&lt;br /&gt;
|-&lt;br /&gt;
|1213&lt;br /&gt;
|14&lt;br /&gt;
|E&#039;&lt;br /&gt;
|Very slight&lt;br /&gt;
|Bend&lt;br /&gt;
|-&lt;br /&gt;
|2582&lt;br /&gt;
|0&lt;br /&gt;
|A&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;&#039;&lt;br /&gt;
|No&lt;br /&gt;
|Symmetric stretch&lt;br /&gt;
|-&lt;br /&gt;
|2716&lt;br /&gt;
|126&lt;br /&gt;
|E&#039;&lt;br /&gt;
|Yes&lt;br /&gt;
|Asymmetric stretch&lt;br /&gt;
|-&lt;br /&gt;
|2716&lt;br /&gt;
|126&lt;br /&gt;
|E&#039;&lt;br /&gt;
|Yes&lt;br /&gt;
|Asymmetric stretch&lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;IR spectrum&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
[[file:Hyc116_ir_bh3.png|400*600]]&lt;br /&gt;
&lt;br /&gt;
There are only three peaks on the IR spectrum of BH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;, despite that there are 6 vibrational modes for the molecule. As shown in the table above, the symmetric stretching mode with A1 symmetry at 2582 cm&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt; is not IR active; naturally, that vibrational mode doesn’t give a peak on the IR spectrum. As shown from the table, two pairs of vibrational modes, the bond angle deformation/bend at 1213 cm&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt; and the asymmetric bond stretch at 2716 cm&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;, are degenerate with the symmetry label E. This means that they have the same energy, and hence give the same wavenumber on the IR spectrum. Each pair of degenerate vibrational modes give rise to one peak. This leaves three peaks, as confirmed by the IR spectrum above.&lt;br /&gt;
&lt;br /&gt;
===Molecular orbitals of BH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;===&lt;br /&gt;
&lt;br /&gt;
[[file:hyc116_bh3_MO_diagram.png]]&lt;br /&gt;
&lt;br /&gt;
The above molecular orbital diagram was taken from Dr Patricia Hunt&#039;s &amp;lt;i&amp;gt;Lecture 4 Tutorial Problem Model Answers&amp;lt;/i&amp;gt;.&amp;lt;ref&amp;gt;P. Hunt, &amp;quot;Lecture 4 Tutorial Problem Model Answers&amp;quot;, 2 (2018)&amp;lt;/ref&amp;gt; Diagrams of the &amp;quot;real&amp;quot; MOs were obtained from Gaussian.&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
There is no significant difference between the LCAO MOs and the real ones. Features such as orbital phases are shown clearly on both the LCAO MOs and the real MOs, illustrating the bonding/anti-bonding characters of the molecular orbitals. This suggests that the the qualitative MO theory is highly accurate and useful when studying the molecular orbitals of molecules.&lt;br /&gt;
&lt;br /&gt;
==Associated energies: ammonium borane==&lt;br /&gt;
&lt;br /&gt;
===NH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;===&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;Calculation type&amp;lt;/b&amp;gt;: Optimisation&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;Calculation Method&amp;lt;/b&amp;gt;: B3LYP&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;Basis set&amp;lt;/b&amp;gt;: 6-31G(d,p) &lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Summary table&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
[[file:Hyc116_nh3_631g_summarytable.png]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Items table&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;pre&amp;gt;&lt;br /&gt;
Item               Value     Threshold  Converged?&lt;br /&gt;
 Maximum Force            0.000006     0.000450     YES&lt;br /&gt;
 RMS     Force            0.000004     0.000300     YES&lt;br /&gt;
 Maximum Displacement     0.000012     0.001800     YES&lt;br /&gt;
 RMS     Displacement     0.000008     0.001200     YES&lt;br /&gt;
&amp;lt;/pre&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Frequency log file&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
[[Media:HYC116_NH3_FREQ.LOG]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Frequencies&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;pre&amp;gt;&lt;br /&gt;
Low frequencies ---   -8.5646   -8.5588   -0.0047    0.0454    0.1784   26.4183&lt;br /&gt;
Low frequencies --- 1089.7603 1694.1865 1694.1865&lt;br /&gt;
&amp;lt;/pre&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;jmol of NH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;&#039;&#039;&#039;&lt;br /&gt;
&amp;lt;jmol&amp;gt;&amp;lt;jmolApplet&amp;gt;&lt;br /&gt;
  &amp;lt;title&amp;gt;optimised NH3&amp;lt;/title&amp;gt;&lt;br /&gt;
  &amp;lt;color&amp;gt;black&amp;lt;/color&amp;gt;&lt;br /&gt;
  &amp;lt;size&amp;gt;200&amp;lt;/size&amp;gt;&lt;br /&gt;
  &amp;lt;uploadedFileContents&amp;gt;HYC116_NH3_FREQ.LOG&amp;lt;/uploadedFileContents&amp;gt;&lt;br /&gt;
&amp;lt;/jmolApplet&amp;gt;&amp;lt;/jmol&amp;gt;&lt;br /&gt;
&lt;br /&gt;
===NH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;BH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;===&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;Calculation type&amp;lt;/b&amp;gt;: Optimisation&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;Calculation Method&amp;lt;/b&amp;gt;: B3LYP&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;Basis set&amp;lt;/b&amp;gt;: 6-31G(d,p) &lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Summary table&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
[[file:Hyc116_nh3bh3_631g_summarytable1.png]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Items table&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;pre&amp;gt;&lt;br /&gt;
Item               Value     Threshold  Converged?&lt;br /&gt;
 Maximum Force            0.000121     0.000450     YES&lt;br /&gt;
 RMS     Force            0.000057     0.000300     YES&lt;br /&gt;
 Maximum Displacement     0.000501     0.001800     YES&lt;br /&gt;
 RMS     Displacement     0.000293     0.001200     YES&lt;br /&gt;
&amp;lt;/pre&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Frequency log file&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
[[Media:HYC116_NH3BH3_FREQ1.LOG]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Frequencies&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;pre&amp;gt;&lt;br /&gt;
Low frequencies ---   -0.0574   -0.0501   -0.0074   21.6276   21.6377   40.3839&lt;br /&gt;
Low frequencies ---  265.9973  632.3725  640.1275&lt;br /&gt;
&amp;lt;/pre&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;jmol of NH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;BH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;&#039;&#039;&#039;&lt;br /&gt;
&amp;lt;jmol&amp;gt;&amp;lt;jmolApplet&amp;gt;&lt;br /&gt;
  &amp;lt;title&amp;gt;optimised NH3BH3&amp;lt;/title&amp;gt;&lt;br /&gt;
  &amp;lt;color&amp;gt;black&amp;lt;/color&amp;gt;&lt;br /&gt;
  &amp;lt;size&amp;gt;200&amp;lt;/size&amp;gt;&lt;br /&gt;
  &amp;lt;uploadedFileContents&amp;gt;HYC116_NH3BH3_FREQ.LOG&amp;lt;/uploadedFileContents&amp;gt;&lt;br /&gt;
&amp;lt;/jmolApplet&amp;gt;&amp;lt;/jmol&amp;gt;&lt;br /&gt;
&lt;br /&gt;
===Association energy===&lt;br /&gt;
&lt;br /&gt;
E(BH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;) (using the optimisation with the correct symmetry) = -26.61532363 a.u. = &amp;lt;b&amp;gt;-26.61532 a.u. (5 d.p.)&amp;lt;/b&amp;gt;&lt;br /&gt;
&lt;br /&gt;
E(NH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;) = -56.55776873 a.u. = &amp;lt;b&amp;gt;-56.55777 a.u. (5 d.p.)&amp;lt;/b&amp;gt;&lt;br /&gt;
&lt;br /&gt;
E(NH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;BH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;) = -83.22468892 a.u. = &amp;lt;b&amp;gt;-83.22469 a.u. (5 d.p.)&amp;lt;/b&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
Carrying out calculations using numbers which has already been rounded up can possibly result in errors in the last digit. Hence, here the calculations were carried out using the numbers provided from the optimisations (i.e. with more decimal places than necessary); the answer was then rounded up to the desired accuracy. &lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
ΔE = E(NH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;BH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;)-[E(NH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;)+E(BH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;)]&lt;br /&gt;
&lt;br /&gt;
ΔE = -83.22468892 - (-56.55776873 + -26.61532363) = -0.05159656 a.u. &lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;ΔE = -0.05160 a.u. (5 d.p.)&amp;lt;/b&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Converting energy from a.u. to kJ/mol&#039;&#039;&#039;&lt;br /&gt;
An atomic unit for energy is Hartree, which is equal to 2625.5 kJ/mol.&lt;br /&gt;
&amp;lt;ref&amp;gt;https://cccbdb.nist.gov/hartree.asp (Accessed: 22.05.2018)&amp;lt;/ref&amp;gt;&lt;br /&gt;
 &lt;br /&gt;
&lt;br /&gt;
So ΔE in kJ/mol = -0.05159657 * 2625.5 = -135.46676828 kJ/mol&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;ΔE = -135 kJ/mol (nearest integer)&amp;lt;/b&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
The energy difference calculated above comes from the formation of the B-N dative bond. It is a relatively weak bond. According to a bond energy data sheet provided by the University of California,&amp;lt;ref&amp;gt;https://labs.chem.ucsb.edu/zakarian/armen/11---bonddissociationenergy.pdf (Accessed: 24.05.2018)&amp;lt;/ref&amp;gt;  the bond energy of the C-C bond of an ethane molecule is 368 kJ/mol. This is a fair comparison to the NH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;BH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt; molecule as the two molecules have the same structure, only with the carbon atoms on ethane swapped for Boron and Nitrogen in NH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;BH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;&lt;br /&gt;
&lt;br /&gt;
==Using a mixture of basis-sets and pseudo-potentials==&lt;br /&gt;
&lt;br /&gt;
===BBr&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;===&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;Calculation type&amp;lt;/b&amp;gt;: Optimisation&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;Calculation Method&amp;lt;/b&amp;gt;: B3LYP&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;Basis set&amp;lt;/b&amp;gt;: Boron: 6-31G(d,p) ; Br: LANL2DZ&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
Larger calculations are often sent to a web-server to run on a high-performance computer instead of a desktop. In order to experience and learn to use a web-server, the optimisation and the frequency analysis for BBr&amp;lt;sub&amp;gt;3&amp;lt;/sub were both sent and done on a server instead of the desktop. The calculation results were downloaded from the web-server once they were finished.   &lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Summary table&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
[[file:Hyc116_bbr3_opt_summarytable.png]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Items table&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;pre&amp;gt;&lt;br /&gt;
Item               Value     Threshold  Converged?&lt;br /&gt;
 Maximum Force            0.000008     0.000450     YES&lt;br /&gt;
 RMS     Force            0.000005     0.000300     YES&lt;br /&gt;
 Maximum Displacement     0.000036     0.001800     YES&lt;br /&gt;
 RMS     Displacement     0.000023     0.001200     YES&lt;br /&gt;
&amp;lt;/pre&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Frequency log file&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
[[Media:Hyc116_bbr3_freq.log]]&lt;br /&gt;
&lt;br /&gt;
Attached above is the frequency file saved onto the computer from the SCAN server portal. The frequency file was also published on the chemistry database DSpace. {{DOI|10042/202442}}&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Frequencies&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;pre&amp;gt;&lt;br /&gt;
Low frequencies ---   -0.0137   -0.0064   -0.0046    2.4315    2.4315    4.8421&lt;br /&gt;
Low frequencies ---  155.9631  155.9651  267.7052&lt;br /&gt;
&amp;lt;/pre&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;jmol of BBr&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;&#039;&#039;&#039;&lt;br /&gt;
&amp;lt;jmol&amp;gt;&amp;lt;jmolApplet&amp;gt;&lt;br /&gt;
  &amp;lt;title&amp;gt;optimised BBr3&amp;lt;/title&amp;gt;&lt;br /&gt;
  &amp;lt;color&amp;gt;black&amp;lt;/color&amp;gt;&lt;br /&gt;
  &amp;lt;size&amp;gt;200&amp;lt;/size&amp;gt;&lt;br /&gt;
  &amp;lt;uploadedFileContents&amp;gt;Hyc116_bbr3_freq.log&amp;lt;/uploadedFileContents&amp;gt;&lt;br /&gt;
&amp;lt;/jmolApplet&amp;gt;&amp;lt;/jmol&amp;gt;&lt;br /&gt;
&lt;br /&gt;
==Aromaticity==&lt;br /&gt;
&lt;br /&gt;
===Benzene===&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;Calculation type&amp;lt;/b&amp;gt;: Optimisation&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;Calculation Method&amp;lt;/b&amp;gt;: B3LYP&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;Basis set&amp;lt;/b&amp;gt;: 6-31G(d,p) &lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Summary table&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
[[file:Hyc116_c6h6_summarytable.png]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Items table&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;pre&amp;gt;&lt;br /&gt;
Item               Value     Threshold  Converged?&lt;br /&gt;
 Maximum Force            0.000193     0.000450     YES&lt;br /&gt;
 RMS     Force            0.000079     0.000300     YES&lt;br /&gt;
 Maximum Displacement     0.000830     0.001800     YES&lt;br /&gt;
 RMS     Displacement     0.000294     0.001200     YES&lt;br /&gt;
&amp;lt;/pre&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Frequency log file&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
[[Media:HYC116_C6H6_FREQ.LOG]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Frequencies&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;pre&amp;gt;&lt;br /&gt;
Low frequencies ---   -3.5606   -3.5606   -0.0089   -0.0043   -0.0043   10.0905&lt;br /&gt;
Low frequencies ---  413.9582  413.9582  621.1416&lt;br /&gt;
&amp;lt;/pre&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;jmol of C&amp;lt;sub&amp;gt;6&amp;lt;/sub&amp;gt;H&amp;lt;sub&amp;gt;6&amp;lt;/sub&amp;gt;&#039;&#039;&#039;&lt;br /&gt;
&amp;lt;jmol&amp;gt;&amp;lt;jmolApplet&amp;gt;&lt;br /&gt;
  &amp;lt;title&amp;gt;optimised Benzene&amp;lt;/title&amp;gt;&lt;br /&gt;
  &amp;lt;color&amp;gt;black&amp;lt;/color&amp;gt;&lt;br /&gt;
  &amp;lt;size&amp;gt;200&amp;lt;/size&amp;gt;&lt;br /&gt;
  &amp;lt;uploadedFileContents&amp;gt;HYC116_C6H6_FREQ.LOG&amp;lt;/uploadedFileContents&amp;gt;&lt;br /&gt;
&amp;lt;/jmolApplet&amp;gt;&amp;lt;/jmol&amp;gt;&lt;br /&gt;
&lt;br /&gt;
===Borazine===&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;Calculation type&amp;lt;/b&amp;gt;: Optimisation&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;Calculation Method&amp;lt;/b&amp;gt;: B3LYP&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;Basis set&amp;lt;/b&amp;gt;: 6-31G(d,p) &lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Summary table&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
[[file:Hyc116_borazine_summarytable.png]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Items table&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;pre&amp;gt;&lt;br /&gt;
Item               Value     Threshold  Converged?&lt;br /&gt;
 Maximum Force            0.000085     0.000450     YES&lt;br /&gt;
 RMS     Force            0.000033     0.000300     YES&lt;br /&gt;
 Maximum Displacement     0.000250     0.001800     YES&lt;br /&gt;
 RMS     Displacement     0.000074     0.001200     YES&lt;br /&gt;
&amp;lt;/pre&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Frequency log file&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
[[Media:HYC116_BORAZINE_FREQ.LOG]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Frequencies&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;pre&amp;gt;&lt;br /&gt;
Low frequencies ---  -12.6626  -12.6626   -8.9272   -0.0211   -0.0104   -0.0104&lt;br /&gt;
Low frequencies ---  289.1112  289.1112  403.8613&lt;br /&gt;
&amp;lt;/pre&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;jmol of Borazine&#039;&#039;&#039;&lt;br /&gt;
&amp;lt;jmol&amp;gt;&amp;lt;jmolApplet&amp;gt;&lt;br /&gt;
  &amp;lt;title&amp;gt;optimised Borazine&amp;lt;/title&amp;gt;&lt;br /&gt;
  &amp;lt;color&amp;gt;black&amp;lt;/color&amp;gt;&lt;br /&gt;
  &amp;lt;size&amp;gt;200&amp;lt;/size&amp;gt;&lt;br /&gt;
  &amp;lt;uploadedFileContents&amp;gt;HYC116_BORAZINE_FREQ.LOG&amp;lt;/uploadedFileContents&amp;gt;&lt;br /&gt;
&amp;lt;/jmolApplet&amp;gt;&amp;lt;/jmol&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
===Charge distribution===&lt;br /&gt;
&lt;br /&gt;
An NBO charge analysis was carried out on both the optimised benzene and borazine. Visualisations of the charge distribution are shown in the table below, with the colour range going from -1.102 to 1.102 for both molecule. This large scale was chosen as it allows direct comparison of the charge on any atoms in these two molecules and shows the relative magnitude of charges on all these atoms. Negative charges are shown in red, and positive charges are shown in green. A neutral charge is displayed in black, so the smaller a charge is (positive or negative), the darker its colour representation is. Larger charges are shown in brighter colours. The charges are also displayed on the atoms as numbers with a neutral charge being zero. Negative charges are shown as negative number and positive charges are shown as positive numbers. &lt;br /&gt;
&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot;&lt;br /&gt;
!&lt;br /&gt;
!Benzene&lt;br /&gt;
!Borazine&lt;br /&gt;
|-&lt;br /&gt;
!Visualisation of charge distribution&lt;br /&gt;
|[[File:Hyc116_benzene_charge_distribution1.png|500x500px|thumb|centre|Charge distribution of Benzene visualisation]]&lt;br /&gt;
|[[File:Hyc116_borazine_charge_distribution1.png|500x500px|thumb|centre|Charge distribution of Borazine visualisation]]&lt;br /&gt;
|-&lt;br /&gt;
!Charge &lt;br /&gt;
|Carbon: -0.239&lt;br /&gt;
&lt;br /&gt;
Hydrogen: 0.239&lt;br /&gt;
|Nitrogen: -1.102 &lt;br /&gt;
&lt;br /&gt;
Boron: 0.747&lt;br /&gt;
&lt;br /&gt;
Hydrogen (bonded to N): 0.432&lt;br /&gt;
&lt;br /&gt;
Hydrogen (bonded to B): -0.077&lt;br /&gt;
|-&lt;br /&gt;
!Discussion&lt;br /&gt;
|From the visualisation, it is shown that there is a slightly negative charge on the carbon atoms, and a positive charge of the same magnitude on the hydrogen atoms. All the carbon atoms have the same charge as they are in identical environments. The same applies to all the hydrogen atoms. This is due to the highly symmetrical structure of benzene. Since the same colour scale was used for both benzene and borazine, and the charges are much smaller in magnitude on atoms in benzene than atoms on borazine, the colours on the charge distribution visualisation is much darker. &lt;br /&gt;
|Polar bonds between nitrogen and boron are demonstration from the above visualisation. From the colours displayed on the charge distribution visualisation as well as the charge values, it is shown that nitrogen has a relatively large negative charge, while boron has a positive charge. This is due to the difference in electrogenativity between these atoms: nitrogen atoms are more electronegative than boron and tends to attract electrons towards themselves. It is worth noting that the hydrogen atoms do not all have the same charge. The hydrogen atoms bonded to boron have a slightly negative charge, and the ones bonded to nitrogen have a small positive charge. &lt;br /&gt;
&lt;br /&gt;
The fact that the same colour scale was used for both molecules comes in helpful here. It allows the charges on atoms to be compared directly. For example, just from looking at the colours, one can tell that or example, even though both carbon and nitrogen are electronegative, nitrogen is much more electronegative, which is quantitatively shown by Pauling&#039;s electronegativity scale.&amp;lt;ref&amp;gt;http://www.tutor-homework.com/Chemistry_Help/electronegativity_table/electronegativity.html (Accessed: 24.0502018&amp;lt;/ref&amp;gt;&lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
===Comparative MOs of Benzene and Borazine===&lt;br /&gt;
&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot;&lt;br /&gt;
!&lt;br /&gt;
!Benzene&lt;br /&gt;
!Borazine&lt;br /&gt;
!Comparison and Discussion&lt;br /&gt;
|-&lt;br /&gt;
!1st comparative pair&lt;br /&gt;
|[[File:Hyc116_benzene_1st_MO_pair_7.png|200x200px|centre]]&lt;br /&gt;
|[[File:Hyc116_borazine_1st_MO_pair_level9.png|200x200px|centre]]&lt;br /&gt;
|MO 9 of both benzene and borazine are comparable. They both show delocalised molecular orbital with an overall bonding character. There is a nodal plane across the molecular orbitals for both benzene and borazine. For benzene, there is contribution from all the carbon and hydrogen s orbitals. Moreover, the molecular orbitals are symmetric to their counterpart of opposite phase, giving an E&amp;lt;sub&amp;gt;1g&amp;lt;/sub&amp;gt; MO. That is not the case for borazine; they are less symmetric in borazine. This MO of borazine has an E&#039; symmetry. Nitrogen atoms are more electronegative than boron atoms and pull electron density towards themselves, resulting in a larger lobe. There is contribution from all the boron and nitrogen s orbitals, and three of the hydrogen s orbitals, though not all of them. &lt;br /&gt;
|-&lt;br /&gt;
!2nd comparative pair&lt;br /&gt;
|[[File:Hyc116_benzene_2nd_MO_pair_10.png|200x200px|centre]]&lt;br /&gt;
|[[File:Hyc116_borazine_2nd_MO_pair_level11.png|200x200px|centre]]&lt;br /&gt;
|MO 10 of benzene and MO 11 of borazine are comparable. Here shows a pair of rather delocalised molecular orbitals with slightly more antibonding character than the first pair shown above. On both MOs, there is no contribution from one pair of opposite hydrogen atoms, but contribution from s orbitals of all other atoms on both molecule. The benzene MO has an E&amp;lt;sub&amp;gt;2g&amp;lt;/sub&amp;gt; symmetry. In borazine, the lobes are in different sizes due to the higher electronegativity of nitrogen. The lobes at the nitrogen atoms are larger as they attract electrons towards themselves more so than boron atoms do. This borazine MO has an E&#039; symmetry. &lt;br /&gt;
|-&lt;br /&gt;
!3rd comparative pair&lt;br /&gt;
|[[File:Hyc116_benzene_3rd_MO_pair_21.png|200x200px|centre]]&lt;br /&gt;
|[[File:Hyc116_borazine_3rd_MO_pair_level21.png|200x200px|centre]]&lt;br /&gt;
|The HOMO (MO 21) of benzene and the HOMO (MO 21) of borazine are comparable. They are both made of p orbitals of all carbon atoms (or all boron and nitrogen atoms in the case of borazine); there is no contribution from hydrogen atoms as they do not have p orbitals. There is a nodal plan perpendicular to the z axis (highest rotational axis) and one parallel to the z axis. On benzene, the MO is very symmetric and has an E&amp;lt;sub&amp;gt;1g&amp;lt;/sub&amp;gt; symmetry; the lobes of the MO are the same in size. On borazine, the lobe where there are two nitrogen atoms is bigger in size, again due to the higher electronegtivity of nitrogen compared to boron. The borazine MO has an E&#039;&#039; symmetry.&lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
===Aromaticity: some theories===&lt;br /&gt;
&lt;br /&gt;
Aromatic compounds display properties such as their high stability and bond lengths between typical single and double bonds. A simple understanding of aromaticity involves the overlap of p orbitals perpendicular to the cyclic plane; the delocalisation of electrons on the pi system is identified to be responsible of the stability of aromatic systems. Aromatic compounds can be identified by the Huckel’s rule, which states that conjugated planar cyclic molecules with (4n +2) π electrons are aromatic. Both benzene and borazine obey the Huckel’s rule and fit the conventional description of aromaticity. &lt;br /&gt;
&lt;br /&gt;
However, it is proved in recent years that the conventional criteria do not necessarily have to be obeyed for a compound to be aromatic. For instance, there has been shown that some non-planar compounds display aromaticity. This suggests that the criteria for aromaticity is not simply structural, and these advances give rise to concepts such as quasiaromaticity and pseudoaromaticity. Recent advances show that there are quantum mechanics basis on the idea of aromaticity. &lt;br /&gt;
In conclusion, while the overlap of pi orbitals provides a simple understanding for aromaticity, it is not a sufficient description for aromaticity.&lt;br /&gt;
&lt;br /&gt;
==References==&lt;br /&gt;
{{reflist}}&lt;/div&gt;</summary>
		<author><name>Hyc116</name></author>
	</entry>
	<entry>
		<id>https://chemwiki.ch.ic.ac.uk/index.php?title=MO_hyc116&amp;diff=732273</id>
		<title>MO hyc116</title>
		<link rel="alternate" type="text/html" href="https://chemwiki.ch.ic.ac.uk/index.php?title=MO_hyc116&amp;diff=732273"/>
		<updated>2018-05-25T14:47:59Z</updated>

		<summary type="html">&lt;p&gt;Hyc116: /* Charge distribution */&lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;==BH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;==&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;Calculation type&amp;lt;/b&amp;gt;: Optimisation&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;Calculation Method&amp;lt;/b&amp;gt;: B3LYP&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;Basis set&amp;lt;/b&amp;gt;: 6-31G(d,p) &lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Summary table&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
[[file:Hyc116_bh3_631g_opt_summarytable.png]]&lt;br /&gt;
&lt;br /&gt;
The above summary table was obtained after the 2nd optimisation of BH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt; (after the initial optimisation using the 3-21G basis set). Notice how the symmetry is incorrect and shown as Cs. This is because the symmetry was manually broken at the beginning by changing the bond length of B-H bonds. The point group was manually adjusted and the molecule was optimised again before the frequency analysis and the new summary table is attached below.&lt;br /&gt;
&lt;br /&gt;
[[file:Hyc116_bh3_correctsummarytable.png]]&lt;br /&gt;
&lt;br /&gt;
The above summary table was obtained from the optimisation after adjusting the symmetry. The point shown in this summary table is D&amp;lt;sub&amp;gt;3h&amp;lt;/sub&amp;gt;, which is the correct for BH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;. &lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Items table&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
Below is the items table taken from the optimisation with the correct point group.&lt;br /&gt;
&lt;br /&gt;
&amp;lt;pre&amp;gt;&lt;br /&gt;
Item               Value     Threshold  Converged?&lt;br /&gt;
 Maximum Force            0.000015     0.000450     YES&lt;br /&gt;
 RMS     Force            0.000010     0.000300     YES&lt;br /&gt;
 Maximum Displacement     0.000058     0.001800     YES&lt;br /&gt;
 RMS     Displacement     0.000038     0.001200     YES&lt;br /&gt;
&amp;lt;/pre&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Frequency log file&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
[[Media:HYC116 BH3 FREQ.LOG]] &lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Frequencies&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;pre&amp;gt;&lt;br /&gt;
Low frequencies ---  -10.3498   -3.4492   -1.2454   -0.0055    0.4779    3.2165&lt;br /&gt;
Low frequencies --- 1162.9519 1213.1527 1213.1554&lt;br /&gt;
&amp;lt;/pre&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;jmol of BH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;&#039;&#039;&#039;&lt;br /&gt;
&amp;lt;jmol&amp;gt;&amp;lt;jmolApplet&amp;gt;&lt;br /&gt;
  &amp;lt;title&amp;gt;optimised BH3&amp;lt;/title&amp;gt;&lt;br /&gt;
  &amp;lt;color&amp;gt;black&amp;lt;/color&amp;gt;&lt;br /&gt;
  &amp;lt;size&amp;gt;200&amp;lt;/size&amp;gt;&lt;br /&gt;
  &amp;lt;uploadedFileContents&amp;gt;HYC116_BH3_FREQ.LOG&amp;lt;/uploadedFileContents&amp;gt;&lt;br /&gt;
&amp;lt;/jmolApplet&amp;gt;&amp;lt;/jmol&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
===Vibrational spectrum===&lt;br /&gt;
&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot;&lt;br /&gt;
!wavenumber (cm&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;)&lt;br /&gt;
!Intensity (arbitrary units)&lt;br /&gt;
!symmetry&lt;br /&gt;
!IR active?&lt;br /&gt;
!type&lt;br /&gt;
|-&lt;br /&gt;
|1163&lt;br /&gt;
|93&lt;br /&gt;
|A&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;&#039; &#039;&lt;br /&gt;
|Yes&lt;br /&gt;
|Out of plane bend&lt;br /&gt;
|-&lt;br /&gt;
|1213&lt;br /&gt;
|14&lt;br /&gt;
|E&#039;&lt;br /&gt;
|Very slight&lt;br /&gt;
|Bend&lt;br /&gt;
|-&lt;br /&gt;
|1213&lt;br /&gt;
|14&lt;br /&gt;
|E&#039;&lt;br /&gt;
|Very slight&lt;br /&gt;
|Bend&lt;br /&gt;
|-&lt;br /&gt;
|2582&lt;br /&gt;
|0&lt;br /&gt;
|A&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;&#039;&lt;br /&gt;
|No&lt;br /&gt;
|Symmetric stretch&lt;br /&gt;
|-&lt;br /&gt;
|2716&lt;br /&gt;
|126&lt;br /&gt;
|E&#039;&lt;br /&gt;
|Yes&lt;br /&gt;
|Asymmetric stretch&lt;br /&gt;
|-&lt;br /&gt;
|2716&lt;br /&gt;
|126&lt;br /&gt;
|E&#039;&lt;br /&gt;
|Yes&lt;br /&gt;
|Asymmetric stretch&lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;IR spectrum&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
[[file:Hyc116_ir_bh3.png|400*600]]&lt;br /&gt;
&lt;br /&gt;
There are only three peaks on the IR spectrum of BH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;, despite that there are 6 vibrational modes for the molecule. As shown in the table above, the symmetric stretching mode with A1 symmetry at 2582 cm&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt; is not IR active; naturally, that vibrational mode doesn’t give a peak on the IR spectrum. As shown from the table, two pairs of vibrational modes, the bond angle deformation/bend at 1213 cm&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt; and the asymmetric bond stretch at 2716 cm&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;, are degenerate with the symmetry label E. This means that they have the same energy, and hence give the same wavenumber on the IR spectrum. Each pair of degenerate vibrational modes give rise to one peak. This leaves three peaks, as confirmed by the IR spectrum above.&lt;br /&gt;
&lt;br /&gt;
===Molecular orbitals of BH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;===&lt;br /&gt;
&lt;br /&gt;
[[file:hyc116_bh3_MO_diagram.png]]&lt;br /&gt;
&lt;br /&gt;
The above molecular orbital diagram was taken from Dr Patricia Hunt&#039;s &amp;lt;i&amp;gt;Lecture 4 Tutorial Problem Model Answers&amp;lt;/i&amp;gt;.&amp;lt;ref&amp;gt;P. Hunt, &amp;quot;Lecture 4 Tutorial Problem Model Answers&amp;quot;, 2 (2018)&amp;lt;/ref&amp;gt; Diagrams of the &amp;quot;real&amp;quot; MOs were obtained from Gaussian.&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
There is no significant difference between the LCAO MOs and the real ones. Features such as orbital phases are shown clearly on both the LCAO MOs and the real MOs, illustrating the bonding/anti-bonding characters of the molecular orbitals. This suggests that the the qualitative MO theory is highly accurate and useful when studying the molecular orbitals of molecules.&lt;br /&gt;
&lt;br /&gt;
==Associated energies: ammonium borane==&lt;br /&gt;
&lt;br /&gt;
===NH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;===&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;Calculation type&amp;lt;/b&amp;gt;: Optimisation&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;Calculation Method&amp;lt;/b&amp;gt;: B3LYP&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;Basis set&amp;lt;/b&amp;gt;: 6-31G(d,p) &lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Summary table&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
[[file:Hyc116_nh3_631g_summarytable.png]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Items table&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;pre&amp;gt;&lt;br /&gt;
Item               Value     Threshold  Converged?&lt;br /&gt;
 Maximum Force            0.000006     0.000450     YES&lt;br /&gt;
 RMS     Force            0.000004     0.000300     YES&lt;br /&gt;
 Maximum Displacement     0.000012     0.001800     YES&lt;br /&gt;
 RMS     Displacement     0.000008     0.001200     YES&lt;br /&gt;
&amp;lt;/pre&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Frequency log file&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
[[Media:HYC116_NH3_FREQ.LOG]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Frequencies&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;pre&amp;gt;&lt;br /&gt;
Low frequencies ---   -8.5646   -8.5588   -0.0047    0.0454    0.1784   26.4183&lt;br /&gt;
Low frequencies --- 1089.7603 1694.1865 1694.1865&lt;br /&gt;
&amp;lt;/pre&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;jmol of NH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;&#039;&#039;&#039;&lt;br /&gt;
&amp;lt;jmol&amp;gt;&amp;lt;jmolApplet&amp;gt;&lt;br /&gt;
  &amp;lt;title&amp;gt;optimised NH3&amp;lt;/title&amp;gt;&lt;br /&gt;
  &amp;lt;color&amp;gt;black&amp;lt;/color&amp;gt;&lt;br /&gt;
  &amp;lt;size&amp;gt;200&amp;lt;/size&amp;gt;&lt;br /&gt;
  &amp;lt;uploadedFileContents&amp;gt;HYC116_NH3_FREQ.LOG&amp;lt;/uploadedFileContents&amp;gt;&lt;br /&gt;
&amp;lt;/jmolApplet&amp;gt;&amp;lt;/jmol&amp;gt;&lt;br /&gt;
&lt;br /&gt;
===NH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;BH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;===&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;Calculation type&amp;lt;/b&amp;gt;: Optimisation&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;Calculation Method&amp;lt;/b&amp;gt;: B3LYP&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;Basis set&amp;lt;/b&amp;gt;: 6-31G(d,p) &lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Summary table&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
[[file:Hyc116_nh3bh3_631g_summarytable1.png]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Items table&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;pre&amp;gt;&lt;br /&gt;
Item               Value     Threshold  Converged?&lt;br /&gt;
 Maximum Force            0.000121     0.000450     YES&lt;br /&gt;
 RMS     Force            0.000057     0.000300     YES&lt;br /&gt;
 Maximum Displacement     0.000501     0.001800     YES&lt;br /&gt;
 RMS     Displacement     0.000293     0.001200     YES&lt;br /&gt;
&amp;lt;/pre&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Frequency log file&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
[[Media:HYC116_NH3BH3_FREQ1.LOG]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Frequencies&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;pre&amp;gt;&lt;br /&gt;
Low frequencies ---   -0.0574   -0.0501   -0.0074   21.6276   21.6377   40.3839&lt;br /&gt;
Low frequencies ---  265.9973  632.3725  640.1275&lt;br /&gt;
&amp;lt;/pre&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;jmol of NH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;BH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;&#039;&#039;&#039;&lt;br /&gt;
&amp;lt;jmol&amp;gt;&amp;lt;jmolApplet&amp;gt;&lt;br /&gt;
  &amp;lt;title&amp;gt;optimised NH3BH3&amp;lt;/title&amp;gt;&lt;br /&gt;
  &amp;lt;color&amp;gt;black&amp;lt;/color&amp;gt;&lt;br /&gt;
  &amp;lt;size&amp;gt;200&amp;lt;/size&amp;gt;&lt;br /&gt;
  &amp;lt;uploadedFileContents&amp;gt;HYC116_NH3BH3_FREQ.LOG&amp;lt;/uploadedFileContents&amp;gt;&lt;br /&gt;
&amp;lt;/jmolApplet&amp;gt;&amp;lt;/jmol&amp;gt;&lt;br /&gt;
&lt;br /&gt;
===Association energy===&lt;br /&gt;
&lt;br /&gt;
E(BH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;) (using the optimisation with the correct symmetry) = -26.61532363 a.u. = &amp;lt;b&amp;gt;-26.61532 a.u. (5 d.p.)&amp;lt;/b&amp;gt;&lt;br /&gt;
&lt;br /&gt;
E(NH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;) = -56.55776873 a.u. = &amp;lt;b&amp;gt;-56.55777 a.u. (5 d.p.)&amp;lt;/b&amp;gt;&lt;br /&gt;
&lt;br /&gt;
E(NH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;BH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;) = -83.22468892 a.u. = &amp;lt;b&amp;gt;-83.22469 a.u. (5 d.p.)&amp;lt;/b&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
Carrying out calculations using numbers which has already been rounded up can possibly result in errors in the last digit. Hence, here the calculations were carried out using the numbers provided from the optimisations (i.e. with more decimal places than necessary); the answer was then rounded up to the desired accuracy. &lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
ΔE = E(NH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;BH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;)-[E(NH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;)+E(BH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;)]&lt;br /&gt;
&lt;br /&gt;
ΔE = -83.22468892 - (-56.55776873 + -26.61532363) = -0.05159656 a.u. &lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;ΔE = -0.05160 a.u. (5 d.p.)&amp;lt;/b&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Converting energy from a.u. to kJ/mol&#039;&#039;&#039;&lt;br /&gt;
An atomic unit for energy is Hartree, which is equal to 2625.5 kJ/mol.&lt;br /&gt;
&amp;lt;ref&amp;gt;https://cccbdb.nist.gov/hartree.asp (Accessed: 22.05.2018)&amp;lt;/ref&amp;gt;&lt;br /&gt;
 &lt;br /&gt;
&lt;br /&gt;
So ΔE in kJ/mol = -0.05159657 * 2625.5 = -135.46676828 kJ/mol&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;ΔE = -135 kJ/mol (nearest integer)&amp;lt;/b&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
The energy difference calculated above comes from the formation of the B-N dative bond. It is a relatively weak bond. According to a bond energy data sheet provided by the University of California,&amp;lt;ref&amp;gt;https://labs.chem.ucsb.edu/zakarian/armen/11---bonddissociationenergy.pdf (Accessed: 24.05.2018)&amp;lt;/ref&amp;gt;  the bond energy of the C-C bond of an ethane molecule is 368 kJ/mol. This is a fair comparison to the NH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;BH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt; molecule as the two molecules have the same structure, only with the carbon atoms on ethane swapped for Boron and Nitrogen in NH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;BH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;&lt;br /&gt;
&lt;br /&gt;
==Using a mixture of basis-sets and pseudo-potentials==&lt;br /&gt;
&lt;br /&gt;
===BBr&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;===&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;Calculation type&amp;lt;/b&amp;gt;: Optimisation&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;Calculation Method&amp;lt;/b&amp;gt;: B3LYP&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;Basis set&amp;lt;/b&amp;gt;: Boron: 6-31G(d,p) ; Br: LANL2DZ&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
Larger calculations are often sent to a web-server to run on a high-performance computer instead of a desktop. In order to experience and learn to use a web-server, the optimisation and the frequency analysis for BBr&amp;lt;sub&amp;gt;3&amp;lt;/sub were both sent and done on a server instead of the desktop. The calculation results were downloaded from the web-server once they were finished.   &lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Summary table&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
[[file:Hyc116_bbr3_opt_summarytable.png]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Items table&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;pre&amp;gt;&lt;br /&gt;
Item               Value     Threshold  Converged?&lt;br /&gt;
 Maximum Force            0.000008     0.000450     YES&lt;br /&gt;
 RMS     Force            0.000005     0.000300     YES&lt;br /&gt;
 Maximum Displacement     0.000036     0.001800     YES&lt;br /&gt;
 RMS     Displacement     0.000023     0.001200     YES&lt;br /&gt;
&amp;lt;/pre&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Frequency log file&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
[[Media:Hyc116_bbr3_freq.log]]&lt;br /&gt;
&lt;br /&gt;
Attached above is the frequency file saved onto the computer from the SCAN server portal. The frequency file was also published on the chemistry database DSpace. {{DOI|10042/202442}}&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Frequencies&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;pre&amp;gt;&lt;br /&gt;
Low frequencies ---   -0.0137   -0.0064   -0.0046    2.4315    2.4315    4.8421&lt;br /&gt;
Low frequencies ---  155.9631  155.9651  267.7052&lt;br /&gt;
&amp;lt;/pre&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;jmol of BBr&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;&#039;&#039;&#039;&lt;br /&gt;
&amp;lt;jmol&amp;gt;&amp;lt;jmolApplet&amp;gt;&lt;br /&gt;
  &amp;lt;title&amp;gt;optimised BBr3&amp;lt;/title&amp;gt;&lt;br /&gt;
  &amp;lt;color&amp;gt;black&amp;lt;/color&amp;gt;&lt;br /&gt;
  &amp;lt;size&amp;gt;200&amp;lt;/size&amp;gt;&lt;br /&gt;
  &amp;lt;uploadedFileContents&amp;gt;Hyc116_bbr3_freq.log&amp;lt;/uploadedFileContents&amp;gt;&lt;br /&gt;
&amp;lt;/jmolApplet&amp;gt;&amp;lt;/jmol&amp;gt;&lt;br /&gt;
&lt;br /&gt;
==Aromaticity==&lt;br /&gt;
&lt;br /&gt;
===Benzene===&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;Calculation type&amp;lt;/b&amp;gt;: Optimisation&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;Calculation Method&amp;lt;/b&amp;gt;: B3LYP&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;Basis set&amp;lt;/b&amp;gt;: 6-31G(d,p) &lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Summary table&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
[[file:Hyc116_c6h6_summarytable.png]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Items table&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;pre&amp;gt;&lt;br /&gt;
Item               Value     Threshold  Converged?&lt;br /&gt;
 Maximum Force            0.000193     0.000450     YES&lt;br /&gt;
 RMS     Force            0.000079     0.000300     YES&lt;br /&gt;
 Maximum Displacement     0.000830     0.001800     YES&lt;br /&gt;
 RMS     Displacement     0.000294     0.001200     YES&lt;br /&gt;
&amp;lt;/pre&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Frequency log file&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
[[Media:HYC116_C6H6_FREQ.LOG]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Frequencies&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;pre&amp;gt;&lt;br /&gt;
Low frequencies ---   -3.5606   -3.5606   -0.0089   -0.0043   -0.0043   10.0905&lt;br /&gt;
Low frequencies ---  413.9582  413.9582  621.1416&lt;br /&gt;
&amp;lt;/pre&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;jmol of C&amp;lt;sub&amp;gt;6&amp;lt;/sub&amp;gt;H&amp;lt;sub&amp;gt;6&amp;lt;/sub&amp;gt;&#039;&#039;&#039;&lt;br /&gt;
&amp;lt;jmol&amp;gt;&amp;lt;jmolApplet&amp;gt;&lt;br /&gt;
  &amp;lt;title&amp;gt;optimised Benzene&amp;lt;/title&amp;gt;&lt;br /&gt;
  &amp;lt;color&amp;gt;black&amp;lt;/color&amp;gt;&lt;br /&gt;
  &amp;lt;size&amp;gt;200&amp;lt;/size&amp;gt;&lt;br /&gt;
  &amp;lt;uploadedFileContents&amp;gt;HYC116_C6H6_FREQ.LOG&amp;lt;/uploadedFileContents&amp;gt;&lt;br /&gt;
&amp;lt;/jmolApplet&amp;gt;&amp;lt;/jmol&amp;gt;&lt;br /&gt;
&lt;br /&gt;
===Borazine===&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;Calculation type&amp;lt;/b&amp;gt;: Optimisation&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;Calculation Method&amp;lt;/b&amp;gt;: B3LYP&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;Basis set&amp;lt;/b&amp;gt;: 6-31G(d,p) &lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Summary table&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
[[file:Hyc116_borazine_summarytable.png]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Items table&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;pre&amp;gt;&lt;br /&gt;
Item               Value     Threshold  Converged?&lt;br /&gt;
 Maximum Force            0.000085     0.000450     YES&lt;br /&gt;
 RMS     Force            0.000033     0.000300     YES&lt;br /&gt;
 Maximum Displacement     0.000250     0.001800     YES&lt;br /&gt;
 RMS     Displacement     0.000074     0.001200     YES&lt;br /&gt;
&amp;lt;/pre&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Frequency log file&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
[[Media:HYC116_BORAZINE_FREQ.LOG]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Frequencies&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;pre&amp;gt;&lt;br /&gt;
Low frequencies ---  -12.6626  -12.6626   -8.9272   -0.0211   -0.0104   -0.0104&lt;br /&gt;
Low frequencies ---  289.1112  289.1112  403.8613&lt;br /&gt;
&amp;lt;/pre&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;jmol of Borazine&#039;&#039;&#039;&lt;br /&gt;
&amp;lt;jmol&amp;gt;&amp;lt;jmolApplet&amp;gt;&lt;br /&gt;
  &amp;lt;title&amp;gt;optimised Borazine&amp;lt;/title&amp;gt;&lt;br /&gt;
  &amp;lt;color&amp;gt;black&amp;lt;/color&amp;gt;&lt;br /&gt;
  &amp;lt;size&amp;gt;200&amp;lt;/size&amp;gt;&lt;br /&gt;
  &amp;lt;uploadedFileContents&amp;gt;HYC116_BORAZINE_FREQ.LOG&amp;lt;/uploadedFileContents&amp;gt;&lt;br /&gt;
&amp;lt;/jmolApplet&amp;gt;&amp;lt;/jmol&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
===Charge distribution===&lt;br /&gt;
&lt;br /&gt;
An NBO charge analysis was carried out on both the optimised benzene and borazine. Visualisations of the charge distribution are shown in the table below, with the colour range going from -1.102 to 1.102 for both molecule. This large scale was chosen as it allows direct comparison of the charge on any atoms in these two molecules and shows the relative magnitude of charges on all these atoms. Negative charges are shown in red, and positive charges are shown in green. A neutral charge is displayed in black, so the smaller a charge is (positive or negative), the darker its colour representation is. Larger charges are shown in brighter colours. The charges are also displayed on the atoms as numbers with a neutral charge being zero. Negative charges are shown as negative number and positive charges are shown as positive numbers. &lt;br /&gt;
&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot;&lt;br /&gt;
!&lt;br /&gt;
!Benzene&lt;br /&gt;
!Borazine&lt;br /&gt;
|-&lt;br /&gt;
!Visualisation of charge distribution&lt;br /&gt;
|[[File:Hyc116_benzene_charge_distribution1.png|500x500px|thumb|centre|Charge distribution of Benzene visualisation]]&lt;br /&gt;
|[[File:Hyc116_borazine_charge_distribution1.png|500x500px|thumb|centre|Charge distribution of Borazine visualisation]]&lt;br /&gt;
|-&lt;br /&gt;
!Charge &lt;br /&gt;
|Carbon: -0.239&lt;br /&gt;
&lt;br /&gt;
Hydrogen: 0.239&lt;br /&gt;
|Nitrogen: -1.102 &lt;br /&gt;
&lt;br /&gt;
Boron: 0.747&lt;br /&gt;
&lt;br /&gt;
Hydrogen (bonded to N): 0.432&lt;br /&gt;
&lt;br /&gt;
Hydrogen (bonded to B): -0.077&lt;br /&gt;
|-&lt;br /&gt;
!Discussion&lt;br /&gt;
|From the visualisation, it is shown that there is a slightly negative charge on the carbon atoms, and a positive charge of the same magnitude on the hydrogen atoms. All the carbon atoms have the same charge as they are in identical environments. The same applies to all the hydrogen atoms. This is due to the highly symmetrical structure of benzene. Since the same colour scale was used for both benzene and borazine, and the charges are much smaller in magnitude on atoms in benzene than atoms on borazine, the colours on the charge distribution visualisation is much darker. &lt;br /&gt;
|Polar bonds between nitrogen and boron are demonstration from the above visualisation. From the colours displayed on the charge distribution visualisation as well as the charge values, it is shown that nitrogen has a relatively large negative charge, while boron has a positive charge. This is due to the difference in electrogenativity between these atoms: nitrogen atoms are more electronegative than boron and tends to attract electrons towards themselves. It is worth noting that the hydrogen atoms do not all have the same charge. The hydrogen atoms bonded to boron have a slightly negative charge, and the ones bonded to nitrogen have a small positive charge. &lt;br /&gt;
&lt;br /&gt;
The fact that the same colour scale was used for both molecules comes in helpful here. It allows the charges on atoms to be compared directly. For example, just from looking at the colours, one can tell that or example, even though both carbon and nitrogen are electronegative, nitrogen is much more electronegative, which is quantitatively shown by Pauling&#039;s electronegativity scale.&amp;lt;ref&amp;gt;http://www.tutor-homework.com/Chemistry_Help/electronegativity_table/electronegativity.html (Accessed: 24.0502018&amp;lt;/ref&amp;gt;&lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
===Comparative MOs of Benzene and Borazine===&lt;br /&gt;
&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot;&lt;br /&gt;
!&lt;br /&gt;
!Benzene&lt;br /&gt;
!Borazine&lt;br /&gt;
!Comparison and Discussion&lt;br /&gt;
|-&lt;br /&gt;
!1st comparative pair&lt;br /&gt;
|[[File:Hyc116_benzene_1st_MO_pair_7.png|200x200px|centre]]&lt;br /&gt;
|[[File:Hyc116_borazine_1st_MO_pair_level9.png|200x200px|centre]]&lt;br /&gt;
|MO 9 of both benzene and borazine are comparable. They both show delocalised molecular orbital with an overall bonding character. There is a nodal plane across the molecular orbitals for both benzene and borazine. For benzene, there is contribution from all the carbon and hydrogen s orbitals. Moreover, the molecular orbitals are symmetric to their counterpart of opposite phase, giving an E&amp;lt;sub&amp;gt;1g&amp;lt;/sub&amp;gt; MO. That is not the case for borazine; they are less symmetric in borazine. Nitrogen atoms are more electronegative than boron atoms and pull electron density towards themselves, resulting in a larger MO. There is contribution from all the boron and nitrogen s orbitals, and three of the hydrogen s orbitals, though not all of them. &lt;br /&gt;
|-&lt;br /&gt;
!2nd comparative pair&lt;br /&gt;
|[[File:Hyc116_benzene_2nd_MO_pair_10.png|200x200px|centre]]&lt;br /&gt;
|[[File:Hyc116_borazine_2nd_MO_pair_level11.png|200x200px|centre]]&lt;br /&gt;
|MO 10 of benzene and MO 11 of borazine are comparable. Here shows a pair of rather delocalised molecular orbitals with slightly more antibonding character than the first pair shown above. On both MOs, there is no contribution from one pair of opposite hydrogen atoms, but contribution from s orbitals of all other atoms on both molecule. The benzene MO has an E&amp;lt;sub&amp;gt;2g&amp;lt;/sub&amp;gt; symmetry. In borazine, the lobes are in different sizes due to the higher electronegativity of nitrogen. The lobes at the nitrogen atoms are larger as they attract electrons towards themselves more so than boron atoms do. &lt;br /&gt;
|-&lt;br /&gt;
!3rd comparative pair&lt;br /&gt;
|[[File:Hyc116_benzene_3rd_MO_pair_21.png|200x200px|centre]]&lt;br /&gt;
|[[File:Hyc116_borazine_3rd_MO_pair_level21.png|200x200px|centre]]&lt;br /&gt;
|The HOMO (MO 21) of benzene and the HOMO (MO 21) of borazine are comparable. They are both made of p orbitals of all carbon atoms (or all boron and nitrogen atoms in the case of borazine); there is no contribution from hydrogen atoms as they do not have p orbitals. There is a nodal plan perpendicular to the z axis (highest rotational axis) and one parallel to the z axis. On benzene, the MO is very symmetric and has an E&amp;lt;sub&amp;gt;1g&amp;lt;/sub&amp;gt; symmetry; the lobes of the MO are the same in size. On borazine, the lobe where there are two nitrogen atoms is bigger in size, again due to the higher electronegtivity of nitrogen compared to boron. &lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
===Aromaticity: some theories===&lt;br /&gt;
&lt;br /&gt;
Aromatic compounds display properties such as their high stability and bond lengths between typical single and double bonds. A simple understanding of aromaticity involves the overlap of p orbitals perpendicular to the cyclic plane; the delocalisation of electrons on the pi system is identified to be responsible of the stability of aromatic systems. Aromatic compounds can be identified by the Huckel’s rule, which states that conjugated planar cyclic molecules with (4n +2) π electrons are aromatic. Both benzene and borazine obey the Huckel’s rule and fit the conventional description of aromaticity. &lt;br /&gt;
&lt;br /&gt;
However, it is proved in recent years that the conventional criteria do not necessarily have to be obeyed for a compound to be aromatic. For instance, there has been shown that some non-planar compounds display aromaticity. This suggests that the criteria for aromaticity is not simply structural, and these advances give rise to concepts such as quasiaromaticity and pseudoaromaticity. Recent advances show that there are quantum mechanics basis on the idea of aromaticity. &lt;br /&gt;
In conclusion, while the overlap of pi orbitals provides a simple understanding for aromaticity, it is not a sufficient description for aromaticity.&lt;br /&gt;
&lt;br /&gt;
==References==&lt;br /&gt;
{{reflist}}&lt;/div&gt;</summary>
		<author><name>Hyc116</name></author>
	</entry>
	<entry>
		<id>https://chemwiki.ch.ic.ac.uk/index.php?title=MO_hyc116&amp;diff=732262</id>
		<title>MO hyc116</title>
		<link rel="alternate" type="text/html" href="https://chemwiki.ch.ic.ac.uk/index.php?title=MO_hyc116&amp;diff=732262"/>
		<updated>2018-05-25T14:46:44Z</updated>

		<summary type="html">&lt;p&gt;Hyc116: /* Aromaticity: some theories */&lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;==BH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;==&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;Calculation type&amp;lt;/b&amp;gt;: Optimisation&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;Calculation Method&amp;lt;/b&amp;gt;: B3LYP&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;Basis set&amp;lt;/b&amp;gt;: 6-31G(d,p) &lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Summary table&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
[[file:Hyc116_bh3_631g_opt_summarytable.png]]&lt;br /&gt;
&lt;br /&gt;
The above summary table was obtained after the 2nd optimisation of BH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt; (after the initial optimisation using the 3-21G basis set). Notice how the symmetry is incorrect and shown as Cs. This is because the symmetry was manually broken at the beginning by changing the bond length of B-H bonds. The point group was manually adjusted and the molecule was optimised again before the frequency analysis and the new summary table is attached below.&lt;br /&gt;
&lt;br /&gt;
[[file:Hyc116_bh3_correctsummarytable.png]]&lt;br /&gt;
&lt;br /&gt;
The above summary table was obtained from the optimisation after adjusting the symmetry. The point shown in this summary table is D&amp;lt;sub&amp;gt;3h&amp;lt;/sub&amp;gt;, which is the correct for BH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;. &lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Items table&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
Below is the items table taken from the optimisation with the correct point group.&lt;br /&gt;
&lt;br /&gt;
&amp;lt;pre&amp;gt;&lt;br /&gt;
Item               Value     Threshold  Converged?&lt;br /&gt;
 Maximum Force            0.000015     0.000450     YES&lt;br /&gt;
 RMS     Force            0.000010     0.000300     YES&lt;br /&gt;
 Maximum Displacement     0.000058     0.001800     YES&lt;br /&gt;
 RMS     Displacement     0.000038     0.001200     YES&lt;br /&gt;
&amp;lt;/pre&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Frequency log file&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
[[Media:HYC116 BH3 FREQ.LOG]] &lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Frequencies&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;pre&amp;gt;&lt;br /&gt;
Low frequencies ---  -10.3498   -3.4492   -1.2454   -0.0055    0.4779    3.2165&lt;br /&gt;
Low frequencies --- 1162.9519 1213.1527 1213.1554&lt;br /&gt;
&amp;lt;/pre&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;jmol of BH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;&#039;&#039;&#039;&lt;br /&gt;
&amp;lt;jmol&amp;gt;&amp;lt;jmolApplet&amp;gt;&lt;br /&gt;
  &amp;lt;title&amp;gt;optimised BH3&amp;lt;/title&amp;gt;&lt;br /&gt;
  &amp;lt;color&amp;gt;black&amp;lt;/color&amp;gt;&lt;br /&gt;
  &amp;lt;size&amp;gt;200&amp;lt;/size&amp;gt;&lt;br /&gt;
  &amp;lt;uploadedFileContents&amp;gt;HYC116_BH3_FREQ.LOG&amp;lt;/uploadedFileContents&amp;gt;&lt;br /&gt;
&amp;lt;/jmolApplet&amp;gt;&amp;lt;/jmol&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
===Vibrational spectrum===&lt;br /&gt;
&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot;&lt;br /&gt;
!wavenumber (cm&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;)&lt;br /&gt;
!Intensity (arbitrary units)&lt;br /&gt;
!symmetry&lt;br /&gt;
!IR active?&lt;br /&gt;
!type&lt;br /&gt;
|-&lt;br /&gt;
|1163&lt;br /&gt;
|93&lt;br /&gt;
|A&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;&#039; &#039;&lt;br /&gt;
|Yes&lt;br /&gt;
|Out of plane bend&lt;br /&gt;
|-&lt;br /&gt;
|1213&lt;br /&gt;
|14&lt;br /&gt;
|E&#039;&lt;br /&gt;
|Very slight&lt;br /&gt;
|Bend&lt;br /&gt;
|-&lt;br /&gt;
|1213&lt;br /&gt;
|14&lt;br /&gt;
|E&#039;&lt;br /&gt;
|Very slight&lt;br /&gt;
|Bend&lt;br /&gt;
|-&lt;br /&gt;
|2582&lt;br /&gt;
|0&lt;br /&gt;
|A&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;&#039;&lt;br /&gt;
|No&lt;br /&gt;
|Symmetric stretch&lt;br /&gt;
|-&lt;br /&gt;
|2716&lt;br /&gt;
|126&lt;br /&gt;
|E&#039;&lt;br /&gt;
|Yes&lt;br /&gt;
|Asymmetric stretch&lt;br /&gt;
|-&lt;br /&gt;
|2716&lt;br /&gt;
|126&lt;br /&gt;
|E&#039;&lt;br /&gt;
|Yes&lt;br /&gt;
|Asymmetric stretch&lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;IR spectrum&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
[[file:Hyc116_ir_bh3.png|400*600]]&lt;br /&gt;
&lt;br /&gt;
There are only three peaks on the IR spectrum of BH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;, despite that there are 6 vibrational modes for the molecule. As shown in the table above, the symmetric stretching mode with A1 symmetry at 2582 cm&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt; is not IR active; naturally, that vibrational mode doesn’t give a peak on the IR spectrum. As shown from the table, two pairs of vibrational modes, the bond angle deformation/bend at 1213 cm&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt; and the asymmetric bond stretch at 2716 cm&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;, are degenerate with the symmetry label E. This means that they have the same energy, and hence give the same wavenumber on the IR spectrum. Each pair of degenerate vibrational modes give rise to one peak. This leaves three peaks, as confirmed by the IR spectrum above.&lt;br /&gt;
&lt;br /&gt;
===Molecular orbitals of BH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;===&lt;br /&gt;
&lt;br /&gt;
[[file:hyc116_bh3_MO_diagram.png]]&lt;br /&gt;
&lt;br /&gt;
The above molecular orbital diagram was taken from Dr Patricia Hunt&#039;s &amp;lt;i&amp;gt;Lecture 4 Tutorial Problem Model Answers&amp;lt;/i&amp;gt;.&amp;lt;ref&amp;gt;P. Hunt, &amp;quot;Lecture 4 Tutorial Problem Model Answers&amp;quot;, 2 (2018)&amp;lt;/ref&amp;gt; Diagrams of the &amp;quot;real&amp;quot; MOs were obtained from Gaussian.&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
There is no significant difference between the LCAO MOs and the real ones. Features such as orbital phases are shown clearly on both the LCAO MOs and the real MOs, illustrating the bonding/anti-bonding characters of the molecular orbitals. This suggests that the the qualitative MO theory is highly accurate and useful when studying the molecular orbitals of molecules.&lt;br /&gt;
&lt;br /&gt;
==Associated energies: ammonium borane==&lt;br /&gt;
&lt;br /&gt;
===NH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;===&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;Calculation type&amp;lt;/b&amp;gt;: Optimisation&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;Calculation Method&amp;lt;/b&amp;gt;: B3LYP&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;Basis set&amp;lt;/b&amp;gt;: 6-31G(d,p) &lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Summary table&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
[[file:Hyc116_nh3_631g_summarytable.png]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Items table&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;pre&amp;gt;&lt;br /&gt;
Item               Value     Threshold  Converged?&lt;br /&gt;
 Maximum Force            0.000006     0.000450     YES&lt;br /&gt;
 RMS     Force            0.000004     0.000300     YES&lt;br /&gt;
 Maximum Displacement     0.000012     0.001800     YES&lt;br /&gt;
 RMS     Displacement     0.000008     0.001200     YES&lt;br /&gt;
&amp;lt;/pre&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Frequency log file&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
[[Media:HYC116_NH3_FREQ.LOG]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Frequencies&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;pre&amp;gt;&lt;br /&gt;
Low frequencies ---   -8.5646   -8.5588   -0.0047    0.0454    0.1784   26.4183&lt;br /&gt;
Low frequencies --- 1089.7603 1694.1865 1694.1865&lt;br /&gt;
&amp;lt;/pre&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;jmol of NH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;&#039;&#039;&#039;&lt;br /&gt;
&amp;lt;jmol&amp;gt;&amp;lt;jmolApplet&amp;gt;&lt;br /&gt;
  &amp;lt;title&amp;gt;optimised NH3&amp;lt;/title&amp;gt;&lt;br /&gt;
  &amp;lt;color&amp;gt;black&amp;lt;/color&amp;gt;&lt;br /&gt;
  &amp;lt;size&amp;gt;200&amp;lt;/size&amp;gt;&lt;br /&gt;
  &amp;lt;uploadedFileContents&amp;gt;HYC116_NH3_FREQ.LOG&amp;lt;/uploadedFileContents&amp;gt;&lt;br /&gt;
&amp;lt;/jmolApplet&amp;gt;&amp;lt;/jmol&amp;gt;&lt;br /&gt;
&lt;br /&gt;
===NH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;BH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;===&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;Calculation type&amp;lt;/b&amp;gt;: Optimisation&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;Calculation Method&amp;lt;/b&amp;gt;: B3LYP&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;Basis set&amp;lt;/b&amp;gt;: 6-31G(d,p) &lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Summary table&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
[[file:Hyc116_nh3bh3_631g_summarytable1.png]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Items table&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;pre&amp;gt;&lt;br /&gt;
Item               Value     Threshold  Converged?&lt;br /&gt;
 Maximum Force            0.000121     0.000450     YES&lt;br /&gt;
 RMS     Force            0.000057     0.000300     YES&lt;br /&gt;
 Maximum Displacement     0.000501     0.001800     YES&lt;br /&gt;
 RMS     Displacement     0.000293     0.001200     YES&lt;br /&gt;
&amp;lt;/pre&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Frequency log file&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
[[Media:HYC116_NH3BH3_FREQ1.LOG]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Frequencies&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;pre&amp;gt;&lt;br /&gt;
Low frequencies ---   -0.0574   -0.0501   -0.0074   21.6276   21.6377   40.3839&lt;br /&gt;
Low frequencies ---  265.9973  632.3725  640.1275&lt;br /&gt;
&amp;lt;/pre&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;jmol of NH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;BH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;&#039;&#039;&#039;&lt;br /&gt;
&amp;lt;jmol&amp;gt;&amp;lt;jmolApplet&amp;gt;&lt;br /&gt;
  &amp;lt;title&amp;gt;optimised NH3BH3&amp;lt;/title&amp;gt;&lt;br /&gt;
  &amp;lt;color&amp;gt;black&amp;lt;/color&amp;gt;&lt;br /&gt;
  &amp;lt;size&amp;gt;200&amp;lt;/size&amp;gt;&lt;br /&gt;
  &amp;lt;uploadedFileContents&amp;gt;HYC116_NH3BH3_FREQ.LOG&amp;lt;/uploadedFileContents&amp;gt;&lt;br /&gt;
&amp;lt;/jmolApplet&amp;gt;&amp;lt;/jmol&amp;gt;&lt;br /&gt;
&lt;br /&gt;
===Association energy===&lt;br /&gt;
&lt;br /&gt;
E(BH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;) (using the optimisation with the correct symmetry) = -26.61532363 a.u. = &amp;lt;b&amp;gt;-26.61532 a.u. (5 d.p.)&amp;lt;/b&amp;gt;&lt;br /&gt;
&lt;br /&gt;
E(NH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;) = -56.55776873 a.u. = &amp;lt;b&amp;gt;-56.55777 a.u. (5 d.p.)&amp;lt;/b&amp;gt;&lt;br /&gt;
&lt;br /&gt;
E(NH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;BH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;) = -83.22468892 a.u. = &amp;lt;b&amp;gt;-83.22469 a.u. (5 d.p.)&amp;lt;/b&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
Carrying out calculations using numbers which has already been rounded up can possibly result in errors in the last digit. Hence, here the calculations were carried out using the numbers provided from the optimisations (i.e. with more decimal places than necessary); the answer was then rounded up to the desired accuracy. &lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
ΔE = E(NH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;BH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;)-[E(NH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;)+E(BH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;)]&lt;br /&gt;
&lt;br /&gt;
ΔE = -83.22468892 - (-56.55776873 + -26.61532363) = -0.05159656 a.u. &lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;ΔE = -0.05160 a.u. (5 d.p.)&amp;lt;/b&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Converting energy from a.u. to kJ/mol&#039;&#039;&#039;&lt;br /&gt;
An atomic unit for energy is Hartree, which is equal to 2625.5 kJ/mol.&lt;br /&gt;
&amp;lt;ref&amp;gt;https://cccbdb.nist.gov/hartree.asp (Accessed: 22.05.2018)&amp;lt;/ref&amp;gt;&lt;br /&gt;
 &lt;br /&gt;
&lt;br /&gt;
So ΔE in kJ/mol = -0.05159657 * 2625.5 = -135.46676828 kJ/mol&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;ΔE = -135 kJ/mol (nearest integer)&amp;lt;/b&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
The energy difference calculated above comes from the formation of the B-N dative bond. It is a relatively weak bond. According to a bond energy data sheet provided by the University of California,&amp;lt;ref&amp;gt;https://labs.chem.ucsb.edu/zakarian/armen/11---bonddissociationenergy.pdf (Accessed: 24.05.2018)&amp;lt;/ref&amp;gt;  the bond energy of the C-C bond of an ethane molecule is 368 kJ/mol. This is a fair comparison to the NH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;BH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt; molecule as the two molecules have the same structure, only with the carbon atoms on ethane swapped for Boron and Nitrogen in NH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;BH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;&lt;br /&gt;
&lt;br /&gt;
==Using a mixture of basis-sets and pseudo-potentials==&lt;br /&gt;
&lt;br /&gt;
===BBr&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;===&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;Calculation type&amp;lt;/b&amp;gt;: Optimisation&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;Calculation Method&amp;lt;/b&amp;gt;: B3LYP&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;Basis set&amp;lt;/b&amp;gt;: Boron: 6-31G(d,p) ; Br: LANL2DZ&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
Larger calculations are often sent to a web-server to run on a high-performance computer instead of a desktop. In order to experience and learn to use a web-server, the optimisation and the frequency analysis for BBr&amp;lt;sub&amp;gt;3&amp;lt;/sub were both sent and done on a server instead of the desktop. The calculation results were downloaded from the web-server once they were finished.   &lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Summary table&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
[[file:Hyc116_bbr3_opt_summarytable.png]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Items table&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;pre&amp;gt;&lt;br /&gt;
Item               Value     Threshold  Converged?&lt;br /&gt;
 Maximum Force            0.000008     0.000450     YES&lt;br /&gt;
 RMS     Force            0.000005     0.000300     YES&lt;br /&gt;
 Maximum Displacement     0.000036     0.001800     YES&lt;br /&gt;
 RMS     Displacement     0.000023     0.001200     YES&lt;br /&gt;
&amp;lt;/pre&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Frequency log file&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
[[Media:Hyc116_bbr3_freq.log]]&lt;br /&gt;
&lt;br /&gt;
Attached above is the frequency file saved onto the computer from the SCAN server portal. The frequency file was also published on the chemistry database DSpace. {{DOI|10042/202442}}&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Frequencies&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;pre&amp;gt;&lt;br /&gt;
Low frequencies ---   -0.0137   -0.0064   -0.0046    2.4315    2.4315    4.8421&lt;br /&gt;
Low frequencies ---  155.9631  155.9651  267.7052&lt;br /&gt;
&amp;lt;/pre&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;jmol of BBr&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;&#039;&#039;&#039;&lt;br /&gt;
&amp;lt;jmol&amp;gt;&amp;lt;jmolApplet&amp;gt;&lt;br /&gt;
  &amp;lt;title&amp;gt;optimised BBr3&amp;lt;/title&amp;gt;&lt;br /&gt;
  &amp;lt;color&amp;gt;black&amp;lt;/color&amp;gt;&lt;br /&gt;
  &amp;lt;size&amp;gt;200&amp;lt;/size&amp;gt;&lt;br /&gt;
  &amp;lt;uploadedFileContents&amp;gt;Hyc116_bbr3_freq.log&amp;lt;/uploadedFileContents&amp;gt;&lt;br /&gt;
&amp;lt;/jmolApplet&amp;gt;&amp;lt;/jmol&amp;gt;&lt;br /&gt;
&lt;br /&gt;
==Aromaticity==&lt;br /&gt;
&lt;br /&gt;
===Benzene===&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;Calculation type&amp;lt;/b&amp;gt;: Optimisation&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;Calculation Method&amp;lt;/b&amp;gt;: B3LYP&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;Basis set&amp;lt;/b&amp;gt;: 6-31G(d,p) &lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Summary table&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
[[file:Hyc116_c6h6_summarytable.png]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Items table&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;pre&amp;gt;&lt;br /&gt;
Item               Value     Threshold  Converged?&lt;br /&gt;
 Maximum Force            0.000193     0.000450     YES&lt;br /&gt;
 RMS     Force            0.000079     0.000300     YES&lt;br /&gt;
 Maximum Displacement     0.000830     0.001800     YES&lt;br /&gt;
 RMS     Displacement     0.000294     0.001200     YES&lt;br /&gt;
&amp;lt;/pre&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Frequency log file&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
[[Media:HYC116_C6H6_FREQ.LOG]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Frequencies&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;pre&amp;gt;&lt;br /&gt;
Low frequencies ---   -3.5606   -3.5606   -0.0089   -0.0043   -0.0043   10.0905&lt;br /&gt;
Low frequencies ---  413.9582  413.9582  621.1416&lt;br /&gt;
&amp;lt;/pre&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;jmol of C&amp;lt;sub&amp;gt;6&amp;lt;/sub&amp;gt;H&amp;lt;sub&amp;gt;6&amp;lt;/sub&amp;gt;&#039;&#039;&#039;&lt;br /&gt;
&amp;lt;jmol&amp;gt;&amp;lt;jmolApplet&amp;gt;&lt;br /&gt;
  &amp;lt;title&amp;gt;optimised Benzene&amp;lt;/title&amp;gt;&lt;br /&gt;
  &amp;lt;color&amp;gt;black&amp;lt;/color&amp;gt;&lt;br /&gt;
  &amp;lt;size&amp;gt;200&amp;lt;/size&amp;gt;&lt;br /&gt;
  &amp;lt;uploadedFileContents&amp;gt;HYC116_C6H6_FREQ.LOG&amp;lt;/uploadedFileContents&amp;gt;&lt;br /&gt;
&amp;lt;/jmolApplet&amp;gt;&amp;lt;/jmol&amp;gt;&lt;br /&gt;
&lt;br /&gt;
===Borazine===&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;Calculation type&amp;lt;/b&amp;gt;: Optimisation&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;Calculation Method&amp;lt;/b&amp;gt;: B3LYP&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;Basis set&amp;lt;/b&amp;gt;: 6-31G(d,p) &lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Summary table&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
[[file:Hyc116_borazine_summarytable.png]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Items table&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;pre&amp;gt;&lt;br /&gt;
Item               Value     Threshold  Converged?&lt;br /&gt;
 Maximum Force            0.000085     0.000450     YES&lt;br /&gt;
 RMS     Force            0.000033     0.000300     YES&lt;br /&gt;
 Maximum Displacement     0.000250     0.001800     YES&lt;br /&gt;
 RMS     Displacement     0.000074     0.001200     YES&lt;br /&gt;
&amp;lt;/pre&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Frequency log file&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
[[Media:HYC116_BORAZINE_FREQ.LOG]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Frequencies&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;pre&amp;gt;&lt;br /&gt;
Low frequencies ---  -12.6626  -12.6626   -8.9272   -0.0211   -0.0104   -0.0104&lt;br /&gt;
Low frequencies ---  289.1112  289.1112  403.8613&lt;br /&gt;
&amp;lt;/pre&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;jmol of Borazine&#039;&#039;&#039;&lt;br /&gt;
&amp;lt;jmol&amp;gt;&amp;lt;jmolApplet&amp;gt;&lt;br /&gt;
  &amp;lt;title&amp;gt;optimised Borazine&amp;lt;/title&amp;gt;&lt;br /&gt;
  &amp;lt;color&amp;gt;black&amp;lt;/color&amp;gt;&lt;br /&gt;
  &amp;lt;size&amp;gt;200&amp;lt;/size&amp;gt;&lt;br /&gt;
  &amp;lt;uploadedFileContents&amp;gt;HYC116_BORAZINE_FREQ.LOG&amp;lt;/uploadedFileContents&amp;gt;&lt;br /&gt;
&amp;lt;/jmolApplet&amp;gt;&amp;lt;/jmol&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
===Charge distribution===&lt;br /&gt;
&lt;br /&gt;
An NBO charge analysis was carried out on both the optimised benzene and borazine. Visualisations of the charge distribution are shown in the table below, with the colour range going from -1.102 to 1.102 for both molecule. This large scale was chosen as it allows direct comparison of the charge on any atoms in these two molecules and shows the relative magnitude of charges on all these atoms. Negative charges are shown in red, and positive charges are shown in green. A neutral charge is displayed in black, so the smaller a charge is (positive or negative), the darker its colour representation is. Larger charges are shown in brighter colours. The charges are also displayed on the atoms as numbers with a neutral charge being zero. Negative charges are shown as negative number and positive charges are shown as positive numbers. &lt;br /&gt;
&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot;&lt;br /&gt;
!&lt;br /&gt;
!Benzene&lt;br /&gt;
!Borazine&lt;br /&gt;
|-&lt;br /&gt;
!Visualisation of charge distribution&lt;br /&gt;
|[[File:Hyc116_benzene_charge_distribution1.png|500x500px|thumb|centre|Charge distribution of Benzene visualisation]]&lt;br /&gt;
|[[File:Hyc116_borazine_charge_distribution1.png|500x500px|thumb|centre|Charge distribution of Borazine visualisation]]&lt;br /&gt;
|-&lt;br /&gt;
!Charge &lt;br /&gt;
|Carbon: -0.239&lt;br /&gt;
&lt;br /&gt;
Hydrogen: 0.239&lt;br /&gt;
|Nitrogen: -1.102 &lt;br /&gt;
&lt;br /&gt;
Boron: 0.747&lt;br /&gt;
&lt;br /&gt;
Hydrogen (bonded to N): 0.432&lt;br /&gt;
&lt;br /&gt;
Hydrogen (bonded to B): -0.077&lt;br /&gt;
|-&lt;br /&gt;
!Discussion&lt;br /&gt;
|From the visualisation, it is shown that there is a slightly negative charge on the carbon atoms, and a positive charge of the same magnitude on the hydrogen atoms. All the carbon atoms have the same charge as they are in identical environments. The same applies to all the hydrogen atoms. This is due to the highly symmetrical structure of benzene. Since the same colour scale was used for both benzene and borazine, and the charges are much smaller in magnitude on atoms in benzene than atoms on borazine, the colours on the charge distribution visualisation is much darker. &lt;br /&gt;
|From the colours displayed on the charge distribution visualisation as well as the charge values, it is shown that nitrogen has a relatively large negative charge, while boron has a positive charge. This is due to the difference in electrogenativity between these atoms: nitrogen atoms are more electronegative than boron and tends to attract electrons towards themselves. It is worth noting that the hydrogen atoms do not all have the same charge. The hydrogen atoms bonded to boron have a slightly negative charge, and the ones bonded to nitrogen have a small positive charge. &lt;br /&gt;
&lt;br /&gt;
The fact that the same colour scale was used for both molecules comes in helpful here. It allows the charges on atoms to be compared directly. For example, just from looking at the colours, one can tell that or example, even though both carbon and nitrogen are electronegative, nitrogen is much more electronegative, which is quantitatively shown by Pauling&#039;s electronegativity scale.&amp;lt;ref&amp;gt;http://www.tutor-homework.com/Chemistry_Help/electronegativity_table/electronegativity.html (Accessed: 24.0502018&amp;lt;/ref&amp;gt;&lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
===Comparative MOs of Benzene and Borazine===&lt;br /&gt;
&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot;&lt;br /&gt;
!&lt;br /&gt;
!Benzene&lt;br /&gt;
!Borazine&lt;br /&gt;
!Comparison and Discussion&lt;br /&gt;
|-&lt;br /&gt;
!1st comparative pair&lt;br /&gt;
|[[File:Hyc116_benzene_1st_MO_pair_7.png|200x200px|centre]]&lt;br /&gt;
|[[File:Hyc116_borazine_1st_MO_pair_level9.png|200x200px|centre]]&lt;br /&gt;
|MO 9 of both benzene and borazine are comparable. They both show delocalised molecular orbital with an overall bonding character. There is a nodal plane across the molecular orbitals for both benzene and borazine. For benzene, there is contribution from all the carbon and hydrogen s orbitals. Moreover, the molecular orbitals are symmetric to their counterpart of opposite phase, giving an E&amp;lt;sub&amp;gt;1g&amp;lt;/sub&amp;gt; MO. That is not the case for borazine; they are less symmetric in borazine. Nitrogen atoms are more electronegative than boron atoms and pull electron density towards themselves, resulting in a larger MO. There is contribution from all the boron and nitrogen s orbitals, and three of the hydrogen s orbitals, though not all of them. &lt;br /&gt;
|-&lt;br /&gt;
!2nd comparative pair&lt;br /&gt;
|[[File:Hyc116_benzene_2nd_MO_pair_10.png|200x200px|centre]]&lt;br /&gt;
|[[File:Hyc116_borazine_2nd_MO_pair_level11.png|200x200px|centre]]&lt;br /&gt;
|MO 10 of benzene and MO 11 of borazine are comparable. Here shows a pair of rather delocalised molecular orbitals with slightly more antibonding character than the first pair shown above. On both MOs, there is no contribution from one pair of opposite hydrogen atoms, but contribution from s orbitals of all other atoms on both molecule. The benzene MO has an E&amp;lt;sub&amp;gt;2g&amp;lt;/sub&amp;gt; symmetry. In borazine, the lobes are in different sizes due to the higher electronegativity of nitrogen. The lobes at the nitrogen atoms are larger as they attract electrons towards themselves more so than boron atoms do. &lt;br /&gt;
|-&lt;br /&gt;
!3rd comparative pair&lt;br /&gt;
|[[File:Hyc116_benzene_3rd_MO_pair_21.png|200x200px|centre]]&lt;br /&gt;
|[[File:Hyc116_borazine_3rd_MO_pair_level21.png|200x200px|centre]]&lt;br /&gt;
|The HOMO (MO 21) of benzene and the HOMO (MO 21) of borazine are comparable. They are both made of p orbitals of all carbon atoms (or all boron and nitrogen atoms in the case of borazine); there is no contribution from hydrogen atoms as they do not have p orbitals. There is a nodal plan perpendicular to the z axis (highest rotational axis) and one parallel to the z axis. On benzene, the MO is very symmetric and has an E&amp;lt;sub&amp;gt;1g&amp;lt;/sub&amp;gt; symmetry; the lobes of the MO are the same in size. On borazine, the lobe where there are two nitrogen atoms is bigger in size, again due to the higher electronegtivity of nitrogen compared to boron. &lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
===Aromaticity: some theories===&lt;br /&gt;
&lt;br /&gt;
Aromatic compounds display properties such as their high stability and bond lengths between typical single and double bonds. A simple understanding of aromaticity involves the overlap of p orbitals perpendicular to the cyclic plane; the delocalisation of electrons on the pi system is identified to be responsible of the stability of aromatic systems. Aromatic compounds can be identified by the Huckel’s rule, which states that conjugated planar cyclic molecules with (4n +2) π electrons are aromatic. Both benzene and borazine obey the Huckel’s rule and fit the conventional description of aromaticity. &lt;br /&gt;
&lt;br /&gt;
However, it is proved in recent years that the conventional criteria do not necessarily have to be obeyed for a compound to be aromatic. For instance, there has been shown that some non-planar compounds display aromaticity. This suggests that the criteria for aromaticity is not simply structural, and these advances give rise to concepts such as quasiaromaticity and pseudoaromaticity. Recent advances show that there are quantum mechanics basis on the idea of aromaticity. &lt;br /&gt;
In conclusion, while the overlap of pi orbitals provides a simple understanding for aromaticity, it is not a sufficient description for aromaticity.&lt;br /&gt;
&lt;br /&gt;
==References==&lt;br /&gt;
{{reflist}}&lt;/div&gt;</summary>
		<author><name>Hyc116</name></author>
	</entry>
	<entry>
		<id>https://chemwiki.ch.ic.ac.uk/index.php?title=MO_hyc116&amp;diff=731457</id>
		<title>MO hyc116</title>
		<link rel="alternate" type="text/html" href="https://chemwiki.ch.ic.ac.uk/index.php?title=MO_hyc116&amp;diff=731457"/>
		<updated>2018-05-25T12:39:34Z</updated>

		<summary type="html">&lt;p&gt;Hyc116: /* Comparative MOs of Benzene and Borazine */&lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;==BH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;==&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;Calculation type&amp;lt;/b&amp;gt;: Optimisation&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;Calculation Method&amp;lt;/b&amp;gt;: B3LYP&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;Basis set&amp;lt;/b&amp;gt;: 6-31G(d,p) &lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Summary table&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
[[file:Hyc116_bh3_631g_opt_summarytable.png]]&lt;br /&gt;
&lt;br /&gt;
The above summary table was obtained after the 2nd optimisation of BH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt; (after the initial optimisation using the 3-21G basis set). Notice how the symmetry is incorrect and shown as Cs. This is because the symmetry was manually broken at the beginning by changing the bond length of B-H bonds. The point group was manually adjusted and the molecule was optimised again before the frequency analysis and the new summary table is attached below.&lt;br /&gt;
&lt;br /&gt;
[[file:Hyc116_bh3_correctsummarytable.png]]&lt;br /&gt;
&lt;br /&gt;
The above summary table was obtained from the optimisation after adjusting the symmetry. The point shown in this summary table is D&amp;lt;sub&amp;gt;3h&amp;lt;/sub&amp;gt;, which is the correct for BH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;. &lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Items table&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
Below is the items table taken from the optimisation with the correct point group.&lt;br /&gt;
&lt;br /&gt;
&amp;lt;pre&amp;gt;&lt;br /&gt;
Item               Value     Threshold  Converged?&lt;br /&gt;
 Maximum Force            0.000015     0.000450     YES&lt;br /&gt;
 RMS     Force            0.000010     0.000300     YES&lt;br /&gt;
 Maximum Displacement     0.000058     0.001800     YES&lt;br /&gt;
 RMS     Displacement     0.000038     0.001200     YES&lt;br /&gt;
&amp;lt;/pre&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Frequency log file&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
[[Media:HYC116 BH3 FREQ.LOG]] &lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Frequencies&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;pre&amp;gt;&lt;br /&gt;
Low frequencies ---  -10.3498   -3.4492   -1.2454   -0.0055    0.4779    3.2165&lt;br /&gt;
Low frequencies --- 1162.9519 1213.1527 1213.1554&lt;br /&gt;
&amp;lt;/pre&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;jmol of BH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;&#039;&#039;&#039;&lt;br /&gt;
&amp;lt;jmol&amp;gt;&amp;lt;jmolApplet&amp;gt;&lt;br /&gt;
  &amp;lt;title&amp;gt;optimised BH3&amp;lt;/title&amp;gt;&lt;br /&gt;
  &amp;lt;color&amp;gt;black&amp;lt;/color&amp;gt;&lt;br /&gt;
  &amp;lt;size&amp;gt;200&amp;lt;/size&amp;gt;&lt;br /&gt;
  &amp;lt;uploadedFileContents&amp;gt;HYC116_BH3_FREQ.LOG&amp;lt;/uploadedFileContents&amp;gt;&lt;br /&gt;
&amp;lt;/jmolApplet&amp;gt;&amp;lt;/jmol&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
===Vibrational spectrum===&lt;br /&gt;
&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot;&lt;br /&gt;
!wavenumber (cm&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;)&lt;br /&gt;
!Intensity (arbitrary units)&lt;br /&gt;
!symmetry&lt;br /&gt;
!IR active?&lt;br /&gt;
!type&lt;br /&gt;
|-&lt;br /&gt;
|1163&lt;br /&gt;
|93&lt;br /&gt;
|A&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;&#039; &#039;&lt;br /&gt;
|Yes&lt;br /&gt;
|Out of plane bend&lt;br /&gt;
|-&lt;br /&gt;
|1213&lt;br /&gt;
|14&lt;br /&gt;
|E&#039;&lt;br /&gt;
|Very slight&lt;br /&gt;
|Bend&lt;br /&gt;
|-&lt;br /&gt;
|1213&lt;br /&gt;
|14&lt;br /&gt;
|E&#039;&lt;br /&gt;
|Very slight&lt;br /&gt;
|Bend&lt;br /&gt;
|-&lt;br /&gt;
|2582&lt;br /&gt;
|0&lt;br /&gt;
|A&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;&#039;&lt;br /&gt;
|No&lt;br /&gt;
|Symmetric stretch&lt;br /&gt;
|-&lt;br /&gt;
|2716&lt;br /&gt;
|126&lt;br /&gt;
|E&#039;&lt;br /&gt;
|Yes&lt;br /&gt;
|Asymmetric stretch&lt;br /&gt;
|-&lt;br /&gt;
|2716&lt;br /&gt;
|126&lt;br /&gt;
|E&#039;&lt;br /&gt;
|Yes&lt;br /&gt;
|Asymmetric stretch&lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;IR spectrum&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
[[file:Hyc116_ir_bh3.png|400*600]]&lt;br /&gt;
&lt;br /&gt;
There are only three peaks on the IR spectrum of BH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;, despite that there are 6 vibrational modes for the molecule. As shown in the table above, the symmetric stretching mode with A1 symmetry at 2582 cm&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt; is not IR active; naturally, that vibrational mode doesn’t give a peak on the IR spectrum. As shown from the table, two pairs of vibrational modes, the bond angle deformation/bend at 1213 cm&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt; and the asymmetric bond stretch at 2716 cm&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;, are degenerate with the symmetry label E. This means that they have the same energy, and hence give the same wavenumber on the IR spectrum. Each pair of degenerate vibrational modes give rise to one peak. This leaves three peaks, as confirmed by the IR spectrum above.&lt;br /&gt;
&lt;br /&gt;
===Molecular orbitals of BH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;===&lt;br /&gt;
&lt;br /&gt;
[[file:hyc116_bh3_MO_diagram.png]]&lt;br /&gt;
&lt;br /&gt;
The above molecular orbital diagram was taken from Dr Patricia Hunt&#039;s &amp;lt;i&amp;gt;Lecture 4 Tutorial Problem Model Answers&amp;lt;/i&amp;gt;.&amp;lt;ref&amp;gt;P. Hunt, &amp;quot;Lecture 4 Tutorial Problem Model Answers&amp;quot;, 2 (2018)&amp;lt;/ref&amp;gt; Diagrams of the &amp;quot;real&amp;quot; MOs were obtained from Gaussian.&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
There is no significant difference between the LCAO MOs and the real ones. Features such as orbital phases are shown clearly on both the LCAO MOs and the real MOs, illustrating the bonding/anti-bonding characters of the molecular orbitals. This suggests that the the qualitative MO theory is highly accurate and useful when studying the molecular orbitals of molecules.&lt;br /&gt;
&lt;br /&gt;
==Associated energies: ammonium borane==&lt;br /&gt;
&lt;br /&gt;
===NH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;===&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;Calculation type&amp;lt;/b&amp;gt;: Optimisation&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;Calculation Method&amp;lt;/b&amp;gt;: B3LYP&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;Basis set&amp;lt;/b&amp;gt;: 6-31G(d,p) &lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Summary table&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
[[file:Hyc116_nh3_631g_summarytable.png]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Items table&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;pre&amp;gt;&lt;br /&gt;
Item               Value     Threshold  Converged?&lt;br /&gt;
 Maximum Force            0.000006     0.000450     YES&lt;br /&gt;
 RMS     Force            0.000004     0.000300     YES&lt;br /&gt;
 Maximum Displacement     0.000012     0.001800     YES&lt;br /&gt;
 RMS     Displacement     0.000008     0.001200     YES&lt;br /&gt;
&amp;lt;/pre&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Frequency log file&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
[[Media:HYC116_NH3_FREQ.LOG]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Frequencies&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;pre&amp;gt;&lt;br /&gt;
Low frequencies ---   -8.5646   -8.5588   -0.0047    0.0454    0.1784   26.4183&lt;br /&gt;
Low frequencies --- 1089.7603 1694.1865 1694.1865&lt;br /&gt;
&amp;lt;/pre&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;jmol of NH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;&#039;&#039;&#039;&lt;br /&gt;
&amp;lt;jmol&amp;gt;&amp;lt;jmolApplet&amp;gt;&lt;br /&gt;
  &amp;lt;title&amp;gt;optimised NH3&amp;lt;/title&amp;gt;&lt;br /&gt;
  &amp;lt;color&amp;gt;black&amp;lt;/color&amp;gt;&lt;br /&gt;
  &amp;lt;size&amp;gt;200&amp;lt;/size&amp;gt;&lt;br /&gt;
  &amp;lt;uploadedFileContents&amp;gt;HYC116_NH3_FREQ.LOG&amp;lt;/uploadedFileContents&amp;gt;&lt;br /&gt;
&amp;lt;/jmolApplet&amp;gt;&amp;lt;/jmol&amp;gt;&lt;br /&gt;
&lt;br /&gt;
===NH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;BH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;===&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;Calculation type&amp;lt;/b&amp;gt;: Optimisation&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;Calculation Method&amp;lt;/b&amp;gt;: B3LYP&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;Basis set&amp;lt;/b&amp;gt;: 6-31G(d,p) &lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Summary table&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
[[file:Hyc116_nh3bh3_631g_summarytable1.png]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Items table&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;pre&amp;gt;&lt;br /&gt;
Item               Value     Threshold  Converged?&lt;br /&gt;
 Maximum Force            0.000121     0.000450     YES&lt;br /&gt;
 RMS     Force            0.000057     0.000300     YES&lt;br /&gt;
 Maximum Displacement     0.000501     0.001800     YES&lt;br /&gt;
 RMS     Displacement     0.000293     0.001200     YES&lt;br /&gt;
&amp;lt;/pre&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Frequency log file&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
[[Media:HYC116_NH3BH3_FREQ1.LOG]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Frequencies&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;pre&amp;gt;&lt;br /&gt;
Low frequencies ---   -0.0574   -0.0501   -0.0074   21.6276   21.6377   40.3839&lt;br /&gt;
Low frequencies ---  265.9973  632.3725  640.1275&lt;br /&gt;
&amp;lt;/pre&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;jmol of NH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;BH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;&#039;&#039;&#039;&lt;br /&gt;
&amp;lt;jmol&amp;gt;&amp;lt;jmolApplet&amp;gt;&lt;br /&gt;
  &amp;lt;title&amp;gt;optimised NH3BH3&amp;lt;/title&amp;gt;&lt;br /&gt;
  &amp;lt;color&amp;gt;black&amp;lt;/color&amp;gt;&lt;br /&gt;
  &amp;lt;size&amp;gt;200&amp;lt;/size&amp;gt;&lt;br /&gt;
  &amp;lt;uploadedFileContents&amp;gt;HYC116_NH3BH3_FREQ.LOG&amp;lt;/uploadedFileContents&amp;gt;&lt;br /&gt;
&amp;lt;/jmolApplet&amp;gt;&amp;lt;/jmol&amp;gt;&lt;br /&gt;
&lt;br /&gt;
===Association energy===&lt;br /&gt;
&lt;br /&gt;
E(BH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;) (using the optimisation with the correct symmetry) = -26.61532363 a.u. = &amp;lt;b&amp;gt;-26.61532 a.u. (5 d.p.)&amp;lt;/b&amp;gt;&lt;br /&gt;
&lt;br /&gt;
E(NH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;) = -56.55776873 a.u. = &amp;lt;b&amp;gt;-56.55777 a.u. (5 d.p.)&amp;lt;/b&amp;gt;&lt;br /&gt;
&lt;br /&gt;
E(NH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;BH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;) = -83.22468892 a.u. = &amp;lt;b&amp;gt;-83.22469 a.u. (5 d.p.)&amp;lt;/b&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
Carrying out calculations using numbers which has already been rounded up can possibly result in errors in the last digit. Hence, here the calculations were carried out using the numbers provided from the optimisations (i.e. with more decimal places than necessary); the answer was then rounded up to the desired accuracy. &lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
ΔE = E(NH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;BH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;)-[E(NH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;)+E(BH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;)]&lt;br /&gt;
&lt;br /&gt;
ΔE = -83.22468892 - (-56.55776873 + -26.61532363) = -0.05159656 a.u. &lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;ΔE = -0.05160 a.u. (5 d.p.)&amp;lt;/b&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Converting energy from a.u. to kJ/mol&#039;&#039;&#039;&lt;br /&gt;
An atomic unit for energy is Hartree, which is equal to 2625.5 kJ/mol.&lt;br /&gt;
&amp;lt;ref&amp;gt;https://cccbdb.nist.gov/hartree.asp (Accessed: 22.05.2018)&amp;lt;/ref&amp;gt;&lt;br /&gt;
 &lt;br /&gt;
&lt;br /&gt;
So ΔE in kJ/mol = -0.05159657 * 2625.5 = -135.46676828 kJ/mol&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;ΔE = -135 kJ/mol (nearest integer)&amp;lt;/b&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
The energy difference calculated above comes from the formation of the B-N dative bond. It is a relatively weak bond. According to a bond energy data sheet provided by the University of California,&amp;lt;ref&amp;gt;https://labs.chem.ucsb.edu/zakarian/armen/11---bonddissociationenergy.pdf (Accessed: 24.05.2018)&amp;lt;/ref&amp;gt;  the bond energy of the C-C bond of an ethane molecule is 368 kJ/mol. This is a fair comparison to the NH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;BH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt; molecule as the two molecules have the same structure, only with the carbon atoms on ethane swapped for Boron and Nitrogen in NH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;BH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;&lt;br /&gt;
&lt;br /&gt;
==Using a mixture of basis-sets and pseudo-potentials==&lt;br /&gt;
&lt;br /&gt;
===BBr&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;===&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;Calculation type&amp;lt;/b&amp;gt;: Optimisation&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;Calculation Method&amp;lt;/b&amp;gt;: B3LYP&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;Basis set&amp;lt;/b&amp;gt;: Boron: 6-31G(d,p) ; Br: LANL2DZ&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
Larger calculations are often sent to a web-server to run on a high-performance computer instead of a desktop. In order to experience and learn to use a web-server, the optimisation and the frequency analysis for BBr&amp;lt;sub&amp;gt;3&amp;lt;/sub were both sent and done on a server instead of the desktop. The calculation results were downloaded from the web-server once they were finished.   &lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Summary table&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
[[file:Hyc116_bbr3_opt_summarytable.png]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Items table&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;pre&amp;gt;&lt;br /&gt;
Item               Value     Threshold  Converged?&lt;br /&gt;
 Maximum Force            0.000008     0.000450     YES&lt;br /&gt;
 RMS     Force            0.000005     0.000300     YES&lt;br /&gt;
 Maximum Displacement     0.000036     0.001800     YES&lt;br /&gt;
 RMS     Displacement     0.000023     0.001200     YES&lt;br /&gt;
&amp;lt;/pre&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Frequency log file&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
[[Media:Hyc116_bbr3_freq.log]]&lt;br /&gt;
&lt;br /&gt;
Attached above is the frequency file saved onto the computer from the SCAN server portal. The frequency file was also published on the chemistry database DSpace. {{DOI|10042/202442}}&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Frequencies&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;pre&amp;gt;&lt;br /&gt;
Low frequencies ---   -0.0137   -0.0064   -0.0046    2.4315    2.4315    4.8421&lt;br /&gt;
Low frequencies ---  155.9631  155.9651  267.7052&lt;br /&gt;
&amp;lt;/pre&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;jmol of BBr&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;&#039;&#039;&#039;&lt;br /&gt;
&amp;lt;jmol&amp;gt;&amp;lt;jmolApplet&amp;gt;&lt;br /&gt;
  &amp;lt;title&amp;gt;optimised BBr3&amp;lt;/title&amp;gt;&lt;br /&gt;
  &amp;lt;color&amp;gt;black&amp;lt;/color&amp;gt;&lt;br /&gt;
  &amp;lt;size&amp;gt;200&amp;lt;/size&amp;gt;&lt;br /&gt;
  &amp;lt;uploadedFileContents&amp;gt;Hyc116_bbr3_freq.log&amp;lt;/uploadedFileContents&amp;gt;&lt;br /&gt;
&amp;lt;/jmolApplet&amp;gt;&amp;lt;/jmol&amp;gt;&lt;br /&gt;
&lt;br /&gt;
==Aromaticity==&lt;br /&gt;
&lt;br /&gt;
===Benzene===&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;Calculation type&amp;lt;/b&amp;gt;: Optimisation&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;Calculation Method&amp;lt;/b&amp;gt;: B3LYP&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;Basis set&amp;lt;/b&amp;gt;: 6-31G(d,p) &lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Summary table&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
[[file:Hyc116_c6h6_summarytable.png]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Items table&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;pre&amp;gt;&lt;br /&gt;
Item               Value     Threshold  Converged?&lt;br /&gt;
 Maximum Force            0.000193     0.000450     YES&lt;br /&gt;
 RMS     Force            0.000079     0.000300     YES&lt;br /&gt;
 Maximum Displacement     0.000830     0.001800     YES&lt;br /&gt;
 RMS     Displacement     0.000294     0.001200     YES&lt;br /&gt;
&amp;lt;/pre&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Frequency log file&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
[[Media:HYC116_C6H6_FREQ.LOG]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Frequencies&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;pre&amp;gt;&lt;br /&gt;
Low frequencies ---   -3.5606   -3.5606   -0.0089   -0.0043   -0.0043   10.0905&lt;br /&gt;
Low frequencies ---  413.9582  413.9582  621.1416&lt;br /&gt;
&amp;lt;/pre&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;jmol of C&amp;lt;sub&amp;gt;6&amp;lt;/sub&amp;gt;H&amp;lt;sub&amp;gt;6&amp;lt;/sub&amp;gt;&#039;&#039;&#039;&lt;br /&gt;
&amp;lt;jmol&amp;gt;&amp;lt;jmolApplet&amp;gt;&lt;br /&gt;
  &amp;lt;title&amp;gt;optimised Benzene&amp;lt;/title&amp;gt;&lt;br /&gt;
  &amp;lt;color&amp;gt;black&amp;lt;/color&amp;gt;&lt;br /&gt;
  &amp;lt;size&amp;gt;200&amp;lt;/size&amp;gt;&lt;br /&gt;
  &amp;lt;uploadedFileContents&amp;gt;HYC116_C6H6_FREQ.LOG&amp;lt;/uploadedFileContents&amp;gt;&lt;br /&gt;
&amp;lt;/jmolApplet&amp;gt;&amp;lt;/jmol&amp;gt;&lt;br /&gt;
&lt;br /&gt;
===Borazine===&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;Calculation type&amp;lt;/b&amp;gt;: Optimisation&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;Calculation Method&amp;lt;/b&amp;gt;: B3LYP&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;Basis set&amp;lt;/b&amp;gt;: 6-31G(d,p) &lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Summary table&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
[[file:Hyc116_borazine_summarytable.png]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Items table&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;pre&amp;gt;&lt;br /&gt;
Item               Value     Threshold  Converged?&lt;br /&gt;
 Maximum Force            0.000085     0.000450     YES&lt;br /&gt;
 RMS     Force            0.000033     0.000300     YES&lt;br /&gt;
 Maximum Displacement     0.000250     0.001800     YES&lt;br /&gt;
 RMS     Displacement     0.000074     0.001200     YES&lt;br /&gt;
&amp;lt;/pre&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Frequency log file&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
[[Media:HYC116_BORAZINE_FREQ.LOG]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Frequencies&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;pre&amp;gt;&lt;br /&gt;
Low frequencies ---  -12.6626  -12.6626   -8.9272   -0.0211   -0.0104   -0.0104&lt;br /&gt;
Low frequencies ---  289.1112  289.1112  403.8613&lt;br /&gt;
&amp;lt;/pre&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;jmol of Borazine&#039;&#039;&#039;&lt;br /&gt;
&amp;lt;jmol&amp;gt;&amp;lt;jmolApplet&amp;gt;&lt;br /&gt;
  &amp;lt;title&amp;gt;optimised Borazine&amp;lt;/title&amp;gt;&lt;br /&gt;
  &amp;lt;color&amp;gt;black&amp;lt;/color&amp;gt;&lt;br /&gt;
  &amp;lt;size&amp;gt;200&amp;lt;/size&amp;gt;&lt;br /&gt;
  &amp;lt;uploadedFileContents&amp;gt;HYC116_BORAZINE_FREQ.LOG&amp;lt;/uploadedFileContents&amp;gt;&lt;br /&gt;
&amp;lt;/jmolApplet&amp;gt;&amp;lt;/jmol&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
===Charge distribution===&lt;br /&gt;
&lt;br /&gt;
An NBO charge analysis was carried out on both the optimised benzene and borazine. Visualisations of the charge distribution are shown in the table below, with the colour range going from -1.102 to 1.102 for both molecule. This large scale was chosen as it allows direct comparison of the charge on any atoms in these two molecules and shows the relative magnitude of charges on all these atoms. Negative charges are shown in red, and positive charges are shown in green. A neutral charge is displayed in black, so the smaller a charge is (positive or negative), the darker its colour representation is. Larger charges are shown in brighter colours. The charges are also displayed on the atoms as numbers with a neutral charge being zero. Negative charges are shown as negative number and positive charges are shown as positive numbers. &lt;br /&gt;
&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot;&lt;br /&gt;
!&lt;br /&gt;
!Benzene&lt;br /&gt;
!Borazine&lt;br /&gt;
|-&lt;br /&gt;
!Visualisation of charge distribution&lt;br /&gt;
|[[File:Hyc116_benzene_charge_distribution1.png|500x500px|thumb|centre|Charge distribution of Benzene visualisation]]&lt;br /&gt;
|[[File:Hyc116_borazine_charge_distribution1.png|500x500px|thumb|centre|Charge distribution of Borazine visualisation]]&lt;br /&gt;
|-&lt;br /&gt;
!Charge &lt;br /&gt;
|Carbon: -0.239&lt;br /&gt;
&lt;br /&gt;
Hydrogen: 0.239&lt;br /&gt;
|Nitrogen: -1.102 &lt;br /&gt;
&lt;br /&gt;
Boron: 0.747&lt;br /&gt;
&lt;br /&gt;
Hydrogen (bonded to N): 0.432&lt;br /&gt;
&lt;br /&gt;
Hydrogen (bonded to B): -0.077&lt;br /&gt;
|-&lt;br /&gt;
!Discussion&lt;br /&gt;
|From the visualisation, it is shown that there is a slightly negative charge on the carbon atoms, and a positive charge of the same magnitude on the hydrogen atoms. All the carbon atoms have the same charge as they are in identical environments. The same applies to all the hydrogen atoms. This is due to the highly symmetrical structure of benzene. Since the same colour scale was used for both benzene and borazine, and the charges are much smaller in magnitude on atoms in benzene than atoms on borazine, the colours on the charge distribution visualisation is much darker. &lt;br /&gt;
|From the colours displayed on the charge distribution visualisation as well as the charge values, it is shown that nitrogen has a relatively large negative charge, while boron has a positive charge. This is due to the difference in electrogenativity between these atoms: nitrogen atoms are more electronegative than boron and tends to attract electrons towards themselves. It is worth noting that the hydrogen atoms do not all have the same charge. The hydrogen atoms bonded to boron have a slightly negative charge, and the ones bonded to nitrogen have a small positive charge. &lt;br /&gt;
&lt;br /&gt;
The fact that the same colour scale was used for both molecules comes in helpful here. It allows the charges on atoms to be compared directly. For example, just from looking at the colours, one can tell that or example, even though both carbon and nitrogen are electronegative, nitrogen is much more electronegative, which is quantitatively shown by Pauling&#039;s electronegativity scale.&amp;lt;ref&amp;gt;http://www.tutor-homework.com/Chemistry_Help/electronegativity_table/electronegativity.html (Accessed: 24.0502018&amp;lt;/ref&amp;gt;&lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
===Comparative MOs of Benzene and Borazine===&lt;br /&gt;
&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot;&lt;br /&gt;
!&lt;br /&gt;
!Benzene&lt;br /&gt;
!Borazine&lt;br /&gt;
!Comparison and Discussion&lt;br /&gt;
|-&lt;br /&gt;
!1st comparative pair&lt;br /&gt;
|[[File:Hyc116_benzene_1st_MO_pair_7.png|200x200px|centre]]&lt;br /&gt;
|[[File:Hyc116_borazine_1st_MO_pair_level9.png|200x200px|centre]]&lt;br /&gt;
|MO 9 of both benzene and borazine are comparable. They both show delocalised molecular orbital with an overall bonding character. There is a nodal plane across the molecular orbitals for both benzene and borazine. For benzene, there is contribution from all the carbon and hydrogen s orbitals. Moreover, the molecular orbitals are symmetric to their counterpart of opposite phase, giving an E&amp;lt;sub&amp;gt;1g&amp;lt;/sub&amp;gt; MO. That is not the case for borazine; they are less symmetric in borazine. Nitrogen atoms are more electronegative than boron atoms and pull electron density towards themselves, resulting in a larger MO. There is contribution from all the boron and nitrogen s orbitals, and three of the hydrogen s orbitals, though not all of them. &lt;br /&gt;
|-&lt;br /&gt;
!2nd comparative pair&lt;br /&gt;
|[[File:Hyc116_benzene_2nd_MO_pair_10.png|200x200px|centre]]&lt;br /&gt;
|[[File:Hyc116_borazine_2nd_MO_pair_level11.png|200x200px|centre]]&lt;br /&gt;
|MO 10 of benzene and MO 11 of borazine are comparable. Here shows a pair of rather delocalised molecular orbitals with slightly more antibonding character than the first pair shown above. On both MOs, there is no contribution from one pair of opposite hydrogen atoms, but contribution from s orbitals of all other atoms on both molecule. The benzene MO has an E&amp;lt;sub&amp;gt;2g&amp;lt;/sub&amp;gt; symmetry. In borazine, the lobes are in different sizes due to the higher electronegativity of nitrogen. The lobes at the nitrogen atoms are larger as they attract electrons towards themselves more so than boron atoms do. &lt;br /&gt;
|-&lt;br /&gt;
!3rd comparative pair&lt;br /&gt;
|[[File:Hyc116_benzene_3rd_MO_pair_21.png|200x200px|centre]]&lt;br /&gt;
|[[File:Hyc116_borazine_3rd_MO_pair_level21.png|200x200px|centre]]&lt;br /&gt;
|The HOMO (MO 21) of benzene and the HOMO (MO 21) of borazine are comparable. They are both made of p orbitals of all carbon atoms (or all boron and nitrogen atoms in the case of borazine); there is no contribution from hydrogen atoms as they do not have p orbitals. There is a nodal plan perpendicular to the z axis (highest rotational axis) and one parallel to the z axis. On benzene, the MO is very symmetric and has an E&amp;lt;sub&amp;gt;1g&amp;lt;/sub&amp;gt; symmetry; the lobes of the MO are the same in size. On borazine, the lobe where there are two nitrogen atoms is bigger in size, again due to the higher electronegtivity of nitrogen compared to boron. &lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
===Aromaticity: some theories===&lt;br /&gt;
&lt;br /&gt;
==References==&lt;br /&gt;
{{reflist}}&lt;/div&gt;</summary>
		<author><name>Hyc116</name></author>
	</entry>
	<entry>
		<id>https://chemwiki.ch.ic.ac.uk/index.php?title=MO_hyc116&amp;diff=731453</id>
		<title>MO hyc116</title>
		<link rel="alternate" type="text/html" href="https://chemwiki.ch.ic.ac.uk/index.php?title=MO_hyc116&amp;diff=731453"/>
		<updated>2018-05-25T12:39:14Z</updated>

		<summary type="html">&lt;p&gt;Hyc116: /* Comparative MOs of Benzene and Borazine */&lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;==BH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;==&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;Calculation type&amp;lt;/b&amp;gt;: Optimisation&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;Calculation Method&amp;lt;/b&amp;gt;: B3LYP&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;Basis set&amp;lt;/b&amp;gt;: 6-31G(d,p) &lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Summary table&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
[[file:Hyc116_bh3_631g_opt_summarytable.png]]&lt;br /&gt;
&lt;br /&gt;
The above summary table was obtained after the 2nd optimisation of BH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt; (after the initial optimisation using the 3-21G basis set). Notice how the symmetry is incorrect and shown as Cs. This is because the symmetry was manually broken at the beginning by changing the bond length of B-H bonds. The point group was manually adjusted and the molecule was optimised again before the frequency analysis and the new summary table is attached below.&lt;br /&gt;
&lt;br /&gt;
[[file:Hyc116_bh3_correctsummarytable.png]]&lt;br /&gt;
&lt;br /&gt;
The above summary table was obtained from the optimisation after adjusting the symmetry. The point shown in this summary table is D&amp;lt;sub&amp;gt;3h&amp;lt;/sub&amp;gt;, which is the correct for BH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;. &lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Items table&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
Below is the items table taken from the optimisation with the correct point group.&lt;br /&gt;
&lt;br /&gt;
&amp;lt;pre&amp;gt;&lt;br /&gt;
Item               Value     Threshold  Converged?&lt;br /&gt;
 Maximum Force            0.000015     0.000450     YES&lt;br /&gt;
 RMS     Force            0.000010     0.000300     YES&lt;br /&gt;
 Maximum Displacement     0.000058     0.001800     YES&lt;br /&gt;
 RMS     Displacement     0.000038     0.001200     YES&lt;br /&gt;
&amp;lt;/pre&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Frequency log file&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
[[Media:HYC116 BH3 FREQ.LOG]] &lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Frequencies&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;pre&amp;gt;&lt;br /&gt;
Low frequencies ---  -10.3498   -3.4492   -1.2454   -0.0055    0.4779    3.2165&lt;br /&gt;
Low frequencies --- 1162.9519 1213.1527 1213.1554&lt;br /&gt;
&amp;lt;/pre&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;jmol of BH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;&#039;&#039;&#039;&lt;br /&gt;
&amp;lt;jmol&amp;gt;&amp;lt;jmolApplet&amp;gt;&lt;br /&gt;
  &amp;lt;title&amp;gt;optimised BH3&amp;lt;/title&amp;gt;&lt;br /&gt;
  &amp;lt;color&amp;gt;black&amp;lt;/color&amp;gt;&lt;br /&gt;
  &amp;lt;size&amp;gt;200&amp;lt;/size&amp;gt;&lt;br /&gt;
  &amp;lt;uploadedFileContents&amp;gt;HYC116_BH3_FREQ.LOG&amp;lt;/uploadedFileContents&amp;gt;&lt;br /&gt;
&amp;lt;/jmolApplet&amp;gt;&amp;lt;/jmol&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
===Vibrational spectrum===&lt;br /&gt;
&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot;&lt;br /&gt;
!wavenumber (cm&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;)&lt;br /&gt;
!Intensity (arbitrary units)&lt;br /&gt;
!symmetry&lt;br /&gt;
!IR active?&lt;br /&gt;
!type&lt;br /&gt;
|-&lt;br /&gt;
|1163&lt;br /&gt;
|93&lt;br /&gt;
|A&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;&#039; &#039;&lt;br /&gt;
|Yes&lt;br /&gt;
|Out of plane bend&lt;br /&gt;
|-&lt;br /&gt;
|1213&lt;br /&gt;
|14&lt;br /&gt;
|E&#039;&lt;br /&gt;
|Very slight&lt;br /&gt;
|Bend&lt;br /&gt;
|-&lt;br /&gt;
|1213&lt;br /&gt;
|14&lt;br /&gt;
|E&#039;&lt;br /&gt;
|Very slight&lt;br /&gt;
|Bend&lt;br /&gt;
|-&lt;br /&gt;
|2582&lt;br /&gt;
|0&lt;br /&gt;
|A&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;&#039;&lt;br /&gt;
|No&lt;br /&gt;
|Symmetric stretch&lt;br /&gt;
|-&lt;br /&gt;
|2716&lt;br /&gt;
|126&lt;br /&gt;
|E&#039;&lt;br /&gt;
|Yes&lt;br /&gt;
|Asymmetric stretch&lt;br /&gt;
|-&lt;br /&gt;
|2716&lt;br /&gt;
|126&lt;br /&gt;
|E&#039;&lt;br /&gt;
|Yes&lt;br /&gt;
|Asymmetric stretch&lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;IR spectrum&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
[[file:Hyc116_ir_bh3.png|400*600]]&lt;br /&gt;
&lt;br /&gt;
There are only three peaks on the IR spectrum of BH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;, despite that there are 6 vibrational modes for the molecule. As shown in the table above, the symmetric stretching mode with A1 symmetry at 2582 cm&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt; is not IR active; naturally, that vibrational mode doesn’t give a peak on the IR spectrum. As shown from the table, two pairs of vibrational modes, the bond angle deformation/bend at 1213 cm&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt; and the asymmetric bond stretch at 2716 cm&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;, are degenerate with the symmetry label E. This means that they have the same energy, and hence give the same wavenumber on the IR spectrum. Each pair of degenerate vibrational modes give rise to one peak. This leaves three peaks, as confirmed by the IR spectrum above.&lt;br /&gt;
&lt;br /&gt;
===Molecular orbitals of BH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;===&lt;br /&gt;
&lt;br /&gt;
[[file:hyc116_bh3_MO_diagram.png]]&lt;br /&gt;
&lt;br /&gt;
The above molecular orbital diagram was taken from Dr Patricia Hunt&#039;s &amp;lt;i&amp;gt;Lecture 4 Tutorial Problem Model Answers&amp;lt;/i&amp;gt;.&amp;lt;ref&amp;gt;P. Hunt, &amp;quot;Lecture 4 Tutorial Problem Model Answers&amp;quot;, 2 (2018)&amp;lt;/ref&amp;gt; Diagrams of the &amp;quot;real&amp;quot; MOs were obtained from Gaussian.&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
There is no significant difference between the LCAO MOs and the real ones. Features such as orbital phases are shown clearly on both the LCAO MOs and the real MOs, illustrating the bonding/anti-bonding characters of the molecular orbitals. This suggests that the the qualitative MO theory is highly accurate and useful when studying the molecular orbitals of molecules.&lt;br /&gt;
&lt;br /&gt;
==Associated energies: ammonium borane==&lt;br /&gt;
&lt;br /&gt;
===NH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;===&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;Calculation type&amp;lt;/b&amp;gt;: Optimisation&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;Calculation Method&amp;lt;/b&amp;gt;: B3LYP&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;Basis set&amp;lt;/b&amp;gt;: 6-31G(d,p) &lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Summary table&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
[[file:Hyc116_nh3_631g_summarytable.png]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Items table&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;pre&amp;gt;&lt;br /&gt;
Item               Value     Threshold  Converged?&lt;br /&gt;
 Maximum Force            0.000006     0.000450     YES&lt;br /&gt;
 RMS     Force            0.000004     0.000300     YES&lt;br /&gt;
 Maximum Displacement     0.000012     0.001800     YES&lt;br /&gt;
 RMS     Displacement     0.000008     0.001200     YES&lt;br /&gt;
&amp;lt;/pre&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Frequency log file&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
[[Media:HYC116_NH3_FREQ.LOG]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Frequencies&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;pre&amp;gt;&lt;br /&gt;
Low frequencies ---   -8.5646   -8.5588   -0.0047    0.0454    0.1784   26.4183&lt;br /&gt;
Low frequencies --- 1089.7603 1694.1865 1694.1865&lt;br /&gt;
&amp;lt;/pre&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;jmol of NH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;&#039;&#039;&#039;&lt;br /&gt;
&amp;lt;jmol&amp;gt;&amp;lt;jmolApplet&amp;gt;&lt;br /&gt;
  &amp;lt;title&amp;gt;optimised NH3&amp;lt;/title&amp;gt;&lt;br /&gt;
  &amp;lt;color&amp;gt;black&amp;lt;/color&amp;gt;&lt;br /&gt;
  &amp;lt;size&amp;gt;200&amp;lt;/size&amp;gt;&lt;br /&gt;
  &amp;lt;uploadedFileContents&amp;gt;HYC116_NH3_FREQ.LOG&amp;lt;/uploadedFileContents&amp;gt;&lt;br /&gt;
&amp;lt;/jmolApplet&amp;gt;&amp;lt;/jmol&amp;gt;&lt;br /&gt;
&lt;br /&gt;
===NH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;BH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;===&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;Calculation type&amp;lt;/b&amp;gt;: Optimisation&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;Calculation Method&amp;lt;/b&amp;gt;: B3LYP&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;Basis set&amp;lt;/b&amp;gt;: 6-31G(d,p) &lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Summary table&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
[[file:Hyc116_nh3bh3_631g_summarytable1.png]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Items table&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;pre&amp;gt;&lt;br /&gt;
Item               Value     Threshold  Converged?&lt;br /&gt;
 Maximum Force            0.000121     0.000450     YES&lt;br /&gt;
 RMS     Force            0.000057     0.000300     YES&lt;br /&gt;
 Maximum Displacement     0.000501     0.001800     YES&lt;br /&gt;
 RMS     Displacement     0.000293     0.001200     YES&lt;br /&gt;
&amp;lt;/pre&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Frequency log file&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
[[Media:HYC116_NH3BH3_FREQ1.LOG]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Frequencies&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;pre&amp;gt;&lt;br /&gt;
Low frequencies ---   -0.0574   -0.0501   -0.0074   21.6276   21.6377   40.3839&lt;br /&gt;
Low frequencies ---  265.9973  632.3725  640.1275&lt;br /&gt;
&amp;lt;/pre&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;jmol of NH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;BH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;&#039;&#039;&#039;&lt;br /&gt;
&amp;lt;jmol&amp;gt;&amp;lt;jmolApplet&amp;gt;&lt;br /&gt;
  &amp;lt;title&amp;gt;optimised NH3BH3&amp;lt;/title&amp;gt;&lt;br /&gt;
  &amp;lt;color&amp;gt;black&amp;lt;/color&amp;gt;&lt;br /&gt;
  &amp;lt;size&amp;gt;200&amp;lt;/size&amp;gt;&lt;br /&gt;
  &amp;lt;uploadedFileContents&amp;gt;HYC116_NH3BH3_FREQ.LOG&amp;lt;/uploadedFileContents&amp;gt;&lt;br /&gt;
&amp;lt;/jmolApplet&amp;gt;&amp;lt;/jmol&amp;gt;&lt;br /&gt;
&lt;br /&gt;
===Association energy===&lt;br /&gt;
&lt;br /&gt;
E(BH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;) (using the optimisation with the correct symmetry) = -26.61532363 a.u. = &amp;lt;b&amp;gt;-26.61532 a.u. (5 d.p.)&amp;lt;/b&amp;gt;&lt;br /&gt;
&lt;br /&gt;
E(NH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;) = -56.55776873 a.u. = &amp;lt;b&amp;gt;-56.55777 a.u. (5 d.p.)&amp;lt;/b&amp;gt;&lt;br /&gt;
&lt;br /&gt;
E(NH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;BH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;) = -83.22468892 a.u. = &amp;lt;b&amp;gt;-83.22469 a.u. (5 d.p.)&amp;lt;/b&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
Carrying out calculations using numbers which has already been rounded up can possibly result in errors in the last digit. Hence, here the calculations were carried out using the numbers provided from the optimisations (i.e. with more decimal places than necessary); the answer was then rounded up to the desired accuracy. &lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
ΔE = E(NH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;BH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;)-[E(NH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;)+E(BH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;)]&lt;br /&gt;
&lt;br /&gt;
ΔE = -83.22468892 - (-56.55776873 + -26.61532363) = -0.05159656 a.u. &lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;ΔE = -0.05160 a.u. (5 d.p.)&amp;lt;/b&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Converting energy from a.u. to kJ/mol&#039;&#039;&#039;&lt;br /&gt;
An atomic unit for energy is Hartree, which is equal to 2625.5 kJ/mol.&lt;br /&gt;
&amp;lt;ref&amp;gt;https://cccbdb.nist.gov/hartree.asp (Accessed: 22.05.2018)&amp;lt;/ref&amp;gt;&lt;br /&gt;
 &lt;br /&gt;
&lt;br /&gt;
So ΔE in kJ/mol = -0.05159657 * 2625.5 = -135.46676828 kJ/mol&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;ΔE = -135 kJ/mol (nearest integer)&amp;lt;/b&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
The energy difference calculated above comes from the formation of the B-N dative bond. It is a relatively weak bond. According to a bond energy data sheet provided by the University of California,&amp;lt;ref&amp;gt;https://labs.chem.ucsb.edu/zakarian/armen/11---bonddissociationenergy.pdf (Accessed: 24.05.2018)&amp;lt;/ref&amp;gt;  the bond energy of the C-C bond of an ethane molecule is 368 kJ/mol. This is a fair comparison to the NH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;BH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt; molecule as the two molecules have the same structure, only with the carbon atoms on ethane swapped for Boron and Nitrogen in NH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;BH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;&lt;br /&gt;
&lt;br /&gt;
==Using a mixture of basis-sets and pseudo-potentials==&lt;br /&gt;
&lt;br /&gt;
===BBr&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;===&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;Calculation type&amp;lt;/b&amp;gt;: Optimisation&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;Calculation Method&amp;lt;/b&amp;gt;: B3LYP&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;Basis set&amp;lt;/b&amp;gt;: Boron: 6-31G(d,p) ; Br: LANL2DZ&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
Larger calculations are often sent to a web-server to run on a high-performance computer instead of a desktop. In order to experience and learn to use a web-server, the optimisation and the frequency analysis for BBr&amp;lt;sub&amp;gt;3&amp;lt;/sub were both sent and done on a server instead of the desktop. The calculation results were downloaded from the web-server once they were finished.   &lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Summary table&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
[[file:Hyc116_bbr3_opt_summarytable.png]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Items table&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;pre&amp;gt;&lt;br /&gt;
Item               Value     Threshold  Converged?&lt;br /&gt;
 Maximum Force            0.000008     0.000450     YES&lt;br /&gt;
 RMS     Force            0.000005     0.000300     YES&lt;br /&gt;
 Maximum Displacement     0.000036     0.001800     YES&lt;br /&gt;
 RMS     Displacement     0.000023     0.001200     YES&lt;br /&gt;
&amp;lt;/pre&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Frequency log file&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
[[Media:Hyc116_bbr3_freq.log]]&lt;br /&gt;
&lt;br /&gt;
Attached above is the frequency file saved onto the computer from the SCAN server portal. The frequency file was also published on the chemistry database DSpace. {{DOI|10042/202442}}&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Frequencies&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;pre&amp;gt;&lt;br /&gt;
Low frequencies ---   -0.0137   -0.0064   -0.0046    2.4315    2.4315    4.8421&lt;br /&gt;
Low frequencies ---  155.9631  155.9651  267.7052&lt;br /&gt;
&amp;lt;/pre&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;jmol of BBr&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;&#039;&#039;&#039;&lt;br /&gt;
&amp;lt;jmol&amp;gt;&amp;lt;jmolApplet&amp;gt;&lt;br /&gt;
  &amp;lt;title&amp;gt;optimised BBr3&amp;lt;/title&amp;gt;&lt;br /&gt;
  &amp;lt;color&amp;gt;black&amp;lt;/color&amp;gt;&lt;br /&gt;
  &amp;lt;size&amp;gt;200&amp;lt;/size&amp;gt;&lt;br /&gt;
  &amp;lt;uploadedFileContents&amp;gt;Hyc116_bbr3_freq.log&amp;lt;/uploadedFileContents&amp;gt;&lt;br /&gt;
&amp;lt;/jmolApplet&amp;gt;&amp;lt;/jmol&amp;gt;&lt;br /&gt;
&lt;br /&gt;
==Aromaticity==&lt;br /&gt;
&lt;br /&gt;
===Benzene===&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;Calculation type&amp;lt;/b&amp;gt;: Optimisation&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;Calculation Method&amp;lt;/b&amp;gt;: B3LYP&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;Basis set&amp;lt;/b&amp;gt;: 6-31G(d,p) &lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Summary table&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
[[file:Hyc116_c6h6_summarytable.png]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Items table&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;pre&amp;gt;&lt;br /&gt;
Item               Value     Threshold  Converged?&lt;br /&gt;
 Maximum Force            0.000193     0.000450     YES&lt;br /&gt;
 RMS     Force            0.000079     0.000300     YES&lt;br /&gt;
 Maximum Displacement     0.000830     0.001800     YES&lt;br /&gt;
 RMS     Displacement     0.000294     0.001200     YES&lt;br /&gt;
&amp;lt;/pre&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Frequency log file&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
[[Media:HYC116_C6H6_FREQ.LOG]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Frequencies&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;pre&amp;gt;&lt;br /&gt;
Low frequencies ---   -3.5606   -3.5606   -0.0089   -0.0043   -0.0043   10.0905&lt;br /&gt;
Low frequencies ---  413.9582  413.9582  621.1416&lt;br /&gt;
&amp;lt;/pre&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;jmol of C&amp;lt;sub&amp;gt;6&amp;lt;/sub&amp;gt;H&amp;lt;sub&amp;gt;6&amp;lt;/sub&amp;gt;&#039;&#039;&#039;&lt;br /&gt;
&amp;lt;jmol&amp;gt;&amp;lt;jmolApplet&amp;gt;&lt;br /&gt;
  &amp;lt;title&amp;gt;optimised Benzene&amp;lt;/title&amp;gt;&lt;br /&gt;
  &amp;lt;color&amp;gt;black&amp;lt;/color&amp;gt;&lt;br /&gt;
  &amp;lt;size&amp;gt;200&amp;lt;/size&amp;gt;&lt;br /&gt;
  &amp;lt;uploadedFileContents&amp;gt;HYC116_C6H6_FREQ.LOG&amp;lt;/uploadedFileContents&amp;gt;&lt;br /&gt;
&amp;lt;/jmolApplet&amp;gt;&amp;lt;/jmol&amp;gt;&lt;br /&gt;
&lt;br /&gt;
===Borazine===&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;Calculation type&amp;lt;/b&amp;gt;: Optimisation&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;Calculation Method&amp;lt;/b&amp;gt;: B3LYP&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;Basis set&amp;lt;/b&amp;gt;: 6-31G(d,p) &lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Summary table&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
[[file:Hyc116_borazine_summarytable.png]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Items table&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;pre&amp;gt;&lt;br /&gt;
Item               Value     Threshold  Converged?&lt;br /&gt;
 Maximum Force            0.000085     0.000450     YES&lt;br /&gt;
 RMS     Force            0.000033     0.000300     YES&lt;br /&gt;
 Maximum Displacement     0.000250     0.001800     YES&lt;br /&gt;
 RMS     Displacement     0.000074     0.001200     YES&lt;br /&gt;
&amp;lt;/pre&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Frequency log file&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
[[Media:HYC116_BORAZINE_FREQ.LOG]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Frequencies&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;pre&amp;gt;&lt;br /&gt;
Low frequencies ---  -12.6626  -12.6626   -8.9272   -0.0211   -0.0104   -0.0104&lt;br /&gt;
Low frequencies ---  289.1112  289.1112  403.8613&lt;br /&gt;
&amp;lt;/pre&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;jmol of Borazine&#039;&#039;&#039;&lt;br /&gt;
&amp;lt;jmol&amp;gt;&amp;lt;jmolApplet&amp;gt;&lt;br /&gt;
  &amp;lt;title&amp;gt;optimised Borazine&amp;lt;/title&amp;gt;&lt;br /&gt;
  &amp;lt;color&amp;gt;black&amp;lt;/color&amp;gt;&lt;br /&gt;
  &amp;lt;size&amp;gt;200&amp;lt;/size&amp;gt;&lt;br /&gt;
  &amp;lt;uploadedFileContents&amp;gt;HYC116_BORAZINE_FREQ.LOG&amp;lt;/uploadedFileContents&amp;gt;&lt;br /&gt;
&amp;lt;/jmolApplet&amp;gt;&amp;lt;/jmol&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
===Charge distribution===&lt;br /&gt;
&lt;br /&gt;
An NBO charge analysis was carried out on both the optimised benzene and borazine. Visualisations of the charge distribution are shown in the table below, with the colour range going from -1.102 to 1.102 for both molecule. This large scale was chosen as it allows direct comparison of the charge on any atoms in these two molecules and shows the relative magnitude of charges on all these atoms. Negative charges are shown in red, and positive charges are shown in green. A neutral charge is displayed in black, so the smaller a charge is (positive or negative), the darker its colour representation is. Larger charges are shown in brighter colours. The charges are also displayed on the atoms as numbers with a neutral charge being zero. Negative charges are shown as negative number and positive charges are shown as positive numbers. &lt;br /&gt;
&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot;&lt;br /&gt;
!&lt;br /&gt;
!Benzene&lt;br /&gt;
!Borazine&lt;br /&gt;
|-&lt;br /&gt;
!Visualisation of charge distribution&lt;br /&gt;
|[[File:Hyc116_benzene_charge_distribution1.png|500x500px|thumb|centre|Charge distribution of Benzene visualisation]]&lt;br /&gt;
|[[File:Hyc116_borazine_charge_distribution1.png|500x500px|thumb|centre|Charge distribution of Borazine visualisation]]&lt;br /&gt;
|-&lt;br /&gt;
!Charge &lt;br /&gt;
|Carbon: -0.239&lt;br /&gt;
&lt;br /&gt;
Hydrogen: 0.239&lt;br /&gt;
|Nitrogen: -1.102 &lt;br /&gt;
&lt;br /&gt;
Boron: 0.747&lt;br /&gt;
&lt;br /&gt;
Hydrogen (bonded to N): 0.432&lt;br /&gt;
&lt;br /&gt;
Hydrogen (bonded to B): -0.077&lt;br /&gt;
|-&lt;br /&gt;
!Discussion&lt;br /&gt;
|From the visualisation, it is shown that there is a slightly negative charge on the carbon atoms, and a positive charge of the same magnitude on the hydrogen atoms. All the carbon atoms have the same charge as they are in identical environments. The same applies to all the hydrogen atoms. This is due to the highly symmetrical structure of benzene. Since the same colour scale was used for both benzene and borazine, and the charges are much smaller in magnitude on atoms in benzene than atoms on borazine, the colours on the charge distribution visualisation is much darker. &lt;br /&gt;
|From the colours displayed on the charge distribution visualisation as well as the charge values, it is shown that nitrogen has a relatively large negative charge, while boron has a positive charge. This is due to the difference in electrogenativity between these atoms: nitrogen atoms are more electronegative than boron and tends to attract electrons towards themselves. It is worth noting that the hydrogen atoms do not all have the same charge. The hydrogen atoms bonded to boron have a slightly negative charge, and the ones bonded to nitrogen have a small positive charge. &lt;br /&gt;
&lt;br /&gt;
The fact that the same colour scale was used for both molecules comes in helpful here. It allows the charges on atoms to be compared directly. For example, just from looking at the colours, one can tell that or example, even though both carbon and nitrogen are electronegative, nitrogen is much more electronegative, which is quantitatively shown by Pauling&#039;s electronegativity scale.&amp;lt;ref&amp;gt;http://www.tutor-homework.com/Chemistry_Help/electronegativity_table/electronegativity.html (Accessed: 24.0502018&amp;lt;/ref&amp;gt;&lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
===Comparative MOs of Benzene and Borazine===&lt;br /&gt;
&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot;&lt;br /&gt;
!&lt;br /&gt;
!Benzene&lt;br /&gt;
!Borazine&lt;br /&gt;
!Comparison and Discussion&lt;br /&gt;
|-&lt;br /&gt;
!1st comparative pair&lt;br /&gt;
|[[File:Hyc116_benzene_1st_MO_pair_7.png|200x200px|centre]]&lt;br /&gt;
|[[File:Hyc116_borazine_1st_MO_pair_level9.png|200x200px|centre]]&lt;br /&gt;
|MO 9 of both benzene and borazine are comparable. They both show delocalised molecular orbital with an overall bonding character. There is a nodal plane across the molecular orbitals for both benzene and borazine. For benzene, there is contribution from all the carbon and hydrogen s orbitals. Moreover, the molecular orbitals are symmetric to their counterpart of opposite phase, giving an E&amp;lt;sub&amp;gt;1g&amp;lt;/sub&amp;gt; MO. That is not the case for borazine; they are less symmetric in borazine. Nitrogen atoms are more electronegative than boron atoms and pull electron density towards themselves, resulting in a larger MO. There is contribution from all the boron and nitrogen s orbitals, and three of the hydrogen s orbitals, though not all of them. &lt;br /&gt;
|-&lt;br /&gt;
!2nd comparative pair&lt;br /&gt;
|[[File:Hyc116_benzene_2nd_MO_pair_10.png|200x200px|centre]]&lt;br /&gt;
|[[File:Hyc116_borazine_2nd_MO_pair_level11.png|200x200px|centre]]&lt;br /&gt;
|MO 10 of benzene and MO 11 of borazine are comparable. Here shows a pair of rather delocalised molecular orbitals with slightly more antibonding character than the first pair shown above. On both MOs, there is no contribution from one pair of opposite hydrogen atoms, but contribution from s orbitals of all other atoms on both molecule. The benzene MO has an E&amp;lt;2g&amp;gt; symmetry. In borazine, the lobes are in different sizes due to the higher electronegativity of nitrogen. The lobes at the nitrogen atoms are larger as they attract electrons towards themselves more so than boron atoms do. &lt;br /&gt;
|-&lt;br /&gt;
!3rd comparative pair&lt;br /&gt;
|[[File:Hyc116_benzene_3rd_MO_pair_21.png|200x200px|centre]]&lt;br /&gt;
|[[File:Hyc116_borazine_3rd_MO_pair_level21.png|200x200px|centre]]&lt;br /&gt;
|The HOMO (MO 21) of benzene and the HOMO (MO 21) of borazine are comparable. They are both made of p orbitals of all carbon atoms (or all boron and nitrogen atoms in the case of borazine); there is no contribution from hydrogen atoms as they do not have p orbitals. There is a nodal plan perpendicular to the z axis (highest rotational axis) and one parallel to the z axis. On benzene, the MO is very symmetric and has an E&amp;lt;sub&amp;gt;1g&amp;lt;/sub&amp;gt; symmetry; the lobes of the MO are the same in size. On borazine, the lobe where there are two nitrogen atoms is bigger in size, again due to the higher electronegtivity of nitrogen compared to boron. &lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
===Aromaticity: some theories===&lt;br /&gt;
&lt;br /&gt;
==References==&lt;br /&gt;
{{reflist}}&lt;/div&gt;</summary>
		<author><name>Hyc116</name></author>
	</entry>
	<entry>
		<id>https://chemwiki.ch.ic.ac.uk/index.php?title=MO_hyc116&amp;diff=731351</id>
		<title>MO hyc116</title>
		<link rel="alternate" type="text/html" href="https://chemwiki.ch.ic.ac.uk/index.php?title=MO_hyc116&amp;diff=731351"/>
		<updated>2018-05-25T12:07:51Z</updated>

		<summary type="html">&lt;p&gt;Hyc116: /* NH3BH3 */&lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;==BH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;==&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;Calculation type&amp;lt;/b&amp;gt;: Optimisation&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;Calculation Method&amp;lt;/b&amp;gt;: B3LYP&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;Basis set&amp;lt;/b&amp;gt;: 6-31G(d,p) &lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Summary table&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
[[file:Hyc116_bh3_631g_opt_summarytable.png]]&lt;br /&gt;
&lt;br /&gt;
The above summary table was obtained after the 2nd optimisation of BH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt; (after the initial optimisation using the 3-21G basis set). Notice how the symmetry is incorrect and shown as Cs. This is because the symmetry was manually broken at the beginning by changing the bond length of B-H bonds. The point group was manually adjusted and the molecule was optimised again before the frequency analysis and the new summary table is attached below.&lt;br /&gt;
&lt;br /&gt;
[[file:Hyc116_bh3_correctsummarytable.png]]&lt;br /&gt;
&lt;br /&gt;
The above summary table was obtained from the optimisation after adjusting the symmetry. The point shown in this summary table is D&amp;lt;sub&amp;gt;3h&amp;lt;/sub&amp;gt;, which is the correct for BH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;. &lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Items table&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
Below is the items table taken from the optimisation with the correct point group.&lt;br /&gt;
&lt;br /&gt;
&amp;lt;pre&amp;gt;&lt;br /&gt;
Item               Value     Threshold  Converged?&lt;br /&gt;
 Maximum Force            0.000015     0.000450     YES&lt;br /&gt;
 RMS     Force            0.000010     0.000300     YES&lt;br /&gt;
 Maximum Displacement     0.000058     0.001800     YES&lt;br /&gt;
 RMS     Displacement     0.000038     0.001200     YES&lt;br /&gt;
&amp;lt;/pre&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Frequency log file&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
[[Media:HYC116 BH3 FREQ.LOG]] &lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Frequencies&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;pre&amp;gt;&lt;br /&gt;
Low frequencies ---  -10.3498   -3.4492   -1.2454   -0.0055    0.4779    3.2165&lt;br /&gt;
Low frequencies --- 1162.9519 1213.1527 1213.1554&lt;br /&gt;
&amp;lt;/pre&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;jmol of BH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;&#039;&#039;&#039;&lt;br /&gt;
&amp;lt;jmol&amp;gt;&amp;lt;jmolApplet&amp;gt;&lt;br /&gt;
  &amp;lt;title&amp;gt;optimised BH3&amp;lt;/title&amp;gt;&lt;br /&gt;
  &amp;lt;color&amp;gt;black&amp;lt;/color&amp;gt;&lt;br /&gt;
  &amp;lt;size&amp;gt;200&amp;lt;/size&amp;gt;&lt;br /&gt;
  &amp;lt;uploadedFileContents&amp;gt;HYC116_BH3_FREQ.LOG&amp;lt;/uploadedFileContents&amp;gt;&lt;br /&gt;
&amp;lt;/jmolApplet&amp;gt;&amp;lt;/jmol&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
===Vibrational spectrum===&lt;br /&gt;
&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot;&lt;br /&gt;
!wavenumber (cm&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;)&lt;br /&gt;
!Intensity (arbitrary units)&lt;br /&gt;
!symmetry&lt;br /&gt;
!IR active?&lt;br /&gt;
!type&lt;br /&gt;
|-&lt;br /&gt;
|1163&lt;br /&gt;
|93&lt;br /&gt;
|A&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;&#039; &#039;&lt;br /&gt;
|Yes&lt;br /&gt;
|Out of plane bend&lt;br /&gt;
|-&lt;br /&gt;
|1213&lt;br /&gt;
|14&lt;br /&gt;
|E&#039;&lt;br /&gt;
|Very slight&lt;br /&gt;
|Bend&lt;br /&gt;
|-&lt;br /&gt;
|1213&lt;br /&gt;
|14&lt;br /&gt;
|E&#039;&lt;br /&gt;
|Very slight&lt;br /&gt;
|Bend&lt;br /&gt;
|-&lt;br /&gt;
|2582&lt;br /&gt;
|0&lt;br /&gt;
|A&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;&#039;&lt;br /&gt;
|No&lt;br /&gt;
|Symmetric stretch&lt;br /&gt;
|-&lt;br /&gt;
|2716&lt;br /&gt;
|126&lt;br /&gt;
|E&#039;&lt;br /&gt;
|Yes&lt;br /&gt;
|Asymmetric stretch&lt;br /&gt;
|-&lt;br /&gt;
|2716&lt;br /&gt;
|126&lt;br /&gt;
|E&#039;&lt;br /&gt;
|Yes&lt;br /&gt;
|Asymmetric stretch&lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;IR spectrum&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
[[file:Hyc116_ir_bh3.png|400*600]]&lt;br /&gt;
&lt;br /&gt;
There are only three peaks on the IR spectrum of BH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;, despite that there are 6 vibrational modes for the molecule. As shown in the table above, the symmetric stretching mode with A1 symmetry at 2582 cm&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt; is not IR active; naturally, that vibrational mode doesn’t give a peak on the IR spectrum. As shown from the table, two pairs of vibrational modes, the bond angle deformation/bend at 1213 cm&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt; and the asymmetric bond stretch at 2716 cm&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;, are degenerate with the symmetry label E. This means that they have the same energy, and hence give the same wavenumber on the IR spectrum. Each pair of degenerate vibrational modes give rise to one peak. This leaves three peaks, as confirmed by the IR spectrum above.&lt;br /&gt;
&lt;br /&gt;
===Molecular orbitals of BH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;===&lt;br /&gt;
&lt;br /&gt;
[[file:hyc116_bh3_MO_diagram.png]]&lt;br /&gt;
&lt;br /&gt;
The above molecular orbital diagram was taken from Dr Patricia Hunt&#039;s &amp;lt;i&amp;gt;Lecture 4 Tutorial Problem Model Answers&amp;lt;/i&amp;gt;.&amp;lt;ref&amp;gt;P. Hunt, &amp;quot;Lecture 4 Tutorial Problem Model Answers&amp;quot;, 2 (2018)&amp;lt;/ref&amp;gt; Diagrams of the &amp;quot;real&amp;quot; MOs were obtained from Gaussian.&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
There is no significant difference between the LCAO MOs and the real ones. Features such as orbital phases are shown clearly on both the LCAO MOs and the real MOs, illustrating the bonding/anti-bonding characters of the molecular orbitals. This suggests that the the qualitative MO theory is highly accurate and useful when studying the molecular orbitals of molecules.&lt;br /&gt;
&lt;br /&gt;
==Associated energies: ammonium borane==&lt;br /&gt;
&lt;br /&gt;
===NH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;===&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;Calculation type&amp;lt;/b&amp;gt;: Optimisation&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;Calculation Method&amp;lt;/b&amp;gt;: B3LYP&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;Basis set&amp;lt;/b&amp;gt;: 6-31G(d,p) &lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Summary table&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
[[file:Hyc116_nh3_631g_summarytable.png]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Items table&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;pre&amp;gt;&lt;br /&gt;
Item               Value     Threshold  Converged?&lt;br /&gt;
 Maximum Force            0.000006     0.000450     YES&lt;br /&gt;
 RMS     Force            0.000004     0.000300     YES&lt;br /&gt;
 Maximum Displacement     0.000012     0.001800     YES&lt;br /&gt;
 RMS     Displacement     0.000008     0.001200     YES&lt;br /&gt;
&amp;lt;/pre&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Frequency log file&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
[[Media:HYC116_NH3_FREQ.LOG]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Frequencies&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;pre&amp;gt;&lt;br /&gt;
Low frequencies ---   -8.5646   -8.5588   -0.0047    0.0454    0.1784   26.4183&lt;br /&gt;
Low frequencies --- 1089.7603 1694.1865 1694.1865&lt;br /&gt;
&amp;lt;/pre&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;jmol of NH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;&#039;&#039;&#039;&lt;br /&gt;
&amp;lt;jmol&amp;gt;&amp;lt;jmolApplet&amp;gt;&lt;br /&gt;
  &amp;lt;title&amp;gt;optimised NH3&amp;lt;/title&amp;gt;&lt;br /&gt;
  &amp;lt;color&amp;gt;black&amp;lt;/color&amp;gt;&lt;br /&gt;
  &amp;lt;size&amp;gt;200&amp;lt;/size&amp;gt;&lt;br /&gt;
  &amp;lt;uploadedFileContents&amp;gt;HYC116_NH3_FREQ.LOG&amp;lt;/uploadedFileContents&amp;gt;&lt;br /&gt;
&amp;lt;/jmolApplet&amp;gt;&amp;lt;/jmol&amp;gt;&lt;br /&gt;
&lt;br /&gt;
===NH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;BH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;===&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;Calculation type&amp;lt;/b&amp;gt;: Optimisation&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;Calculation Method&amp;lt;/b&amp;gt;: B3LYP&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;Basis set&amp;lt;/b&amp;gt;: 6-31G(d,p) &lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Summary table&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
[[file:Hyc116_nh3bh3_631g_summarytable1.png]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Items table&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;pre&amp;gt;&lt;br /&gt;
Item               Value     Threshold  Converged?&lt;br /&gt;
 Maximum Force            0.000121     0.000450     YES&lt;br /&gt;
 RMS     Force            0.000057     0.000300     YES&lt;br /&gt;
 Maximum Displacement     0.000501     0.001800     YES&lt;br /&gt;
 RMS     Displacement     0.000293     0.001200     YES&lt;br /&gt;
&amp;lt;/pre&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Frequency log file&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
[[Media:HYC116_NH3BH3_FREQ1.LOG]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Frequencies&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;pre&amp;gt;&lt;br /&gt;
Low frequencies ---   -0.0574   -0.0501   -0.0074   21.6276   21.6377   40.3839&lt;br /&gt;
Low frequencies ---  265.9973  632.3725  640.1275&lt;br /&gt;
&amp;lt;/pre&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;jmol of NH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;BH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;&#039;&#039;&#039;&lt;br /&gt;
&amp;lt;jmol&amp;gt;&amp;lt;jmolApplet&amp;gt;&lt;br /&gt;
  &amp;lt;title&amp;gt;optimised NH3BH3&amp;lt;/title&amp;gt;&lt;br /&gt;
  &amp;lt;color&amp;gt;black&amp;lt;/color&amp;gt;&lt;br /&gt;
  &amp;lt;size&amp;gt;200&amp;lt;/size&amp;gt;&lt;br /&gt;
  &amp;lt;uploadedFileContents&amp;gt;HYC116_NH3BH3_FREQ.LOG&amp;lt;/uploadedFileContents&amp;gt;&lt;br /&gt;
&amp;lt;/jmolApplet&amp;gt;&amp;lt;/jmol&amp;gt;&lt;br /&gt;
&lt;br /&gt;
===Association energy===&lt;br /&gt;
&lt;br /&gt;
E(BH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;) (using the optimisation with the correct symmetry) = -26.61532363 a.u. = &amp;lt;b&amp;gt;-26.61532 a.u. (5 d.p.)&amp;lt;/b&amp;gt;&lt;br /&gt;
&lt;br /&gt;
E(NH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;) = -56.55776873 a.u. = &amp;lt;b&amp;gt;-56.55777 a.u. (5 d.p.)&amp;lt;/b&amp;gt;&lt;br /&gt;
&lt;br /&gt;
E(NH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;BH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;) = -83.22468892 a.u. = &amp;lt;b&amp;gt;-83.22469 a.u. (5 d.p.)&amp;lt;/b&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
Carrying out calculations using numbers which has already been rounded up can possibly result in errors in the last digit. Hence, here the calculations were carried out using the numbers provided from the optimisations (i.e. with more decimal places than necessary); the answer was then rounded up to the desired accuracy. &lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
ΔE = E(NH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;BH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;)-[E(NH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;)+E(BH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;)]&lt;br /&gt;
&lt;br /&gt;
ΔE = -83.22468892 - (-56.55776873 + -26.61532363) = -0.05159656 a.u. &lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;ΔE = -0.05160 a.u. (5 d.p.)&amp;lt;/b&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Converting energy from a.u. to kJ/mol&#039;&#039;&#039;&lt;br /&gt;
An atomic unit for energy is Hartree, which is equal to 2625.5 kJ/mol.&lt;br /&gt;
&amp;lt;ref&amp;gt;https://cccbdb.nist.gov/hartree.asp (Accessed: 22.05.2018)&amp;lt;/ref&amp;gt;&lt;br /&gt;
 &lt;br /&gt;
&lt;br /&gt;
So ΔE in kJ/mol = -0.05159657 * 2625.5 = -135.46676828 kJ/mol&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;ΔE = -135 kJ/mol (nearest integer)&amp;lt;/b&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
The energy difference calculated above comes from the formation of the B-N dative bond. It is a relatively weak bond. According to a bond energy data sheet provided by the University of California,&amp;lt;ref&amp;gt;https://labs.chem.ucsb.edu/zakarian/armen/11---bonddissociationenergy.pdf (Accessed: 24.05.2018)&amp;lt;/ref&amp;gt;  the bond energy of the C-C bond of an ethane molecule is 368 kJ/mol. This is a fair comparison to the NH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;BH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt; molecule as the two molecules have the same structure, only with the carbon atoms on ethane swapped for Boron and Nitrogen in NH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;BH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;&lt;br /&gt;
&lt;br /&gt;
==Using a mixture of basis-sets and pseudo-potentials==&lt;br /&gt;
&lt;br /&gt;
===BBr&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;===&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;Calculation type&amp;lt;/b&amp;gt;: Optimisation&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;Calculation Method&amp;lt;/b&amp;gt;: B3LYP&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;Basis set&amp;lt;/b&amp;gt;: Boron: 6-31G(d,p) ; Br: LANL2DZ&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
Larger calculations are often sent to a web-server to run on a high-performance computer instead of a desktop. In order to experience and learn to use a web-server, the optimisation and the frequency analysis for BBr&amp;lt;sub&amp;gt;3&amp;lt;/sub were both sent and done on a server instead of the desktop. The calculation results were downloaded from the web-server once they were finished.   &lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Summary table&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
[[file:Hyc116_bbr3_opt_summarytable.png]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Items table&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;pre&amp;gt;&lt;br /&gt;
Item               Value     Threshold  Converged?&lt;br /&gt;
 Maximum Force            0.000008     0.000450     YES&lt;br /&gt;
 RMS     Force            0.000005     0.000300     YES&lt;br /&gt;
 Maximum Displacement     0.000036     0.001800     YES&lt;br /&gt;
 RMS     Displacement     0.000023     0.001200     YES&lt;br /&gt;
&amp;lt;/pre&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Frequency log file&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
[[Media:Hyc116_bbr3_freq.log]]&lt;br /&gt;
&lt;br /&gt;
Attached above is the frequency file saved onto the computer from the SCAN server portal. The frequency file was also published on the chemistry database DSpace. {{DOI|10042/202442}}&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Frequencies&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;pre&amp;gt;&lt;br /&gt;
Low frequencies ---   -0.0137   -0.0064   -0.0046    2.4315    2.4315    4.8421&lt;br /&gt;
Low frequencies ---  155.9631  155.9651  267.7052&lt;br /&gt;
&amp;lt;/pre&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;jmol of BBr&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;&#039;&#039;&#039;&lt;br /&gt;
&amp;lt;jmol&amp;gt;&amp;lt;jmolApplet&amp;gt;&lt;br /&gt;
  &amp;lt;title&amp;gt;optimised BBr3&amp;lt;/title&amp;gt;&lt;br /&gt;
  &amp;lt;color&amp;gt;black&amp;lt;/color&amp;gt;&lt;br /&gt;
  &amp;lt;size&amp;gt;200&amp;lt;/size&amp;gt;&lt;br /&gt;
  &amp;lt;uploadedFileContents&amp;gt;Hyc116_bbr3_freq.log&amp;lt;/uploadedFileContents&amp;gt;&lt;br /&gt;
&amp;lt;/jmolApplet&amp;gt;&amp;lt;/jmol&amp;gt;&lt;br /&gt;
&lt;br /&gt;
==Aromaticity==&lt;br /&gt;
&lt;br /&gt;
===Benzene===&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;Calculation type&amp;lt;/b&amp;gt;: Optimisation&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;Calculation Method&amp;lt;/b&amp;gt;: B3LYP&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;Basis set&amp;lt;/b&amp;gt;: 6-31G(d,p) &lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Summary table&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
[[file:Hyc116_c6h6_summarytable.png]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Items table&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;pre&amp;gt;&lt;br /&gt;
Item               Value     Threshold  Converged?&lt;br /&gt;
 Maximum Force            0.000193     0.000450     YES&lt;br /&gt;
 RMS     Force            0.000079     0.000300     YES&lt;br /&gt;
 Maximum Displacement     0.000830     0.001800     YES&lt;br /&gt;
 RMS     Displacement     0.000294     0.001200     YES&lt;br /&gt;
&amp;lt;/pre&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Frequency log file&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
[[Media:HYC116_C6H6_FREQ.LOG]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Frequencies&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;pre&amp;gt;&lt;br /&gt;
Low frequencies ---   -3.5606   -3.5606   -0.0089   -0.0043   -0.0043   10.0905&lt;br /&gt;
Low frequencies ---  413.9582  413.9582  621.1416&lt;br /&gt;
&amp;lt;/pre&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;jmol of C&amp;lt;sub&amp;gt;6&amp;lt;/sub&amp;gt;H&amp;lt;sub&amp;gt;6&amp;lt;/sub&amp;gt;&#039;&#039;&#039;&lt;br /&gt;
&amp;lt;jmol&amp;gt;&amp;lt;jmolApplet&amp;gt;&lt;br /&gt;
  &amp;lt;title&amp;gt;optimised Benzene&amp;lt;/title&amp;gt;&lt;br /&gt;
  &amp;lt;color&amp;gt;black&amp;lt;/color&amp;gt;&lt;br /&gt;
  &amp;lt;size&amp;gt;200&amp;lt;/size&amp;gt;&lt;br /&gt;
  &amp;lt;uploadedFileContents&amp;gt;HYC116_C6H6_FREQ.LOG&amp;lt;/uploadedFileContents&amp;gt;&lt;br /&gt;
&amp;lt;/jmolApplet&amp;gt;&amp;lt;/jmol&amp;gt;&lt;br /&gt;
&lt;br /&gt;
===Borazine===&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;Calculation type&amp;lt;/b&amp;gt;: Optimisation&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;Calculation Method&amp;lt;/b&amp;gt;: B3LYP&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;Basis set&amp;lt;/b&amp;gt;: 6-31G(d,p) &lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Summary table&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
[[file:Hyc116_borazine_summarytable.png]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Items table&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;pre&amp;gt;&lt;br /&gt;
Item               Value     Threshold  Converged?&lt;br /&gt;
 Maximum Force            0.000085     0.000450     YES&lt;br /&gt;
 RMS     Force            0.000033     0.000300     YES&lt;br /&gt;
 Maximum Displacement     0.000250     0.001800     YES&lt;br /&gt;
 RMS     Displacement     0.000074     0.001200     YES&lt;br /&gt;
&amp;lt;/pre&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Frequency log file&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
[[Media:HYC116_BORAZINE_FREQ.LOG]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Frequencies&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;pre&amp;gt;&lt;br /&gt;
Low frequencies ---  -12.6626  -12.6626   -8.9272   -0.0211   -0.0104   -0.0104&lt;br /&gt;
Low frequencies ---  289.1112  289.1112  403.8613&lt;br /&gt;
&amp;lt;/pre&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;jmol of Borazine&#039;&#039;&#039;&lt;br /&gt;
&amp;lt;jmol&amp;gt;&amp;lt;jmolApplet&amp;gt;&lt;br /&gt;
  &amp;lt;title&amp;gt;optimised Borazine&amp;lt;/title&amp;gt;&lt;br /&gt;
  &amp;lt;color&amp;gt;black&amp;lt;/color&amp;gt;&lt;br /&gt;
  &amp;lt;size&amp;gt;200&amp;lt;/size&amp;gt;&lt;br /&gt;
  &amp;lt;uploadedFileContents&amp;gt;HYC116_BORAZINE_FREQ.LOG&amp;lt;/uploadedFileContents&amp;gt;&lt;br /&gt;
&amp;lt;/jmolApplet&amp;gt;&amp;lt;/jmol&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
===Charge distribution===&lt;br /&gt;
&lt;br /&gt;
An NBO charge analysis was carried out on both the optimised benzene and borazine. Visualisations of the charge distribution are shown in the table below, with the colour range going from -1.102 to 1.102 for both molecule. This large scale was chosen as it allows direct comparison of the charge on any atoms in these two molecules and shows the relative magnitude of charges on all these atoms. Negative charges are shown in red, and positive charges are shown in green. A neutral charge is displayed in black, so the smaller a charge is (positive or negative), the darker its colour representation is. Larger charges are shown in brighter colours. The charges are also displayed on the atoms as numbers with a neutral charge being zero. Negative charges are shown as negative number and positive charges are shown as positive numbers. &lt;br /&gt;
&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot;&lt;br /&gt;
!&lt;br /&gt;
!Benzene&lt;br /&gt;
!Borazine&lt;br /&gt;
|-&lt;br /&gt;
!Visualisation of charge distribution&lt;br /&gt;
|[[File:Hyc116_benzene_charge_distribution1.png|500x500px|thumb|centre|Charge distribution of Benzene visualisation]]&lt;br /&gt;
|[[File:Hyc116_borazine_charge_distribution1.png|500x500px|thumb|centre|Charge distribution of Borazine visualisation]]&lt;br /&gt;
|-&lt;br /&gt;
!Charge &lt;br /&gt;
|Carbon: -0.239&lt;br /&gt;
&lt;br /&gt;
Hydrogen: 0.239&lt;br /&gt;
|Nitrogen: -1.102 &lt;br /&gt;
&lt;br /&gt;
Boron: 0.747&lt;br /&gt;
&lt;br /&gt;
Hydrogen (bonded to N): 0.432&lt;br /&gt;
&lt;br /&gt;
Hydrogen (bonded to B): -0.077&lt;br /&gt;
|-&lt;br /&gt;
!Discussion&lt;br /&gt;
|From the visualisation, it is shown that there is a slightly negative charge on the carbon atoms, and a positive charge of the same magnitude on the hydrogen atoms. All the carbon atoms have the same charge as they are in identical environments. The same applies to all the hydrogen atoms. This is due to the highly symmetrical structure of benzene. Since the same colour scale was used for both benzene and borazine, and the charges are much smaller in magnitude on atoms in benzene than atoms on borazine, the colours on the charge distribution visualisation is much darker. &lt;br /&gt;
|From the colours displayed on the charge distribution visualisation as well as the charge values, it is shown that nitrogen has a relatively large negative charge, while boron has a positive charge. This is due to the difference in electrogenativity between these atoms: nitrogen atoms are more electronegative than boron and tends to attract electrons towards themselves. It is worth noting that the hydrogen atoms do not all have the same charge. The hydrogen atoms bonded to boron have a slightly negative charge, and the ones bonded to nitrogen have a small positive charge. &lt;br /&gt;
&lt;br /&gt;
The fact that the same colour scale was used for both molecules comes in helpful here. It allows the charges on atoms to be compared directly. For example, just from looking at the colours, one can tell that or example, even though both carbon and nitrogen are electronegative, nitrogen is much more electronegative, which is quantitatively shown by Pauling&#039;s electronegativity scale.&amp;lt;ref&amp;gt;http://www.tutor-homework.com/Chemistry_Help/electronegativity_table/electronegativity.html (Accessed: 24.0502018&amp;lt;/ref&amp;gt;&lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
===Comparative MOs of Benzene and Borazine===&lt;br /&gt;
&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot;&lt;br /&gt;
!&lt;br /&gt;
!Benzene&lt;br /&gt;
!Borazine&lt;br /&gt;
!Comparison and Discussion&lt;br /&gt;
|-&lt;br /&gt;
!1st comparative pair&lt;br /&gt;
|[[File:Hyc116_benzene_1st_MO_pair_7.png|200x200px|centre]]&lt;br /&gt;
|[[File:Hyc116_borazine_1st_MO_pair_level9.png|200x200px|centre]]&lt;br /&gt;
|MO 9 of both benzene and borazine are comparable. They both show delocalised molecular orbital with an overall bonding character. There is a nodal plane across the molecular orbitals for both benzene and borazine. For benzene, there is contribution from all the carbon and hydrogen s orbitals. Moreover, the molecular orbitals are symmetric to their counterpart of opposite phase. That is not the case for borazine; they are less symmetric in borazine. Nitrogen atoms are more electronegative than boron atoms and pull electron density towards themselves, resulting in a larger MO. There is contribution from all the boron and nitrogen s orbitals, and three of the hydrogen s orbitals, though not all of them. &lt;br /&gt;
|-&lt;br /&gt;
!2nd comparative pair&lt;br /&gt;
|[[File:Hyc116_benzene_2nd_MO_pair_10.png|200x200px|centre]]&lt;br /&gt;
|[[File:Hyc116_borazine_2nd_MO_pair_level11.png|200x200px|centre]]&lt;br /&gt;
|&lt;br /&gt;
|-&lt;br /&gt;
!3rd comparative pair&lt;br /&gt;
|[[File:Hyc116_benzene_3rd_MO_pair_21.png|200x200px|centre]]&lt;br /&gt;
|[[File:Hyc116_borazine_3rd_MO_pair_level21.png|200x200px|centre]]&lt;br /&gt;
|&lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
===Aromaticity: some theories===&lt;br /&gt;
&lt;br /&gt;
==References==&lt;br /&gt;
{{reflist}}&lt;/div&gt;</summary>
		<author><name>Hyc116</name></author>
	</entry>
	<entry>
		<id>https://chemwiki.ch.ic.ac.uk/index.php?title=File:HYC116_NH3BH3_FREQ1.LOG&amp;diff=731349</id>
		<title>File:HYC116 NH3BH3 FREQ1.LOG</title>
		<link rel="alternate" type="text/html" href="https://chemwiki.ch.ic.ac.uk/index.php?title=File:HYC116_NH3BH3_FREQ1.LOG&amp;diff=731349"/>
		<updated>2018-05-25T12:07:39Z</updated>

		<summary type="html">&lt;p&gt;Hyc116: &lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;&lt;/div&gt;</summary>
		<author><name>Hyc116</name></author>
	</entry>
	<entry>
		<id>https://chemwiki.ch.ic.ac.uk/index.php?title=MO_hyc116&amp;diff=731347</id>
		<title>MO hyc116</title>
		<link rel="alternate" type="text/html" href="https://chemwiki.ch.ic.ac.uk/index.php?title=MO_hyc116&amp;diff=731347"/>
		<updated>2018-05-25T12:06:48Z</updated>

		<summary type="html">&lt;p&gt;Hyc116: /* NH3BH3 */&lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;==BH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;==&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;Calculation type&amp;lt;/b&amp;gt;: Optimisation&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;Calculation Method&amp;lt;/b&amp;gt;: B3LYP&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;Basis set&amp;lt;/b&amp;gt;: 6-31G(d,p) &lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Summary table&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
[[file:Hyc116_bh3_631g_opt_summarytable.png]]&lt;br /&gt;
&lt;br /&gt;
The above summary table was obtained after the 2nd optimisation of BH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt; (after the initial optimisation using the 3-21G basis set). Notice how the symmetry is incorrect and shown as Cs. This is because the symmetry was manually broken at the beginning by changing the bond length of B-H bonds. The point group was manually adjusted and the molecule was optimised again before the frequency analysis and the new summary table is attached below.&lt;br /&gt;
&lt;br /&gt;
[[file:Hyc116_bh3_correctsummarytable.png]]&lt;br /&gt;
&lt;br /&gt;
The above summary table was obtained from the optimisation after adjusting the symmetry. The point shown in this summary table is D&amp;lt;sub&amp;gt;3h&amp;lt;/sub&amp;gt;, which is the correct for BH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;. &lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Items table&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
Below is the items table taken from the optimisation with the correct point group.&lt;br /&gt;
&lt;br /&gt;
&amp;lt;pre&amp;gt;&lt;br /&gt;
Item               Value     Threshold  Converged?&lt;br /&gt;
 Maximum Force            0.000015     0.000450     YES&lt;br /&gt;
 RMS     Force            0.000010     0.000300     YES&lt;br /&gt;
 Maximum Displacement     0.000058     0.001800     YES&lt;br /&gt;
 RMS     Displacement     0.000038     0.001200     YES&lt;br /&gt;
&amp;lt;/pre&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Frequency log file&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
[[Media:HYC116 BH3 FREQ.LOG]] &lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Frequencies&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;pre&amp;gt;&lt;br /&gt;
Low frequencies ---  -10.3498   -3.4492   -1.2454   -0.0055    0.4779    3.2165&lt;br /&gt;
Low frequencies --- 1162.9519 1213.1527 1213.1554&lt;br /&gt;
&amp;lt;/pre&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;jmol of BH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;&#039;&#039;&#039;&lt;br /&gt;
&amp;lt;jmol&amp;gt;&amp;lt;jmolApplet&amp;gt;&lt;br /&gt;
  &amp;lt;title&amp;gt;optimised BH3&amp;lt;/title&amp;gt;&lt;br /&gt;
  &amp;lt;color&amp;gt;black&amp;lt;/color&amp;gt;&lt;br /&gt;
  &amp;lt;size&amp;gt;200&amp;lt;/size&amp;gt;&lt;br /&gt;
  &amp;lt;uploadedFileContents&amp;gt;HYC116_BH3_FREQ.LOG&amp;lt;/uploadedFileContents&amp;gt;&lt;br /&gt;
&amp;lt;/jmolApplet&amp;gt;&amp;lt;/jmol&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
===Vibrational spectrum===&lt;br /&gt;
&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot;&lt;br /&gt;
!wavenumber (cm&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;)&lt;br /&gt;
!Intensity (arbitrary units)&lt;br /&gt;
!symmetry&lt;br /&gt;
!IR active?&lt;br /&gt;
!type&lt;br /&gt;
|-&lt;br /&gt;
|1163&lt;br /&gt;
|93&lt;br /&gt;
|A&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;&#039; &#039;&lt;br /&gt;
|Yes&lt;br /&gt;
|Out of plane bend&lt;br /&gt;
|-&lt;br /&gt;
|1213&lt;br /&gt;
|14&lt;br /&gt;
|E&#039;&lt;br /&gt;
|Very slight&lt;br /&gt;
|Bend&lt;br /&gt;
|-&lt;br /&gt;
|1213&lt;br /&gt;
|14&lt;br /&gt;
|E&#039;&lt;br /&gt;
|Very slight&lt;br /&gt;
|Bend&lt;br /&gt;
|-&lt;br /&gt;
|2582&lt;br /&gt;
|0&lt;br /&gt;
|A&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;&#039;&lt;br /&gt;
|No&lt;br /&gt;
|Symmetric stretch&lt;br /&gt;
|-&lt;br /&gt;
|2716&lt;br /&gt;
|126&lt;br /&gt;
|E&#039;&lt;br /&gt;
|Yes&lt;br /&gt;
|Asymmetric stretch&lt;br /&gt;
|-&lt;br /&gt;
|2716&lt;br /&gt;
|126&lt;br /&gt;
|E&#039;&lt;br /&gt;
|Yes&lt;br /&gt;
|Asymmetric stretch&lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;IR spectrum&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
[[file:Hyc116_ir_bh3.png|400*600]]&lt;br /&gt;
&lt;br /&gt;
There are only three peaks on the IR spectrum of BH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;, despite that there are 6 vibrational modes for the molecule. As shown in the table above, the symmetric stretching mode with A1 symmetry at 2582 cm&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt; is not IR active; naturally, that vibrational mode doesn’t give a peak on the IR spectrum. As shown from the table, two pairs of vibrational modes, the bond angle deformation/bend at 1213 cm&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt; and the asymmetric bond stretch at 2716 cm&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;, are degenerate with the symmetry label E. This means that they have the same energy, and hence give the same wavenumber on the IR spectrum. Each pair of degenerate vibrational modes give rise to one peak. This leaves three peaks, as confirmed by the IR spectrum above.&lt;br /&gt;
&lt;br /&gt;
===Molecular orbitals of BH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;===&lt;br /&gt;
&lt;br /&gt;
[[file:hyc116_bh3_MO_diagram.png]]&lt;br /&gt;
&lt;br /&gt;
The above molecular orbital diagram was taken from Dr Patricia Hunt&#039;s &amp;lt;i&amp;gt;Lecture 4 Tutorial Problem Model Answers&amp;lt;/i&amp;gt;.&amp;lt;ref&amp;gt;P. Hunt, &amp;quot;Lecture 4 Tutorial Problem Model Answers&amp;quot;, 2 (2018)&amp;lt;/ref&amp;gt; Diagrams of the &amp;quot;real&amp;quot; MOs were obtained from Gaussian.&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
There is no significant difference between the LCAO MOs and the real ones. Features such as orbital phases are shown clearly on both the LCAO MOs and the real MOs, illustrating the bonding/anti-bonding characters of the molecular orbitals. This suggests that the the qualitative MO theory is highly accurate and useful when studying the molecular orbitals of molecules.&lt;br /&gt;
&lt;br /&gt;
==Associated energies: ammonium borane==&lt;br /&gt;
&lt;br /&gt;
===NH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;===&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;Calculation type&amp;lt;/b&amp;gt;: Optimisation&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;Calculation Method&amp;lt;/b&amp;gt;: B3LYP&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;Basis set&amp;lt;/b&amp;gt;: 6-31G(d,p) &lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Summary table&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
[[file:Hyc116_nh3_631g_summarytable.png]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Items table&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;pre&amp;gt;&lt;br /&gt;
Item               Value     Threshold  Converged?&lt;br /&gt;
 Maximum Force            0.000006     0.000450     YES&lt;br /&gt;
 RMS     Force            0.000004     0.000300     YES&lt;br /&gt;
 Maximum Displacement     0.000012     0.001800     YES&lt;br /&gt;
 RMS     Displacement     0.000008     0.001200     YES&lt;br /&gt;
&amp;lt;/pre&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Frequency log file&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
[[Media:HYC116_NH3_FREQ.LOG]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Frequencies&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;pre&amp;gt;&lt;br /&gt;
Low frequencies ---   -8.5646   -8.5588   -0.0047    0.0454    0.1784   26.4183&lt;br /&gt;
Low frequencies --- 1089.7603 1694.1865 1694.1865&lt;br /&gt;
&amp;lt;/pre&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;jmol of NH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;&#039;&#039;&#039;&lt;br /&gt;
&amp;lt;jmol&amp;gt;&amp;lt;jmolApplet&amp;gt;&lt;br /&gt;
  &amp;lt;title&amp;gt;optimised NH3&amp;lt;/title&amp;gt;&lt;br /&gt;
  &amp;lt;color&amp;gt;black&amp;lt;/color&amp;gt;&lt;br /&gt;
  &amp;lt;size&amp;gt;200&amp;lt;/size&amp;gt;&lt;br /&gt;
  &amp;lt;uploadedFileContents&amp;gt;HYC116_NH3_FREQ.LOG&amp;lt;/uploadedFileContents&amp;gt;&lt;br /&gt;
&amp;lt;/jmolApplet&amp;gt;&amp;lt;/jmol&amp;gt;&lt;br /&gt;
&lt;br /&gt;
===NH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;BH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;===&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;Calculation type&amp;lt;/b&amp;gt;: Optimisation&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;Calculation Method&amp;lt;/b&amp;gt;: B3LYP&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;Basis set&amp;lt;/b&amp;gt;: 6-31G(d,p) &lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Summary table&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
[[file:Hyc116_nh3bh3_631g_summarytable1.png]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Items table&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;pre&amp;gt;&lt;br /&gt;
Item               Value     Threshold  Converged?&lt;br /&gt;
 Maximum Force            0.000121     0.000450     YES&lt;br /&gt;
 RMS     Force            0.000057     0.000300     YES&lt;br /&gt;
 Maximum Displacement     0.000501     0.001800     YES&lt;br /&gt;
 RMS     Displacement     0.000293     0.001200     YES&lt;br /&gt;
&amp;lt;/pre&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Frequency log file&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
[[Media:HYC116_NH3BH3_FREQ.LOG]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Frequencies&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;pre&amp;gt;&lt;br /&gt;
Low frequencies ---   -0.0574   -0.0501   -0.0074   21.6276   21.6377   40.3839&lt;br /&gt;
Low frequencies ---  265.9973  632.3725  640.1275&lt;br /&gt;
&amp;lt;/pre&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;jmol of NH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;BH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;&#039;&#039;&#039;&lt;br /&gt;
&amp;lt;jmol&amp;gt;&amp;lt;jmolApplet&amp;gt;&lt;br /&gt;
  &amp;lt;title&amp;gt;optimised NH3BH3&amp;lt;/title&amp;gt;&lt;br /&gt;
  &amp;lt;color&amp;gt;black&amp;lt;/color&amp;gt;&lt;br /&gt;
  &amp;lt;size&amp;gt;200&amp;lt;/size&amp;gt;&lt;br /&gt;
  &amp;lt;uploadedFileContents&amp;gt;HYC116_NH3BH3_FREQ.LOG&amp;lt;/uploadedFileContents&amp;gt;&lt;br /&gt;
&amp;lt;/jmolApplet&amp;gt;&amp;lt;/jmol&amp;gt;&lt;br /&gt;
&lt;br /&gt;
===Association energy===&lt;br /&gt;
&lt;br /&gt;
E(BH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;) (using the optimisation with the correct symmetry) = -26.61532363 a.u. = &amp;lt;b&amp;gt;-26.61532 a.u. (5 d.p.)&amp;lt;/b&amp;gt;&lt;br /&gt;
&lt;br /&gt;
E(NH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;) = -56.55776873 a.u. = &amp;lt;b&amp;gt;-56.55777 a.u. (5 d.p.)&amp;lt;/b&amp;gt;&lt;br /&gt;
&lt;br /&gt;
E(NH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;BH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;) = -83.22468892 a.u. = &amp;lt;b&amp;gt;-83.22469 a.u. (5 d.p.)&amp;lt;/b&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
Carrying out calculations using numbers which has already been rounded up can possibly result in errors in the last digit. Hence, here the calculations were carried out using the numbers provided from the optimisations (i.e. with more decimal places than necessary); the answer was then rounded up to the desired accuracy. &lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
ΔE = E(NH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;BH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;)-[E(NH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;)+E(BH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;)]&lt;br /&gt;
&lt;br /&gt;
ΔE = -83.22468892 - (-56.55776873 + -26.61532363) = -0.05159656 a.u. &lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;ΔE = -0.05160 a.u. (5 d.p.)&amp;lt;/b&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Converting energy from a.u. to kJ/mol&#039;&#039;&#039;&lt;br /&gt;
An atomic unit for energy is Hartree, which is equal to 2625.5 kJ/mol.&lt;br /&gt;
&amp;lt;ref&amp;gt;https://cccbdb.nist.gov/hartree.asp (Accessed: 22.05.2018)&amp;lt;/ref&amp;gt;&lt;br /&gt;
 &lt;br /&gt;
&lt;br /&gt;
So ΔE in kJ/mol = -0.05159657 * 2625.5 = -135.46676828 kJ/mol&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;ΔE = -135 kJ/mol (nearest integer)&amp;lt;/b&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
The energy difference calculated above comes from the formation of the B-N dative bond. It is a relatively weak bond. According to a bond energy data sheet provided by the University of California,&amp;lt;ref&amp;gt;https://labs.chem.ucsb.edu/zakarian/armen/11---bonddissociationenergy.pdf (Accessed: 24.05.2018)&amp;lt;/ref&amp;gt;  the bond energy of the C-C bond of an ethane molecule is 368 kJ/mol. This is a fair comparison to the NH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;BH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt; molecule as the two molecules have the same structure, only with the carbon atoms on ethane swapped for Boron and Nitrogen in NH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;BH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;&lt;br /&gt;
&lt;br /&gt;
==Using a mixture of basis-sets and pseudo-potentials==&lt;br /&gt;
&lt;br /&gt;
===BBr&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;===&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;Calculation type&amp;lt;/b&amp;gt;: Optimisation&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;Calculation Method&amp;lt;/b&amp;gt;: B3LYP&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;Basis set&amp;lt;/b&amp;gt;: Boron: 6-31G(d,p) ; Br: LANL2DZ&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
Larger calculations are often sent to a web-server to run on a high-performance computer instead of a desktop. In order to experience and learn to use a web-server, the optimisation and the frequency analysis for BBr&amp;lt;sub&amp;gt;3&amp;lt;/sub were both sent and done on a server instead of the desktop. The calculation results were downloaded from the web-server once they were finished.   &lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Summary table&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
[[file:Hyc116_bbr3_opt_summarytable.png]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Items table&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;pre&amp;gt;&lt;br /&gt;
Item               Value     Threshold  Converged?&lt;br /&gt;
 Maximum Force            0.000008     0.000450     YES&lt;br /&gt;
 RMS     Force            0.000005     0.000300     YES&lt;br /&gt;
 Maximum Displacement     0.000036     0.001800     YES&lt;br /&gt;
 RMS     Displacement     0.000023     0.001200     YES&lt;br /&gt;
&amp;lt;/pre&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Frequency log file&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
[[Media:Hyc116_bbr3_freq.log]]&lt;br /&gt;
&lt;br /&gt;
Attached above is the frequency file saved onto the computer from the SCAN server portal. The frequency file was also published on the chemistry database DSpace. {{DOI|10042/202442}}&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Frequencies&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;pre&amp;gt;&lt;br /&gt;
Low frequencies ---   -0.0137   -0.0064   -0.0046    2.4315    2.4315    4.8421&lt;br /&gt;
Low frequencies ---  155.9631  155.9651  267.7052&lt;br /&gt;
&amp;lt;/pre&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;jmol of BBr&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;&#039;&#039;&#039;&lt;br /&gt;
&amp;lt;jmol&amp;gt;&amp;lt;jmolApplet&amp;gt;&lt;br /&gt;
  &amp;lt;title&amp;gt;optimised BBr3&amp;lt;/title&amp;gt;&lt;br /&gt;
  &amp;lt;color&amp;gt;black&amp;lt;/color&amp;gt;&lt;br /&gt;
  &amp;lt;size&amp;gt;200&amp;lt;/size&amp;gt;&lt;br /&gt;
  &amp;lt;uploadedFileContents&amp;gt;Hyc116_bbr3_freq.log&amp;lt;/uploadedFileContents&amp;gt;&lt;br /&gt;
&amp;lt;/jmolApplet&amp;gt;&amp;lt;/jmol&amp;gt;&lt;br /&gt;
&lt;br /&gt;
==Aromaticity==&lt;br /&gt;
&lt;br /&gt;
===Benzene===&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;Calculation type&amp;lt;/b&amp;gt;: Optimisation&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;Calculation Method&amp;lt;/b&amp;gt;: B3LYP&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;Basis set&amp;lt;/b&amp;gt;: 6-31G(d,p) &lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Summary table&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
[[file:Hyc116_c6h6_summarytable.png]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Items table&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;pre&amp;gt;&lt;br /&gt;
Item               Value     Threshold  Converged?&lt;br /&gt;
 Maximum Force            0.000193     0.000450     YES&lt;br /&gt;
 RMS     Force            0.000079     0.000300     YES&lt;br /&gt;
 Maximum Displacement     0.000830     0.001800     YES&lt;br /&gt;
 RMS     Displacement     0.000294     0.001200     YES&lt;br /&gt;
&amp;lt;/pre&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Frequency log file&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
[[Media:HYC116_C6H6_FREQ.LOG]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Frequencies&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;pre&amp;gt;&lt;br /&gt;
Low frequencies ---   -3.5606   -3.5606   -0.0089   -0.0043   -0.0043   10.0905&lt;br /&gt;
Low frequencies ---  413.9582  413.9582  621.1416&lt;br /&gt;
&amp;lt;/pre&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;jmol of C&amp;lt;sub&amp;gt;6&amp;lt;/sub&amp;gt;H&amp;lt;sub&amp;gt;6&amp;lt;/sub&amp;gt;&#039;&#039;&#039;&lt;br /&gt;
&amp;lt;jmol&amp;gt;&amp;lt;jmolApplet&amp;gt;&lt;br /&gt;
  &amp;lt;title&amp;gt;optimised Benzene&amp;lt;/title&amp;gt;&lt;br /&gt;
  &amp;lt;color&amp;gt;black&amp;lt;/color&amp;gt;&lt;br /&gt;
  &amp;lt;size&amp;gt;200&amp;lt;/size&amp;gt;&lt;br /&gt;
  &amp;lt;uploadedFileContents&amp;gt;HYC116_C6H6_FREQ.LOG&amp;lt;/uploadedFileContents&amp;gt;&lt;br /&gt;
&amp;lt;/jmolApplet&amp;gt;&amp;lt;/jmol&amp;gt;&lt;br /&gt;
&lt;br /&gt;
===Borazine===&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;Calculation type&amp;lt;/b&amp;gt;: Optimisation&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;Calculation Method&amp;lt;/b&amp;gt;: B3LYP&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;Basis set&amp;lt;/b&amp;gt;: 6-31G(d,p) &lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Summary table&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
[[file:Hyc116_borazine_summarytable.png]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Items table&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;pre&amp;gt;&lt;br /&gt;
Item               Value     Threshold  Converged?&lt;br /&gt;
 Maximum Force            0.000085     0.000450     YES&lt;br /&gt;
 RMS     Force            0.000033     0.000300     YES&lt;br /&gt;
 Maximum Displacement     0.000250     0.001800     YES&lt;br /&gt;
 RMS     Displacement     0.000074     0.001200     YES&lt;br /&gt;
&amp;lt;/pre&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Frequency log file&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
[[Media:HYC116_BORAZINE_FREQ.LOG]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Frequencies&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;pre&amp;gt;&lt;br /&gt;
Low frequencies ---  -12.6626  -12.6626   -8.9272   -0.0211   -0.0104   -0.0104&lt;br /&gt;
Low frequencies ---  289.1112  289.1112  403.8613&lt;br /&gt;
&amp;lt;/pre&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;jmol of Borazine&#039;&#039;&#039;&lt;br /&gt;
&amp;lt;jmol&amp;gt;&amp;lt;jmolApplet&amp;gt;&lt;br /&gt;
  &amp;lt;title&amp;gt;optimised Borazine&amp;lt;/title&amp;gt;&lt;br /&gt;
  &amp;lt;color&amp;gt;black&amp;lt;/color&amp;gt;&lt;br /&gt;
  &amp;lt;size&amp;gt;200&amp;lt;/size&amp;gt;&lt;br /&gt;
  &amp;lt;uploadedFileContents&amp;gt;HYC116_BORAZINE_FREQ.LOG&amp;lt;/uploadedFileContents&amp;gt;&lt;br /&gt;
&amp;lt;/jmolApplet&amp;gt;&amp;lt;/jmol&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
===Charge distribution===&lt;br /&gt;
&lt;br /&gt;
An NBO charge analysis was carried out on both the optimised benzene and borazine. Visualisations of the charge distribution are shown in the table below, with the colour range going from -1.102 to 1.102 for both molecule. This large scale was chosen as it allows direct comparison of the charge on any atoms in these two molecules and shows the relative magnitude of charges on all these atoms. Negative charges are shown in red, and positive charges are shown in green. A neutral charge is displayed in black, so the smaller a charge is (positive or negative), the darker its colour representation is. Larger charges are shown in brighter colours. The charges are also displayed on the atoms as numbers with a neutral charge being zero. Negative charges are shown as negative number and positive charges are shown as positive numbers. &lt;br /&gt;
&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot;&lt;br /&gt;
!&lt;br /&gt;
!Benzene&lt;br /&gt;
!Borazine&lt;br /&gt;
|-&lt;br /&gt;
!Visualisation of charge distribution&lt;br /&gt;
|[[File:Hyc116_benzene_charge_distribution1.png|500x500px|thumb|centre|Charge distribution of Benzene visualisation]]&lt;br /&gt;
|[[File:Hyc116_borazine_charge_distribution1.png|500x500px|thumb|centre|Charge distribution of Borazine visualisation]]&lt;br /&gt;
|-&lt;br /&gt;
!Charge &lt;br /&gt;
|Carbon: -0.239&lt;br /&gt;
&lt;br /&gt;
Hydrogen: 0.239&lt;br /&gt;
|Nitrogen: -1.102 &lt;br /&gt;
&lt;br /&gt;
Boron: 0.747&lt;br /&gt;
&lt;br /&gt;
Hydrogen (bonded to N): 0.432&lt;br /&gt;
&lt;br /&gt;
Hydrogen (bonded to B): -0.077&lt;br /&gt;
|-&lt;br /&gt;
!Discussion&lt;br /&gt;
|From the visualisation, it is shown that there is a slightly negative charge on the carbon atoms, and a positive charge of the same magnitude on the hydrogen atoms. All the carbon atoms have the same charge as they are in identical environments. The same applies to all the hydrogen atoms. This is due to the highly symmetrical structure of benzene. Since the same colour scale was used for both benzene and borazine, and the charges are much smaller in magnitude on atoms in benzene than atoms on borazine, the colours on the charge distribution visualisation is much darker. &lt;br /&gt;
|From the colours displayed on the charge distribution visualisation as well as the charge values, it is shown that nitrogen has a relatively large negative charge, while boron has a positive charge. This is due to the difference in electrogenativity between these atoms: nitrogen atoms are more electronegative than boron and tends to attract electrons towards themselves. It is worth noting that the hydrogen atoms do not all have the same charge. The hydrogen atoms bonded to boron have a slightly negative charge, and the ones bonded to nitrogen have a small positive charge. &lt;br /&gt;
&lt;br /&gt;
The fact that the same colour scale was used for both molecules comes in helpful here. It allows the charges on atoms to be compared directly. For example, just from looking at the colours, one can tell that or example, even though both carbon and nitrogen are electronegative, nitrogen is much more electronegative, which is quantitatively shown by Pauling&#039;s electronegativity scale.&amp;lt;ref&amp;gt;http://www.tutor-homework.com/Chemistry_Help/electronegativity_table/electronegativity.html (Accessed: 24.0502018&amp;lt;/ref&amp;gt;&lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
===Comparative MOs of Benzene and Borazine===&lt;br /&gt;
&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot;&lt;br /&gt;
!&lt;br /&gt;
!Benzene&lt;br /&gt;
!Borazine&lt;br /&gt;
!Comparison and Discussion&lt;br /&gt;
|-&lt;br /&gt;
!1st comparative pair&lt;br /&gt;
|[[File:Hyc116_benzene_1st_MO_pair_7.png|200x200px|centre]]&lt;br /&gt;
|[[File:Hyc116_borazine_1st_MO_pair_level9.png|200x200px|centre]]&lt;br /&gt;
|MO 9 of both benzene and borazine are comparable. They both show delocalised molecular orbital with an overall bonding character. There is a nodal plane across the molecular orbitals for both benzene and borazine. For benzene, there is contribution from all the carbon and hydrogen s orbitals. Moreover, the molecular orbitals are symmetric to their counterpart of opposite phase. That is not the case for borazine; they are less symmetric in borazine. Nitrogen atoms are more electronegative than boron atoms and pull electron density towards themselves, resulting in a larger MO. There is contribution from all the boron and nitrogen s orbitals, and three of the hydrogen s orbitals, though not all of them. &lt;br /&gt;
|-&lt;br /&gt;
!2nd comparative pair&lt;br /&gt;
|[[File:Hyc116_benzene_2nd_MO_pair_10.png|200x200px|centre]]&lt;br /&gt;
|[[File:Hyc116_borazine_2nd_MO_pair_level11.png|200x200px|centre]]&lt;br /&gt;
|&lt;br /&gt;
|-&lt;br /&gt;
!3rd comparative pair&lt;br /&gt;
|[[File:Hyc116_benzene_3rd_MO_pair_21.png|200x200px|centre]]&lt;br /&gt;
|[[File:Hyc116_borazine_3rd_MO_pair_level21.png|200x200px|centre]]&lt;br /&gt;
|&lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
===Aromaticity: some theories===&lt;br /&gt;
&lt;br /&gt;
==References==&lt;br /&gt;
{{reflist}}&lt;/div&gt;</summary>
		<author><name>Hyc116</name></author>
	</entry>
	<entry>
		<id>https://chemwiki.ch.ic.ac.uk/index.php?title=File:HYC116_NH3BH3_FREQ.LOG&amp;diff=731346</id>
		<title>File:HYC116 NH3BH3 FREQ.LOG</title>
		<link rel="alternate" type="text/html" href="https://chemwiki.ch.ic.ac.uk/index.php?title=File:HYC116_NH3BH3_FREQ.LOG&amp;diff=731346"/>
		<updated>2018-05-25T12:06:39Z</updated>

		<summary type="html">&lt;p&gt;Hyc116: Hyc116 uploaded a new version of File:HYC116 NH3BH3 FREQ.LOG&lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;&lt;/div&gt;</summary>
		<author><name>Hyc116</name></author>
	</entry>
	<entry>
		<id>https://chemwiki.ch.ic.ac.uk/index.php?title=MO_hyc116&amp;diff=731345</id>
		<title>MO hyc116</title>
		<link rel="alternate" type="text/html" href="https://chemwiki.ch.ic.ac.uk/index.php?title=MO_hyc116&amp;diff=731345"/>
		<updated>2018-05-25T12:05:27Z</updated>

		<summary type="html">&lt;p&gt;Hyc116: /* Association energy */&lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;==BH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;==&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;Calculation type&amp;lt;/b&amp;gt;: Optimisation&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;Calculation Method&amp;lt;/b&amp;gt;: B3LYP&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;Basis set&amp;lt;/b&amp;gt;: 6-31G(d,p) &lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Summary table&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
[[file:Hyc116_bh3_631g_opt_summarytable.png]]&lt;br /&gt;
&lt;br /&gt;
The above summary table was obtained after the 2nd optimisation of BH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt; (after the initial optimisation using the 3-21G basis set). Notice how the symmetry is incorrect and shown as Cs. This is because the symmetry was manually broken at the beginning by changing the bond length of B-H bonds. The point group was manually adjusted and the molecule was optimised again before the frequency analysis and the new summary table is attached below.&lt;br /&gt;
&lt;br /&gt;
[[file:Hyc116_bh3_correctsummarytable.png]]&lt;br /&gt;
&lt;br /&gt;
The above summary table was obtained from the optimisation after adjusting the symmetry. The point shown in this summary table is D&amp;lt;sub&amp;gt;3h&amp;lt;/sub&amp;gt;, which is the correct for BH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;. &lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Items table&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
Below is the items table taken from the optimisation with the correct point group.&lt;br /&gt;
&lt;br /&gt;
&amp;lt;pre&amp;gt;&lt;br /&gt;
Item               Value     Threshold  Converged?&lt;br /&gt;
 Maximum Force            0.000015     0.000450     YES&lt;br /&gt;
 RMS     Force            0.000010     0.000300     YES&lt;br /&gt;
 Maximum Displacement     0.000058     0.001800     YES&lt;br /&gt;
 RMS     Displacement     0.000038     0.001200     YES&lt;br /&gt;
&amp;lt;/pre&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Frequency log file&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
[[Media:HYC116 BH3 FREQ.LOG]] &lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Frequencies&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;pre&amp;gt;&lt;br /&gt;
Low frequencies ---  -10.3498   -3.4492   -1.2454   -0.0055    0.4779    3.2165&lt;br /&gt;
Low frequencies --- 1162.9519 1213.1527 1213.1554&lt;br /&gt;
&amp;lt;/pre&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;jmol of BH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;&#039;&#039;&#039;&lt;br /&gt;
&amp;lt;jmol&amp;gt;&amp;lt;jmolApplet&amp;gt;&lt;br /&gt;
  &amp;lt;title&amp;gt;optimised BH3&amp;lt;/title&amp;gt;&lt;br /&gt;
  &amp;lt;color&amp;gt;black&amp;lt;/color&amp;gt;&lt;br /&gt;
  &amp;lt;size&amp;gt;200&amp;lt;/size&amp;gt;&lt;br /&gt;
  &amp;lt;uploadedFileContents&amp;gt;HYC116_BH3_FREQ.LOG&amp;lt;/uploadedFileContents&amp;gt;&lt;br /&gt;
&amp;lt;/jmolApplet&amp;gt;&amp;lt;/jmol&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
===Vibrational spectrum===&lt;br /&gt;
&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot;&lt;br /&gt;
!wavenumber (cm&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;)&lt;br /&gt;
!Intensity (arbitrary units)&lt;br /&gt;
!symmetry&lt;br /&gt;
!IR active?&lt;br /&gt;
!type&lt;br /&gt;
|-&lt;br /&gt;
|1163&lt;br /&gt;
|93&lt;br /&gt;
|A&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;&#039; &#039;&lt;br /&gt;
|Yes&lt;br /&gt;
|Out of plane bend&lt;br /&gt;
|-&lt;br /&gt;
|1213&lt;br /&gt;
|14&lt;br /&gt;
|E&#039;&lt;br /&gt;
|Very slight&lt;br /&gt;
|Bend&lt;br /&gt;
|-&lt;br /&gt;
|1213&lt;br /&gt;
|14&lt;br /&gt;
|E&#039;&lt;br /&gt;
|Very slight&lt;br /&gt;
|Bend&lt;br /&gt;
|-&lt;br /&gt;
|2582&lt;br /&gt;
|0&lt;br /&gt;
|A&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;&#039;&lt;br /&gt;
|No&lt;br /&gt;
|Symmetric stretch&lt;br /&gt;
|-&lt;br /&gt;
|2716&lt;br /&gt;
|126&lt;br /&gt;
|E&#039;&lt;br /&gt;
|Yes&lt;br /&gt;
|Asymmetric stretch&lt;br /&gt;
|-&lt;br /&gt;
|2716&lt;br /&gt;
|126&lt;br /&gt;
|E&#039;&lt;br /&gt;
|Yes&lt;br /&gt;
|Asymmetric stretch&lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;IR spectrum&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
[[file:Hyc116_ir_bh3.png|400*600]]&lt;br /&gt;
&lt;br /&gt;
There are only three peaks on the IR spectrum of BH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;, despite that there are 6 vibrational modes for the molecule. As shown in the table above, the symmetric stretching mode with A1 symmetry at 2582 cm&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt; is not IR active; naturally, that vibrational mode doesn’t give a peak on the IR spectrum. As shown from the table, two pairs of vibrational modes, the bond angle deformation/bend at 1213 cm&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt; and the asymmetric bond stretch at 2716 cm&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;, are degenerate with the symmetry label E. This means that they have the same energy, and hence give the same wavenumber on the IR spectrum. Each pair of degenerate vibrational modes give rise to one peak. This leaves three peaks, as confirmed by the IR spectrum above.&lt;br /&gt;
&lt;br /&gt;
===Molecular orbitals of BH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;===&lt;br /&gt;
&lt;br /&gt;
[[file:hyc116_bh3_MO_diagram.png]]&lt;br /&gt;
&lt;br /&gt;
The above molecular orbital diagram was taken from Dr Patricia Hunt&#039;s &amp;lt;i&amp;gt;Lecture 4 Tutorial Problem Model Answers&amp;lt;/i&amp;gt;.&amp;lt;ref&amp;gt;P. Hunt, &amp;quot;Lecture 4 Tutorial Problem Model Answers&amp;quot;, 2 (2018)&amp;lt;/ref&amp;gt; Diagrams of the &amp;quot;real&amp;quot; MOs were obtained from Gaussian.&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
There is no significant difference between the LCAO MOs and the real ones. Features such as orbital phases are shown clearly on both the LCAO MOs and the real MOs, illustrating the bonding/anti-bonding characters of the molecular orbitals. This suggests that the the qualitative MO theory is highly accurate and useful when studying the molecular orbitals of molecules.&lt;br /&gt;
&lt;br /&gt;
==Associated energies: ammonium borane==&lt;br /&gt;
&lt;br /&gt;
===NH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;===&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;Calculation type&amp;lt;/b&amp;gt;: Optimisation&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;Calculation Method&amp;lt;/b&amp;gt;: B3LYP&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;Basis set&amp;lt;/b&amp;gt;: 6-31G(d,p) &lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Summary table&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
[[file:Hyc116_nh3_631g_summarytable.png]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Items table&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;pre&amp;gt;&lt;br /&gt;
Item               Value     Threshold  Converged?&lt;br /&gt;
 Maximum Force            0.000006     0.000450     YES&lt;br /&gt;
 RMS     Force            0.000004     0.000300     YES&lt;br /&gt;
 Maximum Displacement     0.000012     0.001800     YES&lt;br /&gt;
 RMS     Displacement     0.000008     0.001200     YES&lt;br /&gt;
&amp;lt;/pre&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Frequency log file&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
[[Media:HYC116_NH3_FREQ.LOG]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Frequencies&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;pre&amp;gt;&lt;br /&gt;
Low frequencies ---   -8.5646   -8.5588   -0.0047    0.0454    0.1784   26.4183&lt;br /&gt;
Low frequencies --- 1089.7603 1694.1865 1694.1865&lt;br /&gt;
&amp;lt;/pre&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;jmol of NH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;&#039;&#039;&#039;&lt;br /&gt;
&amp;lt;jmol&amp;gt;&amp;lt;jmolApplet&amp;gt;&lt;br /&gt;
  &amp;lt;title&amp;gt;optimised NH3&amp;lt;/title&amp;gt;&lt;br /&gt;
  &amp;lt;color&amp;gt;black&amp;lt;/color&amp;gt;&lt;br /&gt;
  &amp;lt;size&amp;gt;200&amp;lt;/size&amp;gt;&lt;br /&gt;
  &amp;lt;uploadedFileContents&amp;gt;HYC116_NH3_FREQ.LOG&amp;lt;/uploadedFileContents&amp;gt;&lt;br /&gt;
&amp;lt;/jmolApplet&amp;gt;&amp;lt;/jmol&amp;gt;&lt;br /&gt;
&lt;br /&gt;
===NH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;BH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;===&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;Calculation type&amp;lt;/b&amp;gt;: Optimisation&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;Calculation Method&amp;lt;/b&amp;gt;: B3LYP&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;Basis set&amp;lt;/b&amp;gt;: 6-31G(d,p) &lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Summary table&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
[[file:Hyc116_nh3bh3_631g_summarytable1.png]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Items table&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;pre&amp;gt;&lt;br /&gt;
Item               Value     Threshold  Converged?&lt;br /&gt;
 Maximum Force            0.000121     0.000450     YES&lt;br /&gt;
 RMS     Force            0.000057     0.000300     YES&lt;br /&gt;
 Maximum Displacement     0.000501     0.001800     YES&lt;br /&gt;
 RMS     Displacement     0.000293     0.001200     YES&lt;br /&gt;
&amp;lt;/pre&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Frequency log file&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
[[Media:HYC116_NH3BH3_FREQ.LOG]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Frequencies&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;pre&amp;gt;&lt;br /&gt;
Low frequencies ---   -0.0014   -0.0011   -0.0006    6.9624   20.4518   43.5542&lt;br /&gt;
Low frequencies ---  266.4530  632.2458  639.0504&lt;br /&gt;
&amp;lt;/pre&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;jmol of NH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;BH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;&#039;&#039;&#039;&lt;br /&gt;
&amp;lt;jmol&amp;gt;&amp;lt;jmolApplet&amp;gt;&lt;br /&gt;
  &amp;lt;title&amp;gt;optimised NH3BH3&amp;lt;/title&amp;gt;&lt;br /&gt;
  &amp;lt;color&amp;gt;black&amp;lt;/color&amp;gt;&lt;br /&gt;
  &amp;lt;size&amp;gt;200&amp;lt;/size&amp;gt;&lt;br /&gt;
  &amp;lt;uploadedFileContents&amp;gt;HYC116_NH3BH3_FREQ.LOG&amp;lt;/uploadedFileContents&amp;gt;&lt;br /&gt;
&amp;lt;/jmolApplet&amp;gt;&amp;lt;/jmol&amp;gt;&lt;br /&gt;
&lt;br /&gt;
===Association energy===&lt;br /&gt;
&lt;br /&gt;
E(BH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;) (using the optimisation with the correct symmetry) = -26.61532363 a.u. = &amp;lt;b&amp;gt;-26.61532 a.u. (5 d.p.)&amp;lt;/b&amp;gt;&lt;br /&gt;
&lt;br /&gt;
E(NH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;) = -56.55776873 a.u. = &amp;lt;b&amp;gt;-56.55777 a.u. (5 d.p.)&amp;lt;/b&amp;gt;&lt;br /&gt;
&lt;br /&gt;
E(NH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;BH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;) = -83.22468892 a.u. = &amp;lt;b&amp;gt;-83.22469 a.u. (5 d.p.)&amp;lt;/b&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
Carrying out calculations using numbers which has already been rounded up can possibly result in errors in the last digit. Hence, here the calculations were carried out using the numbers provided from the optimisations (i.e. with more decimal places than necessary); the answer was then rounded up to the desired accuracy. &lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
ΔE = E(NH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;BH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;)-[E(NH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;)+E(BH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;)]&lt;br /&gt;
&lt;br /&gt;
ΔE = -83.22468892 - (-56.55776873 + -26.61532363) = -0.05159656 a.u. &lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;ΔE = -0.05160 a.u. (5 d.p.)&amp;lt;/b&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Converting energy from a.u. to kJ/mol&#039;&#039;&#039;&lt;br /&gt;
An atomic unit for energy is Hartree, which is equal to 2625.5 kJ/mol.&lt;br /&gt;
&amp;lt;ref&amp;gt;https://cccbdb.nist.gov/hartree.asp (Accessed: 22.05.2018)&amp;lt;/ref&amp;gt;&lt;br /&gt;
 &lt;br /&gt;
&lt;br /&gt;
So ΔE in kJ/mol = -0.05159657 * 2625.5 = -135.46676828 kJ/mol&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;ΔE = -135 kJ/mol (nearest integer)&amp;lt;/b&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
The energy difference calculated above comes from the formation of the B-N dative bond. It is a relatively weak bond. According to a bond energy data sheet provided by the University of California,&amp;lt;ref&amp;gt;https://labs.chem.ucsb.edu/zakarian/armen/11---bonddissociationenergy.pdf (Accessed: 24.05.2018)&amp;lt;/ref&amp;gt;  the bond energy of the C-C bond of an ethane molecule is 368 kJ/mol. This is a fair comparison to the NH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;BH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt; molecule as the two molecules have the same structure, only with the carbon atoms on ethane swapped for Boron and Nitrogen in NH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;BH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;&lt;br /&gt;
&lt;br /&gt;
==Using a mixture of basis-sets and pseudo-potentials==&lt;br /&gt;
&lt;br /&gt;
===BBr&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;===&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;Calculation type&amp;lt;/b&amp;gt;: Optimisation&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;Calculation Method&amp;lt;/b&amp;gt;: B3LYP&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;Basis set&amp;lt;/b&amp;gt;: Boron: 6-31G(d,p) ; Br: LANL2DZ&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
Larger calculations are often sent to a web-server to run on a high-performance computer instead of a desktop. In order to experience and learn to use a web-server, the optimisation and the frequency analysis for BBr&amp;lt;sub&amp;gt;3&amp;lt;/sub were both sent and done on a server instead of the desktop. The calculation results were downloaded from the web-server once they were finished.   &lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Summary table&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
[[file:Hyc116_bbr3_opt_summarytable.png]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Items table&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;pre&amp;gt;&lt;br /&gt;
Item               Value     Threshold  Converged?&lt;br /&gt;
 Maximum Force            0.000008     0.000450     YES&lt;br /&gt;
 RMS     Force            0.000005     0.000300     YES&lt;br /&gt;
 Maximum Displacement     0.000036     0.001800     YES&lt;br /&gt;
 RMS     Displacement     0.000023     0.001200     YES&lt;br /&gt;
&amp;lt;/pre&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Frequency log file&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
[[Media:Hyc116_bbr3_freq.log]]&lt;br /&gt;
&lt;br /&gt;
Attached above is the frequency file saved onto the computer from the SCAN server portal. The frequency file was also published on the chemistry database DSpace. {{DOI|10042/202442}}&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Frequencies&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;pre&amp;gt;&lt;br /&gt;
Low frequencies ---   -0.0137   -0.0064   -0.0046    2.4315    2.4315    4.8421&lt;br /&gt;
Low frequencies ---  155.9631  155.9651  267.7052&lt;br /&gt;
&amp;lt;/pre&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;jmol of BBr&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;&#039;&#039;&#039;&lt;br /&gt;
&amp;lt;jmol&amp;gt;&amp;lt;jmolApplet&amp;gt;&lt;br /&gt;
  &amp;lt;title&amp;gt;optimised BBr3&amp;lt;/title&amp;gt;&lt;br /&gt;
  &amp;lt;color&amp;gt;black&amp;lt;/color&amp;gt;&lt;br /&gt;
  &amp;lt;size&amp;gt;200&amp;lt;/size&amp;gt;&lt;br /&gt;
  &amp;lt;uploadedFileContents&amp;gt;Hyc116_bbr3_freq.log&amp;lt;/uploadedFileContents&amp;gt;&lt;br /&gt;
&amp;lt;/jmolApplet&amp;gt;&amp;lt;/jmol&amp;gt;&lt;br /&gt;
&lt;br /&gt;
==Aromaticity==&lt;br /&gt;
&lt;br /&gt;
===Benzene===&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;Calculation type&amp;lt;/b&amp;gt;: Optimisation&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;Calculation Method&amp;lt;/b&amp;gt;: B3LYP&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;Basis set&amp;lt;/b&amp;gt;: 6-31G(d,p) &lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Summary table&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
[[file:Hyc116_c6h6_summarytable.png]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Items table&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;pre&amp;gt;&lt;br /&gt;
Item               Value     Threshold  Converged?&lt;br /&gt;
 Maximum Force            0.000193     0.000450     YES&lt;br /&gt;
 RMS     Force            0.000079     0.000300     YES&lt;br /&gt;
 Maximum Displacement     0.000830     0.001800     YES&lt;br /&gt;
 RMS     Displacement     0.000294     0.001200     YES&lt;br /&gt;
&amp;lt;/pre&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Frequency log file&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
[[Media:HYC116_C6H6_FREQ.LOG]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Frequencies&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;pre&amp;gt;&lt;br /&gt;
Low frequencies ---   -3.5606   -3.5606   -0.0089   -0.0043   -0.0043   10.0905&lt;br /&gt;
Low frequencies ---  413.9582  413.9582  621.1416&lt;br /&gt;
&amp;lt;/pre&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;jmol of C&amp;lt;sub&amp;gt;6&amp;lt;/sub&amp;gt;H&amp;lt;sub&amp;gt;6&amp;lt;/sub&amp;gt;&#039;&#039;&#039;&lt;br /&gt;
&amp;lt;jmol&amp;gt;&amp;lt;jmolApplet&amp;gt;&lt;br /&gt;
  &amp;lt;title&amp;gt;optimised Benzene&amp;lt;/title&amp;gt;&lt;br /&gt;
  &amp;lt;color&amp;gt;black&amp;lt;/color&amp;gt;&lt;br /&gt;
  &amp;lt;size&amp;gt;200&amp;lt;/size&amp;gt;&lt;br /&gt;
  &amp;lt;uploadedFileContents&amp;gt;HYC116_C6H6_FREQ.LOG&amp;lt;/uploadedFileContents&amp;gt;&lt;br /&gt;
&amp;lt;/jmolApplet&amp;gt;&amp;lt;/jmol&amp;gt;&lt;br /&gt;
&lt;br /&gt;
===Borazine===&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;Calculation type&amp;lt;/b&amp;gt;: Optimisation&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;Calculation Method&amp;lt;/b&amp;gt;: B3LYP&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;Basis set&amp;lt;/b&amp;gt;: 6-31G(d,p) &lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Summary table&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
[[file:Hyc116_borazine_summarytable.png]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Items table&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;pre&amp;gt;&lt;br /&gt;
Item               Value     Threshold  Converged?&lt;br /&gt;
 Maximum Force            0.000085     0.000450     YES&lt;br /&gt;
 RMS     Force            0.000033     0.000300     YES&lt;br /&gt;
 Maximum Displacement     0.000250     0.001800     YES&lt;br /&gt;
 RMS     Displacement     0.000074     0.001200     YES&lt;br /&gt;
&amp;lt;/pre&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Frequency log file&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
[[Media:HYC116_BORAZINE_FREQ.LOG]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Frequencies&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;pre&amp;gt;&lt;br /&gt;
Low frequencies ---  -12.6626  -12.6626   -8.9272   -0.0211   -0.0104   -0.0104&lt;br /&gt;
Low frequencies ---  289.1112  289.1112  403.8613&lt;br /&gt;
&amp;lt;/pre&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;jmol of Borazine&#039;&#039;&#039;&lt;br /&gt;
&amp;lt;jmol&amp;gt;&amp;lt;jmolApplet&amp;gt;&lt;br /&gt;
  &amp;lt;title&amp;gt;optimised Borazine&amp;lt;/title&amp;gt;&lt;br /&gt;
  &amp;lt;color&amp;gt;black&amp;lt;/color&amp;gt;&lt;br /&gt;
  &amp;lt;size&amp;gt;200&amp;lt;/size&amp;gt;&lt;br /&gt;
  &amp;lt;uploadedFileContents&amp;gt;HYC116_BORAZINE_FREQ.LOG&amp;lt;/uploadedFileContents&amp;gt;&lt;br /&gt;
&amp;lt;/jmolApplet&amp;gt;&amp;lt;/jmol&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
===Charge distribution===&lt;br /&gt;
&lt;br /&gt;
An NBO charge analysis was carried out on both the optimised benzene and borazine. Visualisations of the charge distribution are shown in the table below, with the colour range going from -1.102 to 1.102 for both molecule. This large scale was chosen as it allows direct comparison of the charge on any atoms in these two molecules and shows the relative magnitude of charges on all these atoms. Negative charges are shown in red, and positive charges are shown in green. A neutral charge is displayed in black, so the smaller a charge is (positive or negative), the darker its colour representation is. Larger charges are shown in brighter colours. The charges are also displayed on the atoms as numbers with a neutral charge being zero. Negative charges are shown as negative number and positive charges are shown as positive numbers. &lt;br /&gt;
&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot;&lt;br /&gt;
!&lt;br /&gt;
!Benzene&lt;br /&gt;
!Borazine&lt;br /&gt;
|-&lt;br /&gt;
!Visualisation of charge distribution&lt;br /&gt;
|[[File:Hyc116_benzene_charge_distribution1.png|500x500px|thumb|centre|Charge distribution of Benzene visualisation]]&lt;br /&gt;
|[[File:Hyc116_borazine_charge_distribution1.png|500x500px|thumb|centre|Charge distribution of Borazine visualisation]]&lt;br /&gt;
|-&lt;br /&gt;
!Charge &lt;br /&gt;
|Carbon: -0.239&lt;br /&gt;
&lt;br /&gt;
Hydrogen: 0.239&lt;br /&gt;
|Nitrogen: -1.102 &lt;br /&gt;
&lt;br /&gt;
Boron: 0.747&lt;br /&gt;
&lt;br /&gt;
Hydrogen (bonded to N): 0.432&lt;br /&gt;
&lt;br /&gt;
Hydrogen (bonded to B): -0.077&lt;br /&gt;
|-&lt;br /&gt;
!Discussion&lt;br /&gt;
|From the visualisation, it is shown that there is a slightly negative charge on the carbon atoms, and a positive charge of the same magnitude on the hydrogen atoms. All the carbon atoms have the same charge as they are in identical environments. The same applies to all the hydrogen atoms. This is due to the highly symmetrical structure of benzene. Since the same colour scale was used for both benzene and borazine, and the charges are much smaller in magnitude on atoms in benzene than atoms on borazine, the colours on the charge distribution visualisation is much darker. &lt;br /&gt;
|From the colours displayed on the charge distribution visualisation as well as the charge values, it is shown that nitrogen has a relatively large negative charge, while boron has a positive charge. This is due to the difference in electrogenativity between these atoms: nitrogen atoms are more electronegative than boron and tends to attract electrons towards themselves. It is worth noting that the hydrogen atoms do not all have the same charge. The hydrogen atoms bonded to boron have a slightly negative charge, and the ones bonded to nitrogen have a small positive charge. &lt;br /&gt;
&lt;br /&gt;
The fact that the same colour scale was used for both molecules comes in helpful here. It allows the charges on atoms to be compared directly. For example, just from looking at the colours, one can tell that or example, even though both carbon and nitrogen are electronegative, nitrogen is much more electronegative, which is quantitatively shown by Pauling&#039;s electronegativity scale.&amp;lt;ref&amp;gt;http://www.tutor-homework.com/Chemistry_Help/electronegativity_table/electronegativity.html (Accessed: 24.0502018&amp;lt;/ref&amp;gt;&lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
===Comparative MOs of Benzene and Borazine===&lt;br /&gt;
&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot;&lt;br /&gt;
!&lt;br /&gt;
!Benzene&lt;br /&gt;
!Borazine&lt;br /&gt;
!Comparison and Discussion&lt;br /&gt;
|-&lt;br /&gt;
!1st comparative pair&lt;br /&gt;
|[[File:Hyc116_benzene_1st_MO_pair_7.png|200x200px|centre]]&lt;br /&gt;
|[[File:Hyc116_borazine_1st_MO_pair_level9.png|200x200px|centre]]&lt;br /&gt;
|MO 9 of both benzene and borazine are comparable. They both show delocalised molecular orbital with an overall bonding character. There is a nodal plane across the molecular orbitals for both benzene and borazine. For benzene, there is contribution from all the carbon and hydrogen s orbitals. Moreover, the molecular orbitals are symmetric to their counterpart of opposite phase. That is not the case for borazine; they are less symmetric in borazine. Nitrogen atoms are more electronegative than boron atoms and pull electron density towards themselves, resulting in a larger MO. There is contribution from all the boron and nitrogen s orbitals, and three of the hydrogen s orbitals, though not all of them. &lt;br /&gt;
|-&lt;br /&gt;
!2nd comparative pair&lt;br /&gt;
|[[File:Hyc116_benzene_2nd_MO_pair_10.png|200x200px|centre]]&lt;br /&gt;
|[[File:Hyc116_borazine_2nd_MO_pair_level11.png|200x200px|centre]]&lt;br /&gt;
|&lt;br /&gt;
|-&lt;br /&gt;
!3rd comparative pair&lt;br /&gt;
|[[File:Hyc116_benzene_3rd_MO_pair_21.png|200x200px|centre]]&lt;br /&gt;
|[[File:Hyc116_borazine_3rd_MO_pair_level21.png|200x200px|centre]]&lt;br /&gt;
|&lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
===Aromaticity: some theories===&lt;br /&gt;
&lt;br /&gt;
==References==&lt;br /&gt;
{{reflist}}&lt;/div&gt;</summary>
		<author><name>Hyc116</name></author>
	</entry>
	<entry>
		<id>https://chemwiki.ch.ic.ac.uk/index.php?title=MO_hyc116&amp;diff=731338</id>
		<title>MO hyc116</title>
		<link rel="alternate" type="text/html" href="https://chemwiki.ch.ic.ac.uk/index.php?title=MO_hyc116&amp;diff=731338"/>
		<updated>2018-05-25T12:02:26Z</updated>

		<summary type="html">&lt;p&gt;Hyc116: /* NH3BH3 */&lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;==BH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;==&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;Calculation type&amp;lt;/b&amp;gt;: Optimisation&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;Calculation Method&amp;lt;/b&amp;gt;: B3LYP&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;Basis set&amp;lt;/b&amp;gt;: 6-31G(d,p) &lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Summary table&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
[[file:Hyc116_bh3_631g_opt_summarytable.png]]&lt;br /&gt;
&lt;br /&gt;
The above summary table was obtained after the 2nd optimisation of BH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt; (after the initial optimisation using the 3-21G basis set). Notice how the symmetry is incorrect and shown as Cs. This is because the symmetry was manually broken at the beginning by changing the bond length of B-H bonds. The point group was manually adjusted and the molecule was optimised again before the frequency analysis and the new summary table is attached below.&lt;br /&gt;
&lt;br /&gt;
[[file:Hyc116_bh3_correctsummarytable.png]]&lt;br /&gt;
&lt;br /&gt;
The above summary table was obtained from the optimisation after adjusting the symmetry. The point shown in this summary table is D&amp;lt;sub&amp;gt;3h&amp;lt;/sub&amp;gt;, which is the correct for BH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;. &lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Items table&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
Below is the items table taken from the optimisation with the correct point group.&lt;br /&gt;
&lt;br /&gt;
&amp;lt;pre&amp;gt;&lt;br /&gt;
Item               Value     Threshold  Converged?&lt;br /&gt;
 Maximum Force            0.000015     0.000450     YES&lt;br /&gt;
 RMS     Force            0.000010     0.000300     YES&lt;br /&gt;
 Maximum Displacement     0.000058     0.001800     YES&lt;br /&gt;
 RMS     Displacement     0.000038     0.001200     YES&lt;br /&gt;
&amp;lt;/pre&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Frequency log file&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
[[Media:HYC116 BH3 FREQ.LOG]] &lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Frequencies&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;pre&amp;gt;&lt;br /&gt;
Low frequencies ---  -10.3498   -3.4492   -1.2454   -0.0055    0.4779    3.2165&lt;br /&gt;
Low frequencies --- 1162.9519 1213.1527 1213.1554&lt;br /&gt;
&amp;lt;/pre&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;jmol of BH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;&#039;&#039;&#039;&lt;br /&gt;
&amp;lt;jmol&amp;gt;&amp;lt;jmolApplet&amp;gt;&lt;br /&gt;
  &amp;lt;title&amp;gt;optimised BH3&amp;lt;/title&amp;gt;&lt;br /&gt;
  &amp;lt;color&amp;gt;black&amp;lt;/color&amp;gt;&lt;br /&gt;
  &amp;lt;size&amp;gt;200&amp;lt;/size&amp;gt;&lt;br /&gt;
  &amp;lt;uploadedFileContents&amp;gt;HYC116_BH3_FREQ.LOG&amp;lt;/uploadedFileContents&amp;gt;&lt;br /&gt;
&amp;lt;/jmolApplet&amp;gt;&amp;lt;/jmol&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
===Vibrational spectrum===&lt;br /&gt;
&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot;&lt;br /&gt;
!wavenumber (cm&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;)&lt;br /&gt;
!Intensity (arbitrary units)&lt;br /&gt;
!symmetry&lt;br /&gt;
!IR active?&lt;br /&gt;
!type&lt;br /&gt;
|-&lt;br /&gt;
|1163&lt;br /&gt;
|93&lt;br /&gt;
|A&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;&#039; &#039;&lt;br /&gt;
|Yes&lt;br /&gt;
|Out of plane bend&lt;br /&gt;
|-&lt;br /&gt;
|1213&lt;br /&gt;
|14&lt;br /&gt;
|E&#039;&lt;br /&gt;
|Very slight&lt;br /&gt;
|Bend&lt;br /&gt;
|-&lt;br /&gt;
|1213&lt;br /&gt;
|14&lt;br /&gt;
|E&#039;&lt;br /&gt;
|Very slight&lt;br /&gt;
|Bend&lt;br /&gt;
|-&lt;br /&gt;
|2582&lt;br /&gt;
|0&lt;br /&gt;
|A&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;&#039;&lt;br /&gt;
|No&lt;br /&gt;
|Symmetric stretch&lt;br /&gt;
|-&lt;br /&gt;
|2716&lt;br /&gt;
|126&lt;br /&gt;
|E&#039;&lt;br /&gt;
|Yes&lt;br /&gt;
|Asymmetric stretch&lt;br /&gt;
|-&lt;br /&gt;
|2716&lt;br /&gt;
|126&lt;br /&gt;
|E&#039;&lt;br /&gt;
|Yes&lt;br /&gt;
|Asymmetric stretch&lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;IR spectrum&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
[[file:Hyc116_ir_bh3.png|400*600]]&lt;br /&gt;
&lt;br /&gt;
There are only three peaks on the IR spectrum of BH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;, despite that there are 6 vibrational modes for the molecule. As shown in the table above, the symmetric stretching mode with A1 symmetry at 2582 cm&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt; is not IR active; naturally, that vibrational mode doesn’t give a peak on the IR spectrum. As shown from the table, two pairs of vibrational modes, the bond angle deformation/bend at 1213 cm&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt; and the asymmetric bond stretch at 2716 cm&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;, are degenerate with the symmetry label E. This means that they have the same energy, and hence give the same wavenumber on the IR spectrum. Each pair of degenerate vibrational modes give rise to one peak. This leaves three peaks, as confirmed by the IR spectrum above.&lt;br /&gt;
&lt;br /&gt;
===Molecular orbitals of BH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;===&lt;br /&gt;
&lt;br /&gt;
[[file:hyc116_bh3_MO_diagram.png]]&lt;br /&gt;
&lt;br /&gt;
The above molecular orbital diagram was taken from Dr Patricia Hunt&#039;s &amp;lt;i&amp;gt;Lecture 4 Tutorial Problem Model Answers&amp;lt;/i&amp;gt;.&amp;lt;ref&amp;gt;P. Hunt, &amp;quot;Lecture 4 Tutorial Problem Model Answers&amp;quot;, 2 (2018)&amp;lt;/ref&amp;gt; Diagrams of the &amp;quot;real&amp;quot; MOs were obtained from Gaussian.&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
There is no significant difference between the LCAO MOs and the real ones. Features such as orbital phases are shown clearly on both the LCAO MOs and the real MOs, illustrating the bonding/anti-bonding characters of the molecular orbitals. This suggests that the the qualitative MO theory is highly accurate and useful when studying the molecular orbitals of molecules.&lt;br /&gt;
&lt;br /&gt;
==Associated energies: ammonium borane==&lt;br /&gt;
&lt;br /&gt;
===NH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;===&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;Calculation type&amp;lt;/b&amp;gt;: Optimisation&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;Calculation Method&amp;lt;/b&amp;gt;: B3LYP&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;Basis set&amp;lt;/b&amp;gt;: 6-31G(d,p) &lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Summary table&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
[[file:Hyc116_nh3_631g_summarytable.png]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Items table&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;pre&amp;gt;&lt;br /&gt;
Item               Value     Threshold  Converged?&lt;br /&gt;
 Maximum Force            0.000006     0.000450     YES&lt;br /&gt;
 RMS     Force            0.000004     0.000300     YES&lt;br /&gt;
 Maximum Displacement     0.000012     0.001800     YES&lt;br /&gt;
 RMS     Displacement     0.000008     0.001200     YES&lt;br /&gt;
&amp;lt;/pre&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Frequency log file&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
[[Media:HYC116_NH3_FREQ.LOG]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Frequencies&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;pre&amp;gt;&lt;br /&gt;
Low frequencies ---   -8.5646   -8.5588   -0.0047    0.0454    0.1784   26.4183&lt;br /&gt;
Low frequencies --- 1089.7603 1694.1865 1694.1865&lt;br /&gt;
&amp;lt;/pre&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;jmol of NH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;&#039;&#039;&#039;&lt;br /&gt;
&amp;lt;jmol&amp;gt;&amp;lt;jmolApplet&amp;gt;&lt;br /&gt;
  &amp;lt;title&amp;gt;optimised NH3&amp;lt;/title&amp;gt;&lt;br /&gt;
  &amp;lt;color&amp;gt;black&amp;lt;/color&amp;gt;&lt;br /&gt;
  &amp;lt;size&amp;gt;200&amp;lt;/size&amp;gt;&lt;br /&gt;
  &amp;lt;uploadedFileContents&amp;gt;HYC116_NH3_FREQ.LOG&amp;lt;/uploadedFileContents&amp;gt;&lt;br /&gt;
&amp;lt;/jmolApplet&amp;gt;&amp;lt;/jmol&amp;gt;&lt;br /&gt;
&lt;br /&gt;
===NH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;BH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;===&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;Calculation type&amp;lt;/b&amp;gt;: Optimisation&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;Calculation Method&amp;lt;/b&amp;gt;: B3LYP&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;Basis set&amp;lt;/b&amp;gt;: 6-31G(d,p) &lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Summary table&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
[[file:Hyc116_nh3bh3_631g_summarytable1.png]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Items table&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;pre&amp;gt;&lt;br /&gt;
Item               Value     Threshold  Converged?&lt;br /&gt;
 Maximum Force            0.000121     0.000450     YES&lt;br /&gt;
 RMS     Force            0.000057     0.000300     YES&lt;br /&gt;
 Maximum Displacement     0.000501     0.001800     YES&lt;br /&gt;
 RMS     Displacement     0.000293     0.001200     YES&lt;br /&gt;
&amp;lt;/pre&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Frequency log file&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
[[Media:HYC116_NH3BH3_FREQ.LOG]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Frequencies&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;pre&amp;gt;&lt;br /&gt;
Low frequencies ---   -0.0014   -0.0011   -0.0006    6.9624   20.4518   43.5542&lt;br /&gt;
Low frequencies ---  266.4530  632.2458  639.0504&lt;br /&gt;
&amp;lt;/pre&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;jmol of NH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;BH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;&#039;&#039;&#039;&lt;br /&gt;
&amp;lt;jmol&amp;gt;&amp;lt;jmolApplet&amp;gt;&lt;br /&gt;
  &amp;lt;title&amp;gt;optimised NH3BH3&amp;lt;/title&amp;gt;&lt;br /&gt;
  &amp;lt;color&amp;gt;black&amp;lt;/color&amp;gt;&lt;br /&gt;
  &amp;lt;size&amp;gt;200&amp;lt;/size&amp;gt;&lt;br /&gt;
  &amp;lt;uploadedFileContents&amp;gt;HYC116_NH3BH3_FREQ.LOG&amp;lt;/uploadedFileContents&amp;gt;&lt;br /&gt;
&amp;lt;/jmolApplet&amp;gt;&amp;lt;/jmol&amp;gt;&lt;br /&gt;
&lt;br /&gt;
===Association energy===&lt;br /&gt;
&lt;br /&gt;
E(BH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;) (using the optimisation with the correct symmetry) = -26.61532363 a.u. = &amp;lt;b&amp;gt;-26.61532 a.u. (5 d.p.)&amp;lt;/b&amp;gt;&lt;br /&gt;
&lt;br /&gt;
E(NH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;) = -56.55776873 a.u. = &amp;lt;b&amp;gt;-56.55777 a.u. (5 d.p.)&amp;lt;/b&amp;gt;&lt;br /&gt;
&lt;br /&gt;
E(NH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;BH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;) = -83.22468893 a.u. = &amp;lt;b&amp;gt;-83.22469 a.u. (5 d.p.)&amp;lt;/b&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
Carrying out calculations using numbers which has already been rounded up can possibly result in errors in the last digit. Hence, here the calculations were carried out using the numbers provided from the optimisations (i.e. with more decimal places than necessary); the answer was then rounded up to the desired accuracy. &lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
ΔE = E(NH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;BH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;)-[E(NH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;)+E(BH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;)]&lt;br /&gt;
&lt;br /&gt;
ΔE = -83.22468893 - (-56.55776873 + -26.61532363) = -0.05159657 a.u. &lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;ΔE = -0.05160 a.u. (5 d.p.)&amp;lt;/b&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Converting energy from a.u. to kJ/mol&#039;&#039;&#039;&lt;br /&gt;
An atomic unit for energy is Hartree, which is equal to 2625.5 kJ/mol.&lt;br /&gt;
&amp;lt;ref&amp;gt;https://cccbdb.nist.gov/hartree.asp (Accessed: 22.05.2018)&amp;lt;/ref&amp;gt;&lt;br /&gt;
 &lt;br /&gt;
&lt;br /&gt;
So ΔE in kJ/mol = -0.05159657 * 2625.5 = -135.466794535 kJ/mol&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;ΔE = -135 kJ/mol (nearest integer)&amp;lt;/b&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
The energy difference calculated above comes from the formation of the B-N dative bond. It is a relatively weak bond. According to a bond energy data sheet provided by the University of California,&amp;lt;ref&amp;gt;https://labs.chem.ucsb.edu/zakarian/armen/11---bonddissociationenergy.pdf (Accessed: 24.05.2018)&amp;lt;/ref&amp;gt;  the bond energy of the C-C bond of an ethane molecule is 368 kJ/mol. This is a fair comparison to the NH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;BH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt; molecule as the two molecules have the same structure, only with the carbon atoms on ethane swapped for Boron and Nitrogen in NH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;BH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;&lt;br /&gt;
&lt;br /&gt;
==Using a mixture of basis-sets and pseudo-potentials==&lt;br /&gt;
&lt;br /&gt;
===BBr&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;===&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;Calculation type&amp;lt;/b&amp;gt;: Optimisation&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;Calculation Method&amp;lt;/b&amp;gt;: B3LYP&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;Basis set&amp;lt;/b&amp;gt;: Boron: 6-31G(d,p) ; Br: LANL2DZ&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
Larger calculations are often sent to a web-server to run on a high-performance computer instead of a desktop. In order to experience and learn to use a web-server, the optimisation and the frequency analysis for BBr&amp;lt;sub&amp;gt;3&amp;lt;/sub were both sent and done on a server instead of the desktop. The calculation results were downloaded from the web-server once they were finished.   &lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Summary table&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
[[file:Hyc116_bbr3_opt_summarytable.png]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Items table&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;pre&amp;gt;&lt;br /&gt;
Item               Value     Threshold  Converged?&lt;br /&gt;
 Maximum Force            0.000008     0.000450     YES&lt;br /&gt;
 RMS     Force            0.000005     0.000300     YES&lt;br /&gt;
 Maximum Displacement     0.000036     0.001800     YES&lt;br /&gt;
 RMS     Displacement     0.000023     0.001200     YES&lt;br /&gt;
&amp;lt;/pre&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Frequency log file&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
[[Media:Hyc116_bbr3_freq.log]]&lt;br /&gt;
&lt;br /&gt;
Attached above is the frequency file saved onto the computer from the SCAN server portal. The frequency file was also published on the chemistry database DSpace. {{DOI|10042/202442}}&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Frequencies&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;pre&amp;gt;&lt;br /&gt;
Low frequencies ---   -0.0137   -0.0064   -0.0046    2.4315    2.4315    4.8421&lt;br /&gt;
Low frequencies ---  155.9631  155.9651  267.7052&lt;br /&gt;
&amp;lt;/pre&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;jmol of BBr&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;&#039;&#039;&#039;&lt;br /&gt;
&amp;lt;jmol&amp;gt;&amp;lt;jmolApplet&amp;gt;&lt;br /&gt;
  &amp;lt;title&amp;gt;optimised BBr3&amp;lt;/title&amp;gt;&lt;br /&gt;
  &amp;lt;color&amp;gt;black&amp;lt;/color&amp;gt;&lt;br /&gt;
  &amp;lt;size&amp;gt;200&amp;lt;/size&amp;gt;&lt;br /&gt;
  &amp;lt;uploadedFileContents&amp;gt;Hyc116_bbr3_freq.log&amp;lt;/uploadedFileContents&amp;gt;&lt;br /&gt;
&amp;lt;/jmolApplet&amp;gt;&amp;lt;/jmol&amp;gt;&lt;br /&gt;
&lt;br /&gt;
==Aromaticity==&lt;br /&gt;
&lt;br /&gt;
===Benzene===&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;Calculation type&amp;lt;/b&amp;gt;: Optimisation&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;Calculation Method&amp;lt;/b&amp;gt;: B3LYP&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;Basis set&amp;lt;/b&amp;gt;: 6-31G(d,p) &lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Summary table&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
[[file:Hyc116_c6h6_summarytable.png]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Items table&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;pre&amp;gt;&lt;br /&gt;
Item               Value     Threshold  Converged?&lt;br /&gt;
 Maximum Force            0.000193     0.000450     YES&lt;br /&gt;
 RMS     Force            0.000079     0.000300     YES&lt;br /&gt;
 Maximum Displacement     0.000830     0.001800     YES&lt;br /&gt;
 RMS     Displacement     0.000294     0.001200     YES&lt;br /&gt;
&amp;lt;/pre&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Frequency log file&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
[[Media:HYC116_C6H6_FREQ.LOG]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Frequencies&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;pre&amp;gt;&lt;br /&gt;
Low frequencies ---   -3.5606   -3.5606   -0.0089   -0.0043   -0.0043   10.0905&lt;br /&gt;
Low frequencies ---  413.9582  413.9582  621.1416&lt;br /&gt;
&amp;lt;/pre&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;jmol of C&amp;lt;sub&amp;gt;6&amp;lt;/sub&amp;gt;H&amp;lt;sub&amp;gt;6&amp;lt;/sub&amp;gt;&#039;&#039;&#039;&lt;br /&gt;
&amp;lt;jmol&amp;gt;&amp;lt;jmolApplet&amp;gt;&lt;br /&gt;
  &amp;lt;title&amp;gt;optimised Benzene&amp;lt;/title&amp;gt;&lt;br /&gt;
  &amp;lt;color&amp;gt;black&amp;lt;/color&amp;gt;&lt;br /&gt;
  &amp;lt;size&amp;gt;200&amp;lt;/size&amp;gt;&lt;br /&gt;
  &amp;lt;uploadedFileContents&amp;gt;HYC116_C6H6_FREQ.LOG&amp;lt;/uploadedFileContents&amp;gt;&lt;br /&gt;
&amp;lt;/jmolApplet&amp;gt;&amp;lt;/jmol&amp;gt;&lt;br /&gt;
&lt;br /&gt;
===Borazine===&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;Calculation type&amp;lt;/b&amp;gt;: Optimisation&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;Calculation Method&amp;lt;/b&amp;gt;: B3LYP&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;Basis set&amp;lt;/b&amp;gt;: 6-31G(d,p) &lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Summary table&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
[[file:Hyc116_borazine_summarytable.png]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Items table&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;pre&amp;gt;&lt;br /&gt;
Item               Value     Threshold  Converged?&lt;br /&gt;
 Maximum Force            0.000085     0.000450     YES&lt;br /&gt;
 RMS     Force            0.000033     0.000300     YES&lt;br /&gt;
 Maximum Displacement     0.000250     0.001800     YES&lt;br /&gt;
 RMS     Displacement     0.000074     0.001200     YES&lt;br /&gt;
&amp;lt;/pre&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Frequency log file&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
[[Media:HYC116_BORAZINE_FREQ.LOG]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Frequencies&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;pre&amp;gt;&lt;br /&gt;
Low frequencies ---  -12.6626  -12.6626   -8.9272   -0.0211   -0.0104   -0.0104&lt;br /&gt;
Low frequencies ---  289.1112  289.1112  403.8613&lt;br /&gt;
&amp;lt;/pre&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;jmol of Borazine&#039;&#039;&#039;&lt;br /&gt;
&amp;lt;jmol&amp;gt;&amp;lt;jmolApplet&amp;gt;&lt;br /&gt;
  &amp;lt;title&amp;gt;optimised Borazine&amp;lt;/title&amp;gt;&lt;br /&gt;
  &amp;lt;color&amp;gt;black&amp;lt;/color&amp;gt;&lt;br /&gt;
  &amp;lt;size&amp;gt;200&amp;lt;/size&amp;gt;&lt;br /&gt;
  &amp;lt;uploadedFileContents&amp;gt;HYC116_BORAZINE_FREQ.LOG&amp;lt;/uploadedFileContents&amp;gt;&lt;br /&gt;
&amp;lt;/jmolApplet&amp;gt;&amp;lt;/jmol&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
===Charge distribution===&lt;br /&gt;
&lt;br /&gt;
An NBO charge analysis was carried out on both the optimised benzene and borazine. Visualisations of the charge distribution are shown in the table below, with the colour range going from -1.102 to 1.102 for both molecule. This large scale was chosen as it allows direct comparison of the charge on any atoms in these two molecules and shows the relative magnitude of charges on all these atoms. Negative charges are shown in red, and positive charges are shown in green. A neutral charge is displayed in black, so the smaller a charge is (positive or negative), the darker its colour representation is. Larger charges are shown in brighter colours. The charges are also displayed on the atoms as numbers with a neutral charge being zero. Negative charges are shown as negative number and positive charges are shown as positive numbers. &lt;br /&gt;
&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot;&lt;br /&gt;
!&lt;br /&gt;
!Benzene&lt;br /&gt;
!Borazine&lt;br /&gt;
|-&lt;br /&gt;
!Visualisation of charge distribution&lt;br /&gt;
|[[File:Hyc116_benzene_charge_distribution1.png|500x500px|thumb|centre|Charge distribution of Benzene visualisation]]&lt;br /&gt;
|[[File:Hyc116_borazine_charge_distribution1.png|500x500px|thumb|centre|Charge distribution of Borazine visualisation]]&lt;br /&gt;
|-&lt;br /&gt;
!Charge &lt;br /&gt;
|Carbon: -0.239&lt;br /&gt;
&lt;br /&gt;
Hydrogen: 0.239&lt;br /&gt;
|Nitrogen: -1.102 &lt;br /&gt;
&lt;br /&gt;
Boron: 0.747&lt;br /&gt;
&lt;br /&gt;
Hydrogen (bonded to N): 0.432&lt;br /&gt;
&lt;br /&gt;
Hydrogen (bonded to B): -0.077&lt;br /&gt;
|-&lt;br /&gt;
!Discussion&lt;br /&gt;
|From the visualisation, it is shown that there is a slightly negative charge on the carbon atoms, and a positive charge of the same magnitude on the hydrogen atoms. All the carbon atoms have the same charge as they are in identical environments. The same applies to all the hydrogen atoms. This is due to the highly symmetrical structure of benzene. Since the same colour scale was used for both benzene and borazine, and the charges are much smaller in magnitude on atoms in benzene than atoms on borazine, the colours on the charge distribution visualisation is much darker. &lt;br /&gt;
|From the colours displayed on the charge distribution visualisation as well as the charge values, it is shown that nitrogen has a relatively large negative charge, while boron has a positive charge. This is due to the difference in electrogenativity between these atoms: nitrogen atoms are more electronegative than boron and tends to attract electrons towards themselves. It is worth noting that the hydrogen atoms do not all have the same charge. The hydrogen atoms bonded to boron have a slightly negative charge, and the ones bonded to nitrogen have a small positive charge. &lt;br /&gt;
&lt;br /&gt;
The fact that the same colour scale was used for both molecules comes in helpful here. It allows the charges on atoms to be compared directly. For example, just from looking at the colours, one can tell that or example, even though both carbon and nitrogen are electronegative, nitrogen is much more electronegative, which is quantitatively shown by Pauling&#039;s electronegativity scale.&amp;lt;ref&amp;gt;http://www.tutor-homework.com/Chemistry_Help/electronegativity_table/electronegativity.html (Accessed: 24.0502018&amp;lt;/ref&amp;gt;&lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
===Comparative MOs of Benzene and Borazine===&lt;br /&gt;
&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot;&lt;br /&gt;
!&lt;br /&gt;
!Benzene&lt;br /&gt;
!Borazine&lt;br /&gt;
!Comparison and Discussion&lt;br /&gt;
|-&lt;br /&gt;
!1st comparative pair&lt;br /&gt;
|[[File:Hyc116_benzene_1st_MO_pair_7.png|200x200px|centre]]&lt;br /&gt;
|[[File:Hyc116_borazine_1st_MO_pair_level9.png|200x200px|centre]]&lt;br /&gt;
|MO 9 of both benzene and borazine are comparable. They both show delocalised molecular orbital with an overall bonding character. There is a nodal plane across the molecular orbitals for both benzene and borazine. For benzene, there is contribution from all the carbon and hydrogen s orbitals. Moreover, the molecular orbitals are symmetric to their counterpart of opposite phase. That is not the case for borazine; they are less symmetric in borazine. Nitrogen atoms are more electronegative than boron atoms and pull electron density towards themselves, resulting in a larger MO. There is contribution from all the boron and nitrogen s orbitals, and three of the hydrogen s orbitals, though not all of them. &lt;br /&gt;
|-&lt;br /&gt;
!2nd comparative pair&lt;br /&gt;
|[[File:Hyc116_benzene_2nd_MO_pair_10.png|200x200px|centre]]&lt;br /&gt;
|[[File:Hyc116_borazine_2nd_MO_pair_level11.png|200x200px|centre]]&lt;br /&gt;
|&lt;br /&gt;
|-&lt;br /&gt;
!3rd comparative pair&lt;br /&gt;
|[[File:Hyc116_benzene_3rd_MO_pair_21.png|200x200px|centre]]&lt;br /&gt;
|[[File:Hyc116_borazine_3rd_MO_pair_level21.png|200x200px|centre]]&lt;br /&gt;
|&lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
===Aromaticity: some theories===&lt;br /&gt;
&lt;br /&gt;
==References==&lt;br /&gt;
{{reflist}}&lt;/div&gt;</summary>
		<author><name>Hyc116</name></author>
	</entry>
	<entry>
		<id>https://chemwiki.ch.ic.ac.uk/index.php?title=File:Hyc116_nh3bh3_631g_summarytable1.png&amp;diff=731337</id>
		<title>File:Hyc116 nh3bh3 631g summarytable1.png</title>
		<link rel="alternate" type="text/html" href="https://chemwiki.ch.ic.ac.uk/index.php?title=File:Hyc116_nh3bh3_631g_summarytable1.png&amp;diff=731337"/>
		<updated>2018-05-25T12:01:38Z</updated>

		<summary type="html">&lt;p&gt;Hyc116: &lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;&lt;/div&gt;</summary>
		<author><name>Hyc116</name></author>
	</entry>
	<entry>
		<id>https://chemwiki.ch.ic.ac.uk/index.php?title=File:Hyc116_nh3bh3_631g_summarytable.png&amp;diff=731336</id>
		<title>File:Hyc116 nh3bh3 631g summarytable.png</title>
		<link rel="alternate" type="text/html" href="https://chemwiki.ch.ic.ac.uk/index.php?title=File:Hyc116_nh3bh3_631g_summarytable.png&amp;diff=731336"/>
		<updated>2018-05-25T12:00:57Z</updated>

		<summary type="html">&lt;p&gt;Hyc116: Hyc116 uploaded a new version of File:Hyc116 nh3bh3 631g summarytable.png&lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;&lt;/div&gt;</summary>
		<author><name>Hyc116</name></author>
	</entry>
	<entry>
		<id>https://chemwiki.ch.ic.ac.uk/index.php?title=MO_hyc116&amp;diff=730192</id>
		<title>MO hyc116</title>
		<link rel="alternate" type="text/html" href="https://chemwiki.ch.ic.ac.uk/index.php?title=MO_hyc116&amp;diff=730192"/>
		<updated>2018-05-24T17:42:11Z</updated>

		<summary type="html">&lt;p&gt;Hyc116: &lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;==BH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;==&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;Calculation type&amp;lt;/b&amp;gt;: Optimisation&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;Calculation Method&amp;lt;/b&amp;gt;: B3LYP&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;Basis set&amp;lt;/b&amp;gt;: 6-31G(d,p) &lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Summary table&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
[[file:Hyc116_bh3_631g_opt_summarytable.png]]&lt;br /&gt;
&lt;br /&gt;
The above summary table was obtained after the 2nd optimisation of BH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt; (after the initial optimisation using the 3-21G basis set). Notice how the symmetry is incorrect and shown as Cs. This is because the symmetry was manually broken at the beginning by changing the bond length of B-H bonds. The point group was manually adjusted and the molecule was optimised again before the frequency analysis and the new summary table is attached below.&lt;br /&gt;
&lt;br /&gt;
[[file:Hyc116_bh3_correctsummarytable.png]]&lt;br /&gt;
&lt;br /&gt;
The above summary table was obtained from the optimisation after adjusting the symmetry. The point shown in this summary table is D&amp;lt;sub&amp;gt;3h&amp;lt;/sub&amp;gt;, which is the correct for BH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;. &lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Items table&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
Below is the items table taken from the optimisation with the correct point group.&lt;br /&gt;
&lt;br /&gt;
&amp;lt;pre&amp;gt;&lt;br /&gt;
Item               Value     Threshold  Converged?&lt;br /&gt;
 Maximum Force            0.000015     0.000450     YES&lt;br /&gt;
 RMS     Force            0.000010     0.000300     YES&lt;br /&gt;
 Maximum Displacement     0.000058     0.001800     YES&lt;br /&gt;
 RMS     Displacement     0.000038     0.001200     YES&lt;br /&gt;
&amp;lt;/pre&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Frequency log file&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
[[Media:HYC116 BH3 FREQ.LOG]] &lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Frequencies&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;pre&amp;gt;&lt;br /&gt;
Low frequencies ---  -10.3498   -3.4492   -1.2454   -0.0055    0.4779    3.2165&lt;br /&gt;
Low frequencies --- 1162.9519 1213.1527 1213.1554&lt;br /&gt;
&amp;lt;/pre&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;jmol of BH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;&#039;&#039;&#039;&lt;br /&gt;
&amp;lt;jmol&amp;gt;&amp;lt;jmolApplet&amp;gt;&lt;br /&gt;
  &amp;lt;title&amp;gt;optimised BH3&amp;lt;/title&amp;gt;&lt;br /&gt;
  &amp;lt;color&amp;gt;black&amp;lt;/color&amp;gt;&lt;br /&gt;
  &amp;lt;size&amp;gt;200&amp;lt;/size&amp;gt;&lt;br /&gt;
  &amp;lt;uploadedFileContents&amp;gt;HYC116_BH3_FREQ.LOG&amp;lt;/uploadedFileContents&amp;gt;&lt;br /&gt;
&amp;lt;/jmolApplet&amp;gt;&amp;lt;/jmol&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
===Vibrational spectrum===&lt;br /&gt;
&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot;&lt;br /&gt;
!wavenumber (cm&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;)&lt;br /&gt;
!Intensity (arbitrary units)&lt;br /&gt;
!symmetry&lt;br /&gt;
!IR active?&lt;br /&gt;
!type&lt;br /&gt;
|-&lt;br /&gt;
|1163&lt;br /&gt;
|93&lt;br /&gt;
|A&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;&#039; &#039;&lt;br /&gt;
|Yes&lt;br /&gt;
|Out of plane bend&lt;br /&gt;
|-&lt;br /&gt;
|1213&lt;br /&gt;
|14&lt;br /&gt;
|E&#039;&lt;br /&gt;
|Very slight&lt;br /&gt;
|Bend&lt;br /&gt;
|-&lt;br /&gt;
|1213&lt;br /&gt;
|14&lt;br /&gt;
|E&#039;&lt;br /&gt;
|Very slight&lt;br /&gt;
|Bend&lt;br /&gt;
|-&lt;br /&gt;
|2582&lt;br /&gt;
|0&lt;br /&gt;
|A&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;&#039;&lt;br /&gt;
|No&lt;br /&gt;
|Symmetric stretch&lt;br /&gt;
|-&lt;br /&gt;
|2716&lt;br /&gt;
|126&lt;br /&gt;
|E&#039;&lt;br /&gt;
|Yes&lt;br /&gt;
|Asymmetric stretch&lt;br /&gt;
|-&lt;br /&gt;
|2716&lt;br /&gt;
|126&lt;br /&gt;
|E&#039;&lt;br /&gt;
|Yes&lt;br /&gt;
|Asymmetric stretch&lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;IR spectrum&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
[[file:Hyc116_ir_bh3.png|400*600]]&lt;br /&gt;
&lt;br /&gt;
There are only three peaks on the IR spectrum of BH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;, despite that there are 6 vibrational modes for the molecule. As shown in the table above, the symmetric stretching mode with A1 symmetry at 2582 cm&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt; is not IR active; naturally, that vibrational mode doesn’t give a peak on the IR spectrum. As shown from the table, two pairs of vibrational modes, the bond angle deformation/bend at 1213 cm&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt; and the asymmetric bond stretch at 2716 cm&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;, are degenerate with the symmetry label E. This means that they have the same energy, and hence give the same wavenumber on the IR spectrum. Each pair of degenerate vibrational modes give rise to one peak. This leaves three peaks, as confirmed by the IR spectrum above.&lt;br /&gt;
&lt;br /&gt;
===Molecular orbitals of BH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;===&lt;br /&gt;
&lt;br /&gt;
[[file:hyc116_bh3_MO_diagram.png]]&lt;br /&gt;
&lt;br /&gt;
The above molecular orbital diagram was taken from Dr Patricia Hunt&#039;s &amp;lt;i&amp;gt;Lecture 4 Tutorial Problem Model Answers&amp;lt;/i&amp;gt;.&amp;lt;ref&amp;gt;P. Hunt, &amp;quot;Lecture 4 Tutorial Problem Model Answers&amp;quot;, 2 (2018)&amp;lt;/ref&amp;gt; Diagrams of the &amp;quot;real&amp;quot; MOs were obtained from Gaussian.&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
There is no significant difference between the LCAO MOs and the real ones. Features such as orbital phases are shown clearly on both the LCAO MOs and the real MOs, illustrating the bonding/anti-bonding characters of the molecular orbitals. This suggests that the the qualitative MO theory is highly accurate and useful when studying the molecular orbitals of molecules.&lt;br /&gt;
&lt;br /&gt;
==Associated energies: ammonium borane==&lt;br /&gt;
&lt;br /&gt;
===NH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;===&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;Calculation type&amp;lt;/b&amp;gt;: Optimisation&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;Calculation Method&amp;lt;/b&amp;gt;: B3LYP&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;Basis set&amp;lt;/b&amp;gt;: 6-31G(d,p) &lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Summary table&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
[[file:Hyc116_nh3_631g_summarytable.png]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Items table&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;pre&amp;gt;&lt;br /&gt;
Item               Value     Threshold  Converged?&lt;br /&gt;
 Maximum Force            0.000006     0.000450     YES&lt;br /&gt;
 RMS     Force            0.000004     0.000300     YES&lt;br /&gt;
 Maximum Displacement     0.000012     0.001800     YES&lt;br /&gt;
 RMS     Displacement     0.000008     0.001200     YES&lt;br /&gt;
&amp;lt;/pre&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Frequency log file&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
[[Media:HYC116_NH3_FREQ.LOG]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Frequencies&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;pre&amp;gt;&lt;br /&gt;
Low frequencies ---   -8.5646   -8.5588   -0.0047    0.0454    0.1784   26.4183&lt;br /&gt;
Low frequencies --- 1089.7603 1694.1865 1694.1865&lt;br /&gt;
&amp;lt;/pre&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;jmol of NH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;&#039;&#039;&#039;&lt;br /&gt;
&amp;lt;jmol&amp;gt;&amp;lt;jmolApplet&amp;gt;&lt;br /&gt;
  &amp;lt;title&amp;gt;optimised NH3&amp;lt;/title&amp;gt;&lt;br /&gt;
  &amp;lt;color&amp;gt;black&amp;lt;/color&amp;gt;&lt;br /&gt;
  &amp;lt;size&amp;gt;200&amp;lt;/size&amp;gt;&lt;br /&gt;
  &amp;lt;uploadedFileContents&amp;gt;HYC116_NH3_FREQ.LOG&amp;lt;/uploadedFileContents&amp;gt;&lt;br /&gt;
&amp;lt;/jmolApplet&amp;gt;&amp;lt;/jmol&amp;gt;&lt;br /&gt;
&lt;br /&gt;
===NH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;BH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;===&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;Calculation type&amp;lt;/b&amp;gt;: Optimisation&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;Calculation Method&amp;lt;/b&amp;gt;: B3LYP&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;Basis set&amp;lt;/b&amp;gt;: 6-31G(d,p) &lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Summary table&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
[[file:Hyc116_nh3bh3_631g_summarytable.png]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Items table&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;pre&amp;gt;&lt;br /&gt;
Item               Value     Threshold  Converged?&lt;br /&gt;
 Maximum Force            0.000123     0.000450     YES&lt;br /&gt;
 RMS     Force            0.000058     0.000300     YES&lt;br /&gt;
 Maximum Displacement     0.000515     0.001800     YES&lt;br /&gt;
 RMS     Displacement     0.000296     0.001200     YES&lt;br /&gt;
&amp;lt;/pre&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Frequency log file&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
[[Media:HYC116_NH3BH3_FREQ.LOG]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Frequencies&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;pre&amp;gt;&lt;br /&gt;
Low frequencies ---   -0.0014   -0.0011   -0.0006    6.9624   20.4518   43.5542&lt;br /&gt;
Low frequencies ---  266.4530  632.2458  639.0504&lt;br /&gt;
&amp;lt;/pre&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;jmol of NH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;BH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;&#039;&#039;&#039;&lt;br /&gt;
&amp;lt;jmol&amp;gt;&amp;lt;jmolApplet&amp;gt;&lt;br /&gt;
  &amp;lt;title&amp;gt;optimised NH3BH3&amp;lt;/title&amp;gt;&lt;br /&gt;
  &amp;lt;color&amp;gt;black&amp;lt;/color&amp;gt;&lt;br /&gt;
  &amp;lt;size&amp;gt;200&amp;lt;/size&amp;gt;&lt;br /&gt;
  &amp;lt;uploadedFileContents&amp;gt;HYC116_NH3BH3_FREQ.LOG&amp;lt;/uploadedFileContents&amp;gt;&lt;br /&gt;
&amp;lt;/jmolApplet&amp;gt;&amp;lt;/jmol&amp;gt;&lt;br /&gt;
&lt;br /&gt;
===Association energy===&lt;br /&gt;
&lt;br /&gt;
E(BH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;) (using the optimisation with the correct symmetry) = -26.61532363 a.u. = &amp;lt;b&amp;gt;-26.61532 a.u. (5 d.p.)&amp;lt;/b&amp;gt;&lt;br /&gt;
&lt;br /&gt;
E(NH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;) = -56.55776873 a.u. = &amp;lt;b&amp;gt;-56.55777 a.u. (5 d.p.)&amp;lt;/b&amp;gt;&lt;br /&gt;
&lt;br /&gt;
E(NH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;BH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;) = -83.22468893 a.u. = &amp;lt;b&amp;gt;-83.22469 a.u. (5 d.p.)&amp;lt;/b&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
Carrying out calculations using numbers which has already been rounded up can possibly result in errors in the last digit. Hence, here the calculations were carried out using the numbers provided from the optimisations (i.e. with more decimal places than necessary); the answer was then rounded up to the desired accuracy. &lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
ΔE = E(NH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;BH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;)-[E(NH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;)+E(BH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;)]&lt;br /&gt;
&lt;br /&gt;
ΔE = -83.22468893 - (-56.55776873 + -26.61532363) = -0.05159657 a.u. &lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;ΔE = -0.05160 a.u. (5 d.p.)&amp;lt;/b&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Converting energy from a.u. to kJ/mol&#039;&#039;&#039;&lt;br /&gt;
An atomic unit for energy is Hartree, which is equal to 2625.5 kJ/mol.&lt;br /&gt;
&amp;lt;ref&amp;gt;https://cccbdb.nist.gov/hartree.asp (Accessed: 22.05.2018)&amp;lt;/ref&amp;gt;&lt;br /&gt;
 &lt;br /&gt;
&lt;br /&gt;
So ΔE in kJ/mol = -0.05159657 * 2625.5 = -135.466794535 kJ/mol&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;ΔE = -135 kJ/mol (nearest integer)&amp;lt;/b&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
The energy difference calculated above comes from the formation of the B-N dative bond. It is a relatively weak bond. According to a bond energy data sheet provided by the University of California,&amp;lt;ref&amp;gt;https://labs.chem.ucsb.edu/zakarian/armen/11---bonddissociationenergy.pdf (Accessed: 24.05.2018)&amp;lt;/ref&amp;gt;  the bond energy of the C-C bond of an ethane molecule is 368 kJ/mol. This is a fair comparison to the NH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;BH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt; molecule as the two molecules have the same structure, only with the carbon atoms on ethane swapped for Boron and Nitrogen in NH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;BH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;&lt;br /&gt;
&lt;br /&gt;
==Using a mixture of basis-sets and pseudo-potentials==&lt;br /&gt;
&lt;br /&gt;
===BBr&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;===&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;Calculation type&amp;lt;/b&amp;gt;: Optimisation&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;Calculation Method&amp;lt;/b&amp;gt;: B3LYP&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;Basis set&amp;lt;/b&amp;gt;: Boron: 6-31G(d,p) ; Br: LANL2DZ&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
Larger calculations are often sent to a web-server to run on a high-performance computer instead of a desktop. In order to experience and learn to use a web-server, the optimisation and the frequency analysis for BBr&amp;lt;sub&amp;gt;3&amp;lt;/sub were both sent and done on a server instead of the desktop. The calculation results were downloaded from the web-server once they were finished.   &lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Summary table&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
[[file:Hyc116_bbr3_opt_summarytable.png]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Items table&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;pre&amp;gt;&lt;br /&gt;
Item               Value     Threshold  Converged?&lt;br /&gt;
 Maximum Force            0.000008     0.000450     YES&lt;br /&gt;
 RMS     Force            0.000005     0.000300     YES&lt;br /&gt;
 Maximum Displacement     0.000036     0.001800     YES&lt;br /&gt;
 RMS     Displacement     0.000023     0.001200     YES&lt;br /&gt;
&amp;lt;/pre&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Frequency log file&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
[[Media:Hyc116_bbr3_freq.log]]&lt;br /&gt;
&lt;br /&gt;
Attached above is the frequency file saved onto the computer from the SCAN server portal. The frequency file was also published on the chemistry database DSpace. {{DOI|10042/202442}}&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Frequencies&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;pre&amp;gt;&lt;br /&gt;
Low frequencies ---   -0.0137   -0.0064   -0.0046    2.4315    2.4315    4.8421&lt;br /&gt;
Low frequencies ---  155.9631  155.9651  267.7052&lt;br /&gt;
&amp;lt;/pre&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;jmol of BBr&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;&#039;&#039;&#039;&lt;br /&gt;
&amp;lt;jmol&amp;gt;&amp;lt;jmolApplet&amp;gt;&lt;br /&gt;
  &amp;lt;title&amp;gt;optimised BBr3&amp;lt;/title&amp;gt;&lt;br /&gt;
  &amp;lt;color&amp;gt;black&amp;lt;/color&amp;gt;&lt;br /&gt;
  &amp;lt;size&amp;gt;200&amp;lt;/size&amp;gt;&lt;br /&gt;
  &amp;lt;uploadedFileContents&amp;gt;Hyc116_bbr3_freq.log&amp;lt;/uploadedFileContents&amp;gt;&lt;br /&gt;
&amp;lt;/jmolApplet&amp;gt;&amp;lt;/jmol&amp;gt;&lt;br /&gt;
&lt;br /&gt;
==Aromaticity==&lt;br /&gt;
&lt;br /&gt;
===Benzene===&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;Calculation type&amp;lt;/b&amp;gt;: Optimisation&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;Calculation Method&amp;lt;/b&amp;gt;: B3LYP&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;Basis set&amp;lt;/b&amp;gt;: 6-31G(d,p) &lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Summary table&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
[[file:Hyc116_c6h6_summarytable.png]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Items table&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;pre&amp;gt;&lt;br /&gt;
Item               Value     Threshold  Converged?&lt;br /&gt;
 Maximum Force            0.000193     0.000450     YES&lt;br /&gt;
 RMS     Force            0.000079     0.000300     YES&lt;br /&gt;
 Maximum Displacement     0.000830     0.001800     YES&lt;br /&gt;
 RMS     Displacement     0.000294     0.001200     YES&lt;br /&gt;
&amp;lt;/pre&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Frequency log file&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
[[Media:HYC116_C6H6_FREQ.LOG]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Frequencies&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;pre&amp;gt;&lt;br /&gt;
Low frequencies ---   -3.5606   -3.5606   -0.0089   -0.0043   -0.0043   10.0905&lt;br /&gt;
Low frequencies ---  413.9582  413.9582  621.1416&lt;br /&gt;
&amp;lt;/pre&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;jmol of C&amp;lt;sub&amp;gt;6&amp;lt;/sub&amp;gt;H&amp;lt;sub&amp;gt;6&amp;lt;/sub&amp;gt;&#039;&#039;&#039;&lt;br /&gt;
&amp;lt;jmol&amp;gt;&amp;lt;jmolApplet&amp;gt;&lt;br /&gt;
  &amp;lt;title&amp;gt;optimised Benzene&amp;lt;/title&amp;gt;&lt;br /&gt;
  &amp;lt;color&amp;gt;black&amp;lt;/color&amp;gt;&lt;br /&gt;
  &amp;lt;size&amp;gt;200&amp;lt;/size&amp;gt;&lt;br /&gt;
  &amp;lt;uploadedFileContents&amp;gt;HYC116_C6H6_FREQ.LOG&amp;lt;/uploadedFileContents&amp;gt;&lt;br /&gt;
&amp;lt;/jmolApplet&amp;gt;&amp;lt;/jmol&amp;gt;&lt;br /&gt;
&lt;br /&gt;
===Borazine===&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;Calculation type&amp;lt;/b&amp;gt;: Optimisation&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;Calculation Method&amp;lt;/b&amp;gt;: B3LYP&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;Basis set&amp;lt;/b&amp;gt;: 6-31G(d,p) &lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Summary table&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
[[file:Hyc116_borazine_summarytable.png]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Items table&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;pre&amp;gt;&lt;br /&gt;
Item               Value     Threshold  Converged?&lt;br /&gt;
 Maximum Force            0.000085     0.000450     YES&lt;br /&gt;
 RMS     Force            0.000033     0.000300     YES&lt;br /&gt;
 Maximum Displacement     0.000250     0.001800     YES&lt;br /&gt;
 RMS     Displacement     0.000074     0.001200     YES&lt;br /&gt;
&amp;lt;/pre&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Frequency log file&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
[[Media:HYC116_BORAZINE_FREQ.LOG]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Frequencies&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;pre&amp;gt;&lt;br /&gt;
Low frequencies ---  -12.6626  -12.6626   -8.9272   -0.0211   -0.0104   -0.0104&lt;br /&gt;
Low frequencies ---  289.1112  289.1112  403.8613&lt;br /&gt;
&amp;lt;/pre&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;jmol of Borazine&#039;&#039;&#039;&lt;br /&gt;
&amp;lt;jmol&amp;gt;&amp;lt;jmolApplet&amp;gt;&lt;br /&gt;
  &amp;lt;title&amp;gt;optimised Borazine&amp;lt;/title&amp;gt;&lt;br /&gt;
  &amp;lt;color&amp;gt;black&amp;lt;/color&amp;gt;&lt;br /&gt;
  &amp;lt;size&amp;gt;200&amp;lt;/size&amp;gt;&lt;br /&gt;
  &amp;lt;uploadedFileContents&amp;gt;HYC116_BORAZINE_FREQ.LOG&amp;lt;/uploadedFileContents&amp;gt;&lt;br /&gt;
&amp;lt;/jmolApplet&amp;gt;&amp;lt;/jmol&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
===Charge distribution===&lt;br /&gt;
&lt;br /&gt;
An NBO charge analysis was carried out on both the optimised benzene and borazine. Visualisations of the charge distribution are shown in the table below, with the colour range going from -1.102 to 1.102 for both molecule. This large scale was chosen as it allows direct comparison of the charge on any atoms in these two molecules and shows the relative magnitude of charges on all these atoms. Negative charges are shown in red, and positive charges are shown in green. A neutral charge is displayed in black, so the smaller a charge is (positive or negative), the darker its colour representation is. Larger charges are shown in brighter colours. The charges are also displayed on the atoms as numbers with a neutral charge being zero. Negative charges are shown as negative number and positive charges are shown as positive numbers. &lt;br /&gt;
&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot;&lt;br /&gt;
!&lt;br /&gt;
!Benzene&lt;br /&gt;
!Borazine&lt;br /&gt;
|-&lt;br /&gt;
!Visualisation of charge distribution&lt;br /&gt;
|[[File:Hyc116_benzene_charge_distribution1.png|500x500px|thumb|centre|Charge distribution of Benzene visualisation]]&lt;br /&gt;
|[[File:Hyc116_borazine_charge_distribution1.png|500x500px|thumb|centre|Charge distribution of Borazine visualisation]]&lt;br /&gt;
|-&lt;br /&gt;
!Charge &lt;br /&gt;
|Carbon: -0.239&lt;br /&gt;
&lt;br /&gt;
Hydrogen: 0.239&lt;br /&gt;
|Nitrogen: -1.102 &lt;br /&gt;
&lt;br /&gt;
Boron: 0.747&lt;br /&gt;
&lt;br /&gt;
Hydrogen (bonded to N): 0.432&lt;br /&gt;
&lt;br /&gt;
Hydrogen (bonded to B): -0.077&lt;br /&gt;
|-&lt;br /&gt;
!Discussion&lt;br /&gt;
|From the visualisation, it is shown that there is a slightly negative charge on the carbon atoms, and a positive charge of the same magnitude on the hydrogen atoms. All the carbon atoms have the same charge as they are in identical environments. The same applies to all the hydrogen atoms. This is due to the highly symmetrical structure of benzene. Since the same colour scale was used for both benzene and borazine, and the charges are much smaller in magnitude on atoms in benzene than atoms on borazine, the colours on the charge distribution visualisation is much darker. &lt;br /&gt;
|From the colours displayed on the charge distribution visualisation as well as the charge values, it is shown that nitrogen has a relatively large negative charge, while boron has a positive charge. This is due to the difference in electrogenativity between these atoms: nitrogen atoms are more electronegative than boron and tends to attract electrons towards themselves. It is worth noting that the hydrogen atoms do not all have the same charge. The hydrogen atoms bonded to boron have a slightly negative charge, and the ones bonded to nitrogen have a small positive charge. &lt;br /&gt;
&lt;br /&gt;
The fact that the same colour scale was used for both molecules comes in helpful here. It allows the charges on atoms to be compared directly. For example, just from looking at the colours, one can tell that or example, even though both carbon and nitrogen are electronegative, nitrogen is much more electronegative, which is quantitatively shown by Pauling&#039;s electronegativity scale.&amp;lt;ref&amp;gt;http://www.tutor-homework.com/Chemistry_Help/electronegativity_table/electronegativity.html (Accessed: 24.0502018&amp;lt;/ref&amp;gt;&lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
===Comparative MOs of Benzene and Borazine===&lt;br /&gt;
&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot;&lt;br /&gt;
!&lt;br /&gt;
!Benzene&lt;br /&gt;
!Borazine&lt;br /&gt;
!Comparison and Discussion&lt;br /&gt;
|-&lt;br /&gt;
!1st comparative pair&lt;br /&gt;
|[[File:Hyc116_benzene_1st_MO_pair_7.png|200x200px|centre]]&lt;br /&gt;
|[[File:Hyc116_borazine_1st_MO_pair_level9.png|200x200px|centre]]&lt;br /&gt;
|MO 9 of both benzene and borazine are comparable. They both show delocalised molecular orbital with an overall bonding character. There is a nodal plane across the molecular orbitals for both benzene and borazine. For benzene, there is contribution from all the carbon and hydrogen s orbitals. Moreover, the molecular orbitals are symmetric to their counterpart of opposite phase. That is not the case for borazine; they are less symmetric in borazine. Nitrogen atoms are more electronegative than boron atoms and pull electron density towards themselves, resulting in a larger MO. There is contribution from all the boron and nitrogen s orbitals, and three of the hydrogen s orbitals, though not all of them. &lt;br /&gt;
|-&lt;br /&gt;
!2nd comparative pair&lt;br /&gt;
|[[File:Hyc116_benzene_2nd_MO_pair_10.png|200x200px|centre]]&lt;br /&gt;
|[[File:Hyc116_borazine_2nd_MO_pair_level11.png|200x200px|centre]]&lt;br /&gt;
|&lt;br /&gt;
|-&lt;br /&gt;
!3rd comparative pair&lt;br /&gt;
|[[File:Hyc116_benzene_3rd_MO_pair_21.png|200x200px|centre]]&lt;br /&gt;
|[[File:Hyc116_borazine_3rd_MO_pair_level21.png|200x200px|centre]]&lt;br /&gt;
|&lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
===Aromaticity: some theories===&lt;br /&gt;
&lt;br /&gt;
==References==&lt;br /&gt;
{{reflist}}&lt;/div&gt;</summary>
		<author><name>Hyc116</name></author>
	</entry>
	<entry>
		<id>https://chemwiki.ch.ic.ac.uk/index.php?title=MO_hyc116&amp;diff=730190</id>
		<title>MO hyc116</title>
		<link rel="alternate" type="text/html" href="https://chemwiki.ch.ic.ac.uk/index.php?title=MO_hyc116&amp;diff=730190"/>
		<updated>2018-05-24T17:41:51Z</updated>

		<summary type="html">&lt;p&gt;Hyc116: /* References */&lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;==BH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;==&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;Calculation type&amp;lt;/b&amp;gt;: Optimisation&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;Calculation Method&amp;lt;/b&amp;gt;: B3LYP&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;Basis set&amp;lt;/b&amp;gt;: 6-31G(d,p) &lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Summary table&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
[[file:Hyc116_bh3_631g_opt_summarytable.png]]&lt;br /&gt;
&lt;br /&gt;
The above summary table was obtained after the 2nd optimisation of BH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt; (after the initial optimisation using the 3-21G basis set). Notice how the symmetry is incorrect and shown as Cs. This is because the symmetry was manually broken at the beginning by changing the bond length of B-H bonds. The point group was manually adjusted and the molecule was optimised again before the frequency analysis and the new summary table is attached below.&lt;br /&gt;
&lt;br /&gt;
[[file:Hyc116_bh3_correctsummarytable.png]]&lt;br /&gt;
&lt;br /&gt;
The above summary table was obtained from the optimisation after adjusting the symmetry. The point shown in this summary table is D&amp;lt;sub&amp;gt;3h&amp;lt;/sub&amp;gt;, which is the correct for BH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;. &lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Items table&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
Below is the items table taken from the optimisation with the correct point group.&lt;br /&gt;
&lt;br /&gt;
&amp;lt;pre&amp;gt;&lt;br /&gt;
Item               Value     Threshold  Converged?&lt;br /&gt;
 Maximum Force            0.000015     0.000450     YES&lt;br /&gt;
 RMS     Force            0.000010     0.000300     YES&lt;br /&gt;
 Maximum Displacement     0.000058     0.001800     YES&lt;br /&gt;
 RMS     Displacement     0.000038     0.001200     YES&lt;br /&gt;
&amp;lt;/pre&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Frequency log file&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
[[Media:HYC116 BH3 FREQ.LOG]] &lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Frequencies&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;pre&amp;gt;&lt;br /&gt;
Low frequencies ---  -10.3498   -3.4492   -1.2454   -0.0055    0.4779    3.2165&lt;br /&gt;
Low frequencies --- 1162.9519 1213.1527 1213.1554&lt;br /&gt;
&amp;lt;/pre&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;jmol of BH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;&#039;&#039;&#039;&lt;br /&gt;
&amp;lt;jmol&amp;gt;&amp;lt;jmolApplet&amp;gt;&lt;br /&gt;
  &amp;lt;title&amp;gt;optimised BH3&amp;lt;/title&amp;gt;&lt;br /&gt;
  &amp;lt;color&amp;gt;black&amp;lt;/color&amp;gt;&lt;br /&gt;
  &amp;lt;size&amp;gt;200&amp;lt;/size&amp;gt;&lt;br /&gt;
  &amp;lt;uploadedFileContents&amp;gt;HYC116_BH3_FREQ.LOG&amp;lt;/uploadedFileContents&amp;gt;&lt;br /&gt;
&amp;lt;/jmolApplet&amp;gt;&amp;lt;/jmol&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
===Vibrational spectrum===&lt;br /&gt;
&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot;&lt;br /&gt;
!wavenumber (cm&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;)&lt;br /&gt;
!Intensity (arbitrary units)&lt;br /&gt;
!symmetry&lt;br /&gt;
!IR active?&lt;br /&gt;
!type&lt;br /&gt;
|-&lt;br /&gt;
|1163&lt;br /&gt;
|93&lt;br /&gt;
|A&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;&#039; &#039;&lt;br /&gt;
|Yes&lt;br /&gt;
|Out of plane bend&lt;br /&gt;
|-&lt;br /&gt;
|1213&lt;br /&gt;
|14&lt;br /&gt;
|E&#039;&lt;br /&gt;
|Very slight&lt;br /&gt;
|Bend&lt;br /&gt;
|-&lt;br /&gt;
|1213&lt;br /&gt;
|14&lt;br /&gt;
|E&#039;&lt;br /&gt;
|Very slight&lt;br /&gt;
|Bend&lt;br /&gt;
|-&lt;br /&gt;
|2582&lt;br /&gt;
|0&lt;br /&gt;
|A&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;&#039;&lt;br /&gt;
|No&lt;br /&gt;
|Symmetric stretch&lt;br /&gt;
|-&lt;br /&gt;
|2716&lt;br /&gt;
|126&lt;br /&gt;
|E&#039;&lt;br /&gt;
|Yes&lt;br /&gt;
|Asymmetric stretch&lt;br /&gt;
|-&lt;br /&gt;
|2716&lt;br /&gt;
|126&lt;br /&gt;
|E&#039;&lt;br /&gt;
|Yes&lt;br /&gt;
|Asymmetric stretch&lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;IR spectrum&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
[[file:Hyc116_ir_bh3.png|400*600]]&lt;br /&gt;
&lt;br /&gt;
There are only three peaks on the IR spectrum of BH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;, despite that there are 6 vibrational modes for the molecule. As shown in the table above, the symmetric stretching mode with A1 symmetry at 2582 cm&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt; is not IR active; naturally, that vibrational mode doesn’t give a peak on the IR spectrum. As shown from the table, two pairs of vibrational modes, the bond angle deformation/bend at 1213 cm&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt; and the asymmetric bond stretch at 2716 cm&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;, are degenerate with the symmetry label E. This means that they have the same energy, and hence give the same wavenumber on the IR spectrum. Each pair of degenerate vibrational modes give rise to one peak. This leaves three peaks, as confirmed by the IR spectrum above.&lt;br /&gt;
&lt;br /&gt;
===Molecular orbitals of BH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;===&lt;br /&gt;
&lt;br /&gt;
[[file:hyc116_bh3_MO_diagram.png]]&lt;br /&gt;
&lt;br /&gt;
The above molecular orbital diagram was taken from Dr Patricia Hunt&#039;s &amp;lt;i&amp;gt;Lecture 4 Tutorial Problem Model Answers&amp;lt;/i&amp;gt;.&amp;lt;ref&amp;gt;P. Hunt, &amp;quot;Lecture 4 Tutorial Problem Model Answers&amp;quot;, 2 (2018)&amp;lt;/ref&amp;gt; Diagrams of the &amp;quot;real&amp;quot; MOs were obtained from Gaussian.&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
There is no significant difference between the LCAO MOs and the real ones. Features such as orbital phases are shown clearly on both the LCAO MOs and the real MOs, illustrating the bonding/anti-bonding characters of the molecular orbitals. This suggests that the the qualitative MO theory is highly accurate and useful when studying the molecular orbitals of molecules.&lt;br /&gt;
&lt;br /&gt;
==Associated energies: ammonium borane==&lt;br /&gt;
&lt;br /&gt;
===NH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;===&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;Calculation type&amp;lt;/b&amp;gt;: Optimisation&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;Calculation Method&amp;lt;/b&amp;gt;: B3LYP&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;Basis set&amp;lt;/b&amp;gt;: 6-31G(d,p) &lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Summary table&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
[[file:Hyc116_nh3_631g_summarytable.png]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Items table&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;pre&amp;gt;&lt;br /&gt;
Item               Value     Threshold  Converged?&lt;br /&gt;
 Maximum Force            0.000006     0.000450     YES&lt;br /&gt;
 RMS     Force            0.000004     0.000300     YES&lt;br /&gt;
 Maximum Displacement     0.000012     0.001800     YES&lt;br /&gt;
 RMS     Displacement     0.000008     0.001200     YES&lt;br /&gt;
&amp;lt;/pre&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Frequency log file&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
[[Media:HYC116_NH3_FREQ.LOG]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Frequencies&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;pre&amp;gt;&lt;br /&gt;
Low frequencies ---   -8.5646   -8.5588   -0.0047    0.0454    0.1784   26.4183&lt;br /&gt;
Low frequencies --- 1089.7603 1694.1865 1694.1865&lt;br /&gt;
&amp;lt;/pre&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;jmol of NH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;&#039;&#039;&#039;&lt;br /&gt;
&amp;lt;jmol&amp;gt;&amp;lt;jmolApplet&amp;gt;&lt;br /&gt;
  &amp;lt;title&amp;gt;optimised NH3&amp;lt;/title&amp;gt;&lt;br /&gt;
  &amp;lt;color&amp;gt;black&amp;lt;/color&amp;gt;&lt;br /&gt;
  &amp;lt;size&amp;gt;200&amp;lt;/size&amp;gt;&lt;br /&gt;
  &amp;lt;uploadedFileContents&amp;gt;HYC116_NH3_FREQ.LOG&amp;lt;/uploadedFileContents&amp;gt;&lt;br /&gt;
&amp;lt;/jmolApplet&amp;gt;&amp;lt;/jmol&amp;gt;&lt;br /&gt;
&lt;br /&gt;
===NH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;BH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;===&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;Calculation type&amp;lt;/b&amp;gt;: Optimisation&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;Calculation Method&amp;lt;/b&amp;gt;: B3LYP&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;Basis set&amp;lt;/b&amp;gt;: 6-31G(d,p) &lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Summary table&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
[[file:Hyc116_nh3bh3_631g_summarytable.png]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Items table&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;pre&amp;gt;&lt;br /&gt;
Item               Value     Threshold  Converged?&lt;br /&gt;
 Maximum Force            0.000123     0.000450     YES&lt;br /&gt;
 RMS     Force            0.000058     0.000300     YES&lt;br /&gt;
 Maximum Displacement     0.000515     0.001800     YES&lt;br /&gt;
 RMS     Displacement     0.000296     0.001200     YES&lt;br /&gt;
&amp;lt;/pre&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Frequency log file&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
[[Media:HYC116_NH3BH3_FREQ.LOG]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Frequencies&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;pre&amp;gt;&lt;br /&gt;
Low frequencies ---   -0.0014   -0.0011   -0.0006    6.9624   20.4518   43.5542&lt;br /&gt;
Low frequencies ---  266.4530  632.2458  639.0504&lt;br /&gt;
&amp;lt;/pre&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;jmol of NH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;BH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;&#039;&#039;&#039;&lt;br /&gt;
&amp;lt;jmol&amp;gt;&amp;lt;jmolApplet&amp;gt;&lt;br /&gt;
  &amp;lt;title&amp;gt;optimised NH3BH3&amp;lt;/title&amp;gt;&lt;br /&gt;
  &amp;lt;color&amp;gt;black&amp;lt;/color&amp;gt;&lt;br /&gt;
  &amp;lt;size&amp;gt;200&amp;lt;/size&amp;gt;&lt;br /&gt;
  &amp;lt;uploadedFileContents&amp;gt;HYC116_NH3BH3_FREQ.LOG&amp;lt;/uploadedFileContents&amp;gt;&lt;br /&gt;
&amp;lt;/jmolApplet&amp;gt;&amp;lt;/jmol&amp;gt;&lt;br /&gt;
&lt;br /&gt;
===Association energy===&lt;br /&gt;
&lt;br /&gt;
E(BH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;) (using the optimisation with the correct symmetry) = -26.61532363 a.u. = &amp;lt;b&amp;gt;-26.61532 a.u. (5 d.p.)&amp;lt;/b&amp;gt;&lt;br /&gt;
&lt;br /&gt;
E(NH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;) = -56.55776873 a.u. = &amp;lt;b&amp;gt;-56.55777 a.u. (5 d.p.)&amp;lt;/b&amp;gt;&lt;br /&gt;
&lt;br /&gt;
E(NH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;BH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;) = -83.22468893 a.u. = &amp;lt;b&amp;gt;-83.22469 a.u. (5 d.p.)&amp;lt;/b&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
Carrying out calculations using numbers which has already been rounded up can possibly result in errors in the last digit. Hence, here the calculations were carried out using the numbers provided from the optimisations (i.e. with more decimal places than necessary); the answer was then rounded up to the desired accuracy. &lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
ΔE = E(NH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;BH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;)-[E(NH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;)+E(BH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;)]&lt;br /&gt;
&lt;br /&gt;
ΔE = -83.22468893 - (-56.55776873 + -26.61532363) = -0.05159657 a.u. &lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;ΔE = -0.05160 a.u. (5 d.p.)&amp;lt;/b&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Converting energy from a.u. to kJ/mol&#039;&#039;&#039;&lt;br /&gt;
An atomic unit for energy is Hartree, which is equal to 2625.5 kJ/mol.&lt;br /&gt;
&amp;lt;ref&amp;gt;https://cccbdb.nist.gov/hartree.asp (Accessed: 22.05.2018)&amp;lt;/ref&amp;gt;&lt;br /&gt;
 &lt;br /&gt;
&lt;br /&gt;
So ΔE in kJ/mol = -0.05159657 * 2625.5 = -135.466794535 kJ/mol&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;ΔE = -135 kJ/mol (nearest integer)&amp;lt;/b&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
The energy difference calculated above comes from the formation of the B-N dative bond. It is a relatively weak bond. According to a bond energy data sheet provided by the University of California,&amp;lt;ref&amp;gt;https://labs.chem.ucsb.edu/zakarian/armen/11---bonddissociationenergy.pdf (Accessed: 24.05.2018)&amp;lt;/ref&amp;gt;  the bond energy of the C-C bond of an ethane molecule is 368 kJ/mol. This is a fair comparison to the NH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;BH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt; molecule as the two molecules have the same structure, only with the carbon atoms on ethane swapped for Boron and Nitrogen in NH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;BH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;&lt;br /&gt;
&lt;br /&gt;
==Using a mixture of basis-sets and pseudo-potentials==&lt;br /&gt;
&lt;br /&gt;
===BBr&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;===&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;Calculation type&amp;lt;/b&amp;gt;: Optimisation&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;Calculation Method&amp;lt;/b&amp;gt;: B3LYP&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;Basis set&amp;lt;/b&amp;gt;: Boron: 6-31G(d,p) ; Br: LANL2DZ&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
Larger calculations are often sent to a web-server to run on a high-performance computer instead of a desktop. In order to experience and learn to use a web-server, the optimisation and the frequency analysis for BBr&amp;lt;sub&amp;gt;3&amp;lt;/sub were both sent and done on a server instead of the desktop. The calculation results were downloaded from the web-server once they were finished.   &lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Summary table&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
[[file:Hyc116_bbr3_opt_summarytable.png]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Items table&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;pre&amp;gt;&lt;br /&gt;
Item               Value     Threshold  Converged?&lt;br /&gt;
 Maximum Force            0.000008     0.000450     YES&lt;br /&gt;
 RMS     Force            0.000005     0.000300     YES&lt;br /&gt;
 Maximum Displacement     0.000036     0.001800     YES&lt;br /&gt;
 RMS     Displacement     0.000023     0.001200     YES&lt;br /&gt;
&amp;lt;/pre&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Frequency log file&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
[[Media:Hyc116_bbr3_freq.log]]&lt;br /&gt;
&lt;br /&gt;
Attached above is the frequency file saved onto the computer from the SCAN server portal. The frequency file was also published on the chemistry database DSpace. {{DOI|10042/202442}}&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Frequencies&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;pre&amp;gt;&lt;br /&gt;
Low frequencies ---   -0.0137   -0.0064   -0.0046    2.4315    2.4315    4.8421&lt;br /&gt;
Low frequencies ---  155.9631  155.9651  267.7052&lt;br /&gt;
&amp;lt;/pre&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;jmol of BBr&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;&#039;&#039;&#039;&lt;br /&gt;
&amp;lt;jmol&amp;gt;&amp;lt;jmolApplet&amp;gt;&lt;br /&gt;
  &amp;lt;title&amp;gt;optimised BBr3&amp;lt;/title&amp;gt;&lt;br /&gt;
  &amp;lt;color&amp;gt;black&amp;lt;/color&amp;gt;&lt;br /&gt;
  &amp;lt;size&amp;gt;200&amp;lt;/size&amp;gt;&lt;br /&gt;
  &amp;lt;uploadedFileContents&amp;gt;Hyc116_bbr3_freq.log&amp;lt;/uploadedFileContents&amp;gt;&lt;br /&gt;
&amp;lt;/jmolApplet&amp;gt;&amp;lt;/jmol&amp;gt;&lt;br /&gt;
&lt;br /&gt;
==Aromaticity==&lt;br /&gt;
&lt;br /&gt;
===Benzene===&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;Calculation type&amp;lt;/b&amp;gt;: Optimisation&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;Calculation Method&amp;lt;/b&amp;gt;: B3LYP&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;Basis set&amp;lt;/b&amp;gt;: 6-31G(d,p) &lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Summary table&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
[[file:Hyc116_c6h6_summarytable.png]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Items table&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;pre&amp;gt;&lt;br /&gt;
Item               Value     Threshold  Converged?&lt;br /&gt;
 Maximum Force            0.000193     0.000450     YES&lt;br /&gt;
 RMS     Force            0.000079     0.000300     YES&lt;br /&gt;
 Maximum Displacement     0.000830     0.001800     YES&lt;br /&gt;
 RMS     Displacement     0.000294     0.001200     YES&lt;br /&gt;
&amp;lt;/pre&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Frequency log file&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
[[Media:HYC116_C6H6_FREQ.LOG]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Frequencies&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;pre&amp;gt;&lt;br /&gt;
Low frequencies ---   -3.5606   -3.5606   -0.0089   -0.0043   -0.0043   10.0905&lt;br /&gt;
Low frequencies ---  413.9582  413.9582  621.1416&lt;br /&gt;
&amp;lt;/pre&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;jmol of C&amp;lt;sub&amp;gt;6&amp;lt;/sub&amp;gt;H&amp;lt;sub&amp;gt;6&amp;lt;/sub&amp;gt;&#039;&#039;&#039;&lt;br /&gt;
&amp;lt;jmol&amp;gt;&amp;lt;jmolApplet&amp;gt;&lt;br /&gt;
  &amp;lt;title&amp;gt;optimised Benzene&amp;lt;/title&amp;gt;&lt;br /&gt;
  &amp;lt;color&amp;gt;black&amp;lt;/color&amp;gt;&lt;br /&gt;
  &amp;lt;size&amp;gt;200&amp;lt;/size&amp;gt;&lt;br /&gt;
  &amp;lt;uploadedFileContents&amp;gt;HYC116_C6H6_FREQ.LOG&amp;lt;/uploadedFileContents&amp;gt;&lt;br /&gt;
&amp;lt;/jmolApplet&amp;gt;&amp;lt;/jmol&amp;gt;&lt;br /&gt;
&lt;br /&gt;
===Borazine===&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;Calculation type&amp;lt;/b&amp;gt;: Optimisation&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;Calculation Method&amp;lt;/b&amp;gt;: B3LYP&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;Basis set&amp;lt;/b&amp;gt;: 6-31G(d,p) &lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Summary table&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
[[file:Hyc116_borazine_summarytable.png]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Items table&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;pre&amp;gt;&lt;br /&gt;
Item               Value     Threshold  Converged?&lt;br /&gt;
 Maximum Force            0.000085     0.000450     YES&lt;br /&gt;
 RMS     Force            0.000033     0.000300     YES&lt;br /&gt;
 Maximum Displacement     0.000250     0.001800     YES&lt;br /&gt;
 RMS     Displacement     0.000074     0.001200     YES&lt;br /&gt;
&amp;lt;/pre&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Frequency log file&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
[[Media:HYC116_BORAZINE_FREQ.LOG]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Frequencies&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;pre&amp;gt;&lt;br /&gt;
Low frequencies ---  -12.6626  -12.6626   -8.9272   -0.0211   -0.0104   -0.0104&lt;br /&gt;
Low frequencies ---  289.1112  289.1112  403.8613&lt;br /&gt;
&amp;lt;/pre&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;jmol of Borazine&#039;&#039;&#039;&lt;br /&gt;
&amp;lt;jmol&amp;gt;&amp;lt;jmolApplet&amp;gt;&lt;br /&gt;
  &amp;lt;title&amp;gt;optimised Borazine&amp;lt;/title&amp;gt;&lt;br /&gt;
  &amp;lt;color&amp;gt;black&amp;lt;/color&amp;gt;&lt;br /&gt;
  &amp;lt;size&amp;gt;200&amp;lt;/size&amp;gt;&lt;br /&gt;
  &amp;lt;uploadedFileContents&amp;gt;HYC116_BORAZINE_FREQ.LOG&amp;lt;/uploadedFileContents&amp;gt;&lt;br /&gt;
&amp;lt;/jmolApplet&amp;gt;&amp;lt;/jmol&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
===Charge distribution===&lt;br /&gt;
&lt;br /&gt;
An NBO charge analysis was carried out on both the optimised benzene and borazine. Visualisations of the charge distribution are shown in the table below, with the colour range going from -1.102 to 1.102 for both molecule. This large scale was chosen as it allows direct comparison of the charge on any atoms in these two molecules and shows the relative magnitude of charges on all these atoms. Negative charges are shown in red, and positive charges are shown in green. A neutral charge is displayed in black, so the smaller a charge is (positive or negative), the darker its colour representation is. Larger charges are shown in brighter colours. The charges are also displayed on the atoms as numbers with a neutral charge being zero. Negative charges are shown as negative number and positive charges are shown as positive numbers. &lt;br /&gt;
&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot;&lt;br /&gt;
!&lt;br /&gt;
!Benzene&lt;br /&gt;
!Borazine&lt;br /&gt;
|-&lt;br /&gt;
!Visualisation of charge distribution&lt;br /&gt;
|[[File:Hyc116_benzene_charge_distribution1.png|500x500px|thumb|centre|Charge distribution of Benzene visualisation]]&lt;br /&gt;
|[[File:Hyc116_borazine_charge_distribution1.png|500x500px|thumb|centre|Charge distribution of Borazine visualisation]]&lt;br /&gt;
|-&lt;br /&gt;
!Charge &lt;br /&gt;
|Carbon: -0.239&lt;br /&gt;
&lt;br /&gt;
Hydrogen: 0.239&lt;br /&gt;
|Nitrogen: -1.102 &lt;br /&gt;
&lt;br /&gt;
Boron: 0.747&lt;br /&gt;
&lt;br /&gt;
Hydrogen (bonded to N): 0.432&lt;br /&gt;
&lt;br /&gt;
Hydrogen (bonded to B): -0.077&lt;br /&gt;
|-&lt;br /&gt;
!Discussion&lt;br /&gt;
|From the visualisation, it is shown that there is a slightly negative charge on the carbon atoms, and a positive charge of the same magnitude on the hydrogen atoms. All the carbon atoms have the same charge as they are in identical environments. The same applies to all the hydrogen atoms. This is due to the highly symmetrical structure of benzene. Since the same colour scale was used for both benzene and borazine, and the charges are much smaller in magnitude on atoms in benzene than atoms on borazine, the colours on the charge distribution visualisation is much darker. &lt;br /&gt;
|From the colours displayed on the charge distribution visualisation as well as the charge values, it is shown that nitrogen has a relatively large negative charge, while boron has a positive charge. This is due to the difference in electrogenativity between these atoms: nitrogen atoms are more electronegative than boron and tends to attract electrons towards themselves. It is worth noting that the hydrogen atoms do not all have the same charge. The hydrogen atoms bonded to boron have a slightly negative charge, and the ones bonded to nitrogen have a small positive charge. &lt;br /&gt;
&lt;br /&gt;
The fact that the same colour scale was used for both molecules comes in helpful here. It allows the charges on atoms to be compared directly. For example, just from looking at the colours, one can tell that or example, even though both carbon and nitrogen are electronegative, nitrogen is much more electronegative, which is quantitatively shown by Pauling&#039;s electronegativity scale.&amp;lt;ref&amp;gt;http://www.tutor-homework.com/Chemistry_Help/electronegativity_table/electronegativity.html (Accessed: 24.0502018&amp;lt;/ref&amp;gt;&lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
===Comparative MOs of Benzene and Borazine===&lt;br /&gt;
&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot;&lt;br /&gt;
!&lt;br /&gt;
!Benzene&lt;br /&gt;
!Borazine&lt;br /&gt;
!Comparison and Discussion&lt;br /&gt;
|-&lt;br /&gt;
!1st comparative pair&lt;br /&gt;
|[[File:Hyc116_benzene_1st_MO_pair_7.png|200x200px|centre]]&lt;br /&gt;
|[[File:Hyc116_borazine_1st_MO_pair_level9.png|200x200px|centre]]&lt;br /&gt;
|MO 9 of both benzene and borazine are comparable. They both show delocalised molecular orbital with an overall bonding character. There is a nodal plane across the molecular orbitals for both benzene and borazine. For benzene, there is contribution from all the carbon and hydrogen s orbitals. Moreover, the molecular orbitals are symmetric to their counterpart of opposite phase. That is not the case for borazine; they are less symmetric in borazine. Nitrogen atoms are more electronegative than boron atoms and pull electron density towards themselves, resulting in a larger MO. There is contribution from all the boron and nitrogen s orbitals, and three of the hydrogen s orbitals, though not all of them. &lt;br /&gt;
|-&lt;br /&gt;
!2nd comparative pair&lt;br /&gt;
|[[File:Hyc116_benzene_2nd_MO_pair_10.png|200x200px|centre]]&lt;br /&gt;
|[[File:Hyc116_borazine_2nd_MO_pair_level11.png|200x200px|centre]]&lt;br /&gt;
|&lt;br /&gt;
|-&lt;br /&gt;
!3rd comparative pair&lt;br /&gt;
|[[File:Hyc116_benzene_3rd_MO_pair_21.png|200x200px|centre]]&lt;br /&gt;
|[[File:Hyc116_borazine_3rd_MO_pair_level21.png|200x200px|centre]]&lt;br /&gt;
|&lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
===Aromaticity: some theories===&lt;br /&gt;
&lt;br /&gt;
==References==&lt;/div&gt;</summary>
		<author><name>Hyc116</name></author>
	</entry>
	<entry>
		<id>https://chemwiki.ch.ic.ac.uk/index.php?title=MO_hyc116&amp;diff=730188</id>
		<title>MO hyc116</title>
		<link rel="alternate" type="text/html" href="https://chemwiki.ch.ic.ac.uk/index.php?title=MO_hyc116&amp;diff=730188"/>
		<updated>2018-05-24T17:41:38Z</updated>

		<summary type="html">&lt;p&gt;Hyc116: &lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;==BH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;==&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;Calculation type&amp;lt;/b&amp;gt;: Optimisation&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;Calculation Method&amp;lt;/b&amp;gt;: B3LYP&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;Basis set&amp;lt;/b&amp;gt;: 6-31G(d,p) &lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Summary table&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
[[file:Hyc116_bh3_631g_opt_summarytable.png]]&lt;br /&gt;
&lt;br /&gt;
The above summary table was obtained after the 2nd optimisation of BH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt; (after the initial optimisation using the 3-21G basis set). Notice how the symmetry is incorrect and shown as Cs. This is because the symmetry was manually broken at the beginning by changing the bond length of B-H bonds. The point group was manually adjusted and the molecule was optimised again before the frequency analysis and the new summary table is attached below.&lt;br /&gt;
&lt;br /&gt;
[[file:Hyc116_bh3_correctsummarytable.png]]&lt;br /&gt;
&lt;br /&gt;
The above summary table was obtained from the optimisation after adjusting the symmetry. The point shown in this summary table is D&amp;lt;sub&amp;gt;3h&amp;lt;/sub&amp;gt;, which is the correct for BH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;. &lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Items table&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
Below is the items table taken from the optimisation with the correct point group.&lt;br /&gt;
&lt;br /&gt;
&amp;lt;pre&amp;gt;&lt;br /&gt;
Item               Value     Threshold  Converged?&lt;br /&gt;
 Maximum Force            0.000015     0.000450     YES&lt;br /&gt;
 RMS     Force            0.000010     0.000300     YES&lt;br /&gt;
 Maximum Displacement     0.000058     0.001800     YES&lt;br /&gt;
 RMS     Displacement     0.000038     0.001200     YES&lt;br /&gt;
&amp;lt;/pre&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Frequency log file&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
[[Media:HYC116 BH3 FREQ.LOG]] &lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Frequencies&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;pre&amp;gt;&lt;br /&gt;
Low frequencies ---  -10.3498   -3.4492   -1.2454   -0.0055    0.4779    3.2165&lt;br /&gt;
Low frequencies --- 1162.9519 1213.1527 1213.1554&lt;br /&gt;
&amp;lt;/pre&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;jmol of BH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;&#039;&#039;&#039;&lt;br /&gt;
&amp;lt;jmol&amp;gt;&amp;lt;jmolApplet&amp;gt;&lt;br /&gt;
  &amp;lt;title&amp;gt;optimised BH3&amp;lt;/title&amp;gt;&lt;br /&gt;
  &amp;lt;color&amp;gt;black&amp;lt;/color&amp;gt;&lt;br /&gt;
  &amp;lt;size&amp;gt;200&amp;lt;/size&amp;gt;&lt;br /&gt;
  &amp;lt;uploadedFileContents&amp;gt;HYC116_BH3_FREQ.LOG&amp;lt;/uploadedFileContents&amp;gt;&lt;br /&gt;
&amp;lt;/jmolApplet&amp;gt;&amp;lt;/jmol&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
===Vibrational spectrum===&lt;br /&gt;
&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot;&lt;br /&gt;
!wavenumber (cm&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;)&lt;br /&gt;
!Intensity (arbitrary units)&lt;br /&gt;
!symmetry&lt;br /&gt;
!IR active?&lt;br /&gt;
!type&lt;br /&gt;
|-&lt;br /&gt;
|1163&lt;br /&gt;
|93&lt;br /&gt;
|A&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;&#039; &#039;&lt;br /&gt;
|Yes&lt;br /&gt;
|Out of plane bend&lt;br /&gt;
|-&lt;br /&gt;
|1213&lt;br /&gt;
|14&lt;br /&gt;
|E&#039;&lt;br /&gt;
|Very slight&lt;br /&gt;
|Bend&lt;br /&gt;
|-&lt;br /&gt;
|1213&lt;br /&gt;
|14&lt;br /&gt;
|E&#039;&lt;br /&gt;
|Very slight&lt;br /&gt;
|Bend&lt;br /&gt;
|-&lt;br /&gt;
|2582&lt;br /&gt;
|0&lt;br /&gt;
|A&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;&#039;&lt;br /&gt;
|No&lt;br /&gt;
|Symmetric stretch&lt;br /&gt;
|-&lt;br /&gt;
|2716&lt;br /&gt;
|126&lt;br /&gt;
|E&#039;&lt;br /&gt;
|Yes&lt;br /&gt;
|Asymmetric stretch&lt;br /&gt;
|-&lt;br /&gt;
|2716&lt;br /&gt;
|126&lt;br /&gt;
|E&#039;&lt;br /&gt;
|Yes&lt;br /&gt;
|Asymmetric stretch&lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;IR spectrum&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
[[file:Hyc116_ir_bh3.png|400*600]]&lt;br /&gt;
&lt;br /&gt;
There are only three peaks on the IR spectrum of BH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;, despite that there are 6 vibrational modes for the molecule. As shown in the table above, the symmetric stretching mode with A1 symmetry at 2582 cm&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt; is not IR active; naturally, that vibrational mode doesn’t give a peak on the IR spectrum. As shown from the table, two pairs of vibrational modes, the bond angle deformation/bend at 1213 cm&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt; and the asymmetric bond stretch at 2716 cm&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;, are degenerate with the symmetry label E. This means that they have the same energy, and hence give the same wavenumber on the IR spectrum. Each pair of degenerate vibrational modes give rise to one peak. This leaves three peaks, as confirmed by the IR spectrum above.&lt;br /&gt;
&lt;br /&gt;
===Molecular orbitals of BH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;===&lt;br /&gt;
&lt;br /&gt;
[[file:hyc116_bh3_MO_diagram.png]]&lt;br /&gt;
&lt;br /&gt;
The above molecular orbital diagram was taken from Dr Patricia Hunt&#039;s &amp;lt;i&amp;gt;Lecture 4 Tutorial Problem Model Answers&amp;lt;/i&amp;gt;.&amp;lt;ref&amp;gt;P. Hunt, &amp;quot;Lecture 4 Tutorial Problem Model Answers&amp;quot;, 2 (2018)&amp;lt;/ref&amp;gt; Diagrams of the &amp;quot;real&amp;quot; MOs were obtained from Gaussian.&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
There is no significant difference between the LCAO MOs and the real ones. Features such as orbital phases are shown clearly on both the LCAO MOs and the real MOs, illustrating the bonding/anti-bonding characters of the molecular orbitals. This suggests that the the qualitative MO theory is highly accurate and useful when studying the molecular orbitals of molecules.&lt;br /&gt;
&lt;br /&gt;
==Associated energies: ammonium borane==&lt;br /&gt;
&lt;br /&gt;
===NH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;===&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;Calculation type&amp;lt;/b&amp;gt;: Optimisation&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;Calculation Method&amp;lt;/b&amp;gt;: B3LYP&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;Basis set&amp;lt;/b&amp;gt;: 6-31G(d,p) &lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Summary table&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
[[file:Hyc116_nh3_631g_summarytable.png]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Items table&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;pre&amp;gt;&lt;br /&gt;
Item               Value     Threshold  Converged?&lt;br /&gt;
 Maximum Force            0.000006     0.000450     YES&lt;br /&gt;
 RMS     Force            0.000004     0.000300     YES&lt;br /&gt;
 Maximum Displacement     0.000012     0.001800     YES&lt;br /&gt;
 RMS     Displacement     0.000008     0.001200     YES&lt;br /&gt;
&amp;lt;/pre&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Frequency log file&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
[[Media:HYC116_NH3_FREQ.LOG]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Frequencies&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;pre&amp;gt;&lt;br /&gt;
Low frequencies ---   -8.5646   -8.5588   -0.0047    0.0454    0.1784   26.4183&lt;br /&gt;
Low frequencies --- 1089.7603 1694.1865 1694.1865&lt;br /&gt;
&amp;lt;/pre&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;jmol of NH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;&#039;&#039;&#039;&lt;br /&gt;
&amp;lt;jmol&amp;gt;&amp;lt;jmolApplet&amp;gt;&lt;br /&gt;
  &amp;lt;title&amp;gt;optimised NH3&amp;lt;/title&amp;gt;&lt;br /&gt;
  &amp;lt;color&amp;gt;black&amp;lt;/color&amp;gt;&lt;br /&gt;
  &amp;lt;size&amp;gt;200&amp;lt;/size&amp;gt;&lt;br /&gt;
  &amp;lt;uploadedFileContents&amp;gt;HYC116_NH3_FREQ.LOG&amp;lt;/uploadedFileContents&amp;gt;&lt;br /&gt;
&amp;lt;/jmolApplet&amp;gt;&amp;lt;/jmol&amp;gt;&lt;br /&gt;
&lt;br /&gt;
===NH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;BH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;===&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;Calculation type&amp;lt;/b&amp;gt;: Optimisation&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;Calculation Method&amp;lt;/b&amp;gt;: B3LYP&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;Basis set&amp;lt;/b&amp;gt;: 6-31G(d,p) &lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Summary table&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
[[file:Hyc116_nh3bh3_631g_summarytable.png]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Items table&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;pre&amp;gt;&lt;br /&gt;
Item               Value     Threshold  Converged?&lt;br /&gt;
 Maximum Force            0.000123     0.000450     YES&lt;br /&gt;
 RMS     Force            0.000058     0.000300     YES&lt;br /&gt;
 Maximum Displacement     0.000515     0.001800     YES&lt;br /&gt;
 RMS     Displacement     0.000296     0.001200     YES&lt;br /&gt;
&amp;lt;/pre&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Frequency log file&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
[[Media:HYC116_NH3BH3_FREQ.LOG]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Frequencies&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;pre&amp;gt;&lt;br /&gt;
Low frequencies ---   -0.0014   -0.0011   -0.0006    6.9624   20.4518   43.5542&lt;br /&gt;
Low frequencies ---  266.4530  632.2458  639.0504&lt;br /&gt;
&amp;lt;/pre&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;jmol of NH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;BH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;&#039;&#039;&#039;&lt;br /&gt;
&amp;lt;jmol&amp;gt;&amp;lt;jmolApplet&amp;gt;&lt;br /&gt;
  &amp;lt;title&amp;gt;optimised NH3BH3&amp;lt;/title&amp;gt;&lt;br /&gt;
  &amp;lt;color&amp;gt;black&amp;lt;/color&amp;gt;&lt;br /&gt;
  &amp;lt;size&amp;gt;200&amp;lt;/size&amp;gt;&lt;br /&gt;
  &amp;lt;uploadedFileContents&amp;gt;HYC116_NH3BH3_FREQ.LOG&amp;lt;/uploadedFileContents&amp;gt;&lt;br /&gt;
&amp;lt;/jmolApplet&amp;gt;&amp;lt;/jmol&amp;gt;&lt;br /&gt;
&lt;br /&gt;
===Association energy===&lt;br /&gt;
&lt;br /&gt;
E(BH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;) (using the optimisation with the correct symmetry) = -26.61532363 a.u. = &amp;lt;b&amp;gt;-26.61532 a.u. (5 d.p.)&amp;lt;/b&amp;gt;&lt;br /&gt;
&lt;br /&gt;
E(NH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;) = -56.55776873 a.u. = &amp;lt;b&amp;gt;-56.55777 a.u. (5 d.p.)&amp;lt;/b&amp;gt;&lt;br /&gt;
&lt;br /&gt;
E(NH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;BH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;) = -83.22468893 a.u. = &amp;lt;b&amp;gt;-83.22469 a.u. (5 d.p.)&amp;lt;/b&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
Carrying out calculations using numbers which has already been rounded up can possibly result in errors in the last digit. Hence, here the calculations were carried out using the numbers provided from the optimisations (i.e. with more decimal places than necessary); the answer was then rounded up to the desired accuracy. &lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
ΔE = E(NH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;BH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;)-[E(NH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;)+E(BH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;)]&lt;br /&gt;
&lt;br /&gt;
ΔE = -83.22468893 - (-56.55776873 + -26.61532363) = -0.05159657 a.u. &lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;ΔE = -0.05160 a.u. (5 d.p.)&amp;lt;/b&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Converting energy from a.u. to kJ/mol&#039;&#039;&#039;&lt;br /&gt;
An atomic unit for energy is Hartree, which is equal to 2625.5 kJ/mol.&lt;br /&gt;
&amp;lt;ref&amp;gt;https://cccbdb.nist.gov/hartree.asp (Accessed: 22.05.2018)&amp;lt;/ref&amp;gt;&lt;br /&gt;
 &lt;br /&gt;
&lt;br /&gt;
So ΔE in kJ/mol = -0.05159657 * 2625.5 = -135.466794535 kJ/mol&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;ΔE = -135 kJ/mol (nearest integer)&amp;lt;/b&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
The energy difference calculated above comes from the formation of the B-N dative bond. It is a relatively weak bond. According to a bond energy data sheet provided by the University of California,&amp;lt;ref&amp;gt;https://labs.chem.ucsb.edu/zakarian/armen/11---bonddissociationenergy.pdf (Accessed: 24.05.2018)&amp;lt;/ref&amp;gt;  the bond energy of the C-C bond of an ethane molecule is 368 kJ/mol. This is a fair comparison to the NH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;BH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt; molecule as the two molecules have the same structure, only with the carbon atoms on ethane swapped for Boron and Nitrogen in NH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;BH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;&lt;br /&gt;
&lt;br /&gt;
==Using a mixture of basis-sets and pseudo-potentials==&lt;br /&gt;
&lt;br /&gt;
===BBr&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;===&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;Calculation type&amp;lt;/b&amp;gt;: Optimisation&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;Calculation Method&amp;lt;/b&amp;gt;: B3LYP&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;Basis set&amp;lt;/b&amp;gt;: Boron: 6-31G(d,p) ; Br: LANL2DZ&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
Larger calculations are often sent to a web-server to run on a high-performance computer instead of a desktop. In order to experience and learn to use a web-server, the optimisation and the frequency analysis for BBr&amp;lt;sub&amp;gt;3&amp;lt;/sub were both sent and done on a server instead of the desktop. The calculation results were downloaded from the web-server once they were finished.   &lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Summary table&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
[[file:Hyc116_bbr3_opt_summarytable.png]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Items table&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;pre&amp;gt;&lt;br /&gt;
Item               Value     Threshold  Converged?&lt;br /&gt;
 Maximum Force            0.000008     0.000450     YES&lt;br /&gt;
 RMS     Force            0.000005     0.000300     YES&lt;br /&gt;
 Maximum Displacement     0.000036     0.001800     YES&lt;br /&gt;
 RMS     Displacement     0.000023     0.001200     YES&lt;br /&gt;
&amp;lt;/pre&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Frequency log file&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
[[Media:Hyc116_bbr3_freq.log]]&lt;br /&gt;
&lt;br /&gt;
Attached above is the frequency file saved onto the computer from the SCAN server portal. The frequency file was also published on the chemistry database DSpace. {{DOI|10042/202442}}&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Frequencies&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;pre&amp;gt;&lt;br /&gt;
Low frequencies ---   -0.0137   -0.0064   -0.0046    2.4315    2.4315    4.8421&lt;br /&gt;
Low frequencies ---  155.9631  155.9651  267.7052&lt;br /&gt;
&amp;lt;/pre&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;jmol of BBr&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;&#039;&#039;&#039;&lt;br /&gt;
&amp;lt;jmol&amp;gt;&amp;lt;jmolApplet&amp;gt;&lt;br /&gt;
  &amp;lt;title&amp;gt;optimised BBr3&amp;lt;/title&amp;gt;&lt;br /&gt;
  &amp;lt;color&amp;gt;black&amp;lt;/color&amp;gt;&lt;br /&gt;
  &amp;lt;size&amp;gt;200&amp;lt;/size&amp;gt;&lt;br /&gt;
  &amp;lt;uploadedFileContents&amp;gt;Hyc116_bbr3_freq.log&amp;lt;/uploadedFileContents&amp;gt;&lt;br /&gt;
&amp;lt;/jmolApplet&amp;gt;&amp;lt;/jmol&amp;gt;&lt;br /&gt;
&lt;br /&gt;
==Aromaticity==&lt;br /&gt;
&lt;br /&gt;
===Benzene===&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;Calculation type&amp;lt;/b&amp;gt;: Optimisation&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;Calculation Method&amp;lt;/b&amp;gt;: B3LYP&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;Basis set&amp;lt;/b&amp;gt;: 6-31G(d,p) &lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Summary table&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
[[file:Hyc116_c6h6_summarytable.png]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Items table&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;pre&amp;gt;&lt;br /&gt;
Item               Value     Threshold  Converged?&lt;br /&gt;
 Maximum Force            0.000193     0.000450     YES&lt;br /&gt;
 RMS     Force            0.000079     0.000300     YES&lt;br /&gt;
 Maximum Displacement     0.000830     0.001800     YES&lt;br /&gt;
 RMS     Displacement     0.000294     0.001200     YES&lt;br /&gt;
&amp;lt;/pre&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Frequency log file&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
[[Media:HYC116_C6H6_FREQ.LOG]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Frequencies&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;pre&amp;gt;&lt;br /&gt;
Low frequencies ---   -3.5606   -3.5606   -0.0089   -0.0043   -0.0043   10.0905&lt;br /&gt;
Low frequencies ---  413.9582  413.9582  621.1416&lt;br /&gt;
&amp;lt;/pre&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;jmol of C&amp;lt;sub&amp;gt;6&amp;lt;/sub&amp;gt;H&amp;lt;sub&amp;gt;6&amp;lt;/sub&amp;gt;&#039;&#039;&#039;&lt;br /&gt;
&amp;lt;jmol&amp;gt;&amp;lt;jmolApplet&amp;gt;&lt;br /&gt;
  &amp;lt;title&amp;gt;optimised Benzene&amp;lt;/title&amp;gt;&lt;br /&gt;
  &amp;lt;color&amp;gt;black&amp;lt;/color&amp;gt;&lt;br /&gt;
  &amp;lt;size&amp;gt;200&amp;lt;/size&amp;gt;&lt;br /&gt;
  &amp;lt;uploadedFileContents&amp;gt;HYC116_C6H6_FREQ.LOG&amp;lt;/uploadedFileContents&amp;gt;&lt;br /&gt;
&amp;lt;/jmolApplet&amp;gt;&amp;lt;/jmol&amp;gt;&lt;br /&gt;
&lt;br /&gt;
===Borazine===&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;Calculation type&amp;lt;/b&amp;gt;: Optimisation&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;Calculation Method&amp;lt;/b&amp;gt;: B3LYP&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;Basis set&amp;lt;/b&amp;gt;: 6-31G(d,p) &lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Summary table&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
[[file:Hyc116_borazine_summarytable.png]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Items table&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;pre&amp;gt;&lt;br /&gt;
Item               Value     Threshold  Converged?&lt;br /&gt;
 Maximum Force            0.000085     0.000450     YES&lt;br /&gt;
 RMS     Force            0.000033     0.000300     YES&lt;br /&gt;
 Maximum Displacement     0.000250     0.001800     YES&lt;br /&gt;
 RMS     Displacement     0.000074     0.001200     YES&lt;br /&gt;
&amp;lt;/pre&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Frequency log file&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
[[Media:HYC116_BORAZINE_FREQ.LOG]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Frequencies&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;pre&amp;gt;&lt;br /&gt;
Low frequencies ---  -12.6626  -12.6626   -8.9272   -0.0211   -0.0104   -0.0104&lt;br /&gt;
Low frequencies ---  289.1112  289.1112  403.8613&lt;br /&gt;
&amp;lt;/pre&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;jmol of Borazine&#039;&#039;&#039;&lt;br /&gt;
&amp;lt;jmol&amp;gt;&amp;lt;jmolApplet&amp;gt;&lt;br /&gt;
  &amp;lt;title&amp;gt;optimised Borazine&amp;lt;/title&amp;gt;&lt;br /&gt;
  &amp;lt;color&amp;gt;black&amp;lt;/color&amp;gt;&lt;br /&gt;
  &amp;lt;size&amp;gt;200&amp;lt;/size&amp;gt;&lt;br /&gt;
  &amp;lt;uploadedFileContents&amp;gt;HYC116_BORAZINE_FREQ.LOG&amp;lt;/uploadedFileContents&amp;gt;&lt;br /&gt;
&amp;lt;/jmolApplet&amp;gt;&amp;lt;/jmol&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
===Charge distribution===&lt;br /&gt;
&lt;br /&gt;
An NBO charge analysis was carried out on both the optimised benzene and borazine. Visualisations of the charge distribution are shown in the table below, with the colour range going from -1.102 to 1.102 for both molecule. This large scale was chosen as it allows direct comparison of the charge on any atoms in these two molecules and shows the relative magnitude of charges on all these atoms. Negative charges are shown in red, and positive charges are shown in green. A neutral charge is displayed in black, so the smaller a charge is (positive or negative), the darker its colour representation is. Larger charges are shown in brighter colours. The charges are also displayed on the atoms as numbers with a neutral charge being zero. Negative charges are shown as negative number and positive charges are shown as positive numbers. &lt;br /&gt;
&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot;&lt;br /&gt;
!&lt;br /&gt;
!Benzene&lt;br /&gt;
!Borazine&lt;br /&gt;
|-&lt;br /&gt;
!Visualisation of charge distribution&lt;br /&gt;
|[[File:Hyc116_benzene_charge_distribution1.png|500x500px|thumb|centre|Charge distribution of Benzene visualisation]]&lt;br /&gt;
|[[File:Hyc116_borazine_charge_distribution1.png|500x500px|thumb|centre|Charge distribution of Borazine visualisation]]&lt;br /&gt;
|-&lt;br /&gt;
!Charge &lt;br /&gt;
|Carbon: -0.239&lt;br /&gt;
&lt;br /&gt;
Hydrogen: 0.239&lt;br /&gt;
|Nitrogen: -1.102 &lt;br /&gt;
&lt;br /&gt;
Boron: 0.747&lt;br /&gt;
&lt;br /&gt;
Hydrogen (bonded to N): 0.432&lt;br /&gt;
&lt;br /&gt;
Hydrogen (bonded to B): -0.077&lt;br /&gt;
|-&lt;br /&gt;
!Discussion&lt;br /&gt;
|From the visualisation, it is shown that there is a slightly negative charge on the carbon atoms, and a positive charge of the same magnitude on the hydrogen atoms. All the carbon atoms have the same charge as they are in identical environments. The same applies to all the hydrogen atoms. This is due to the highly symmetrical structure of benzene. Since the same colour scale was used for both benzene and borazine, and the charges are much smaller in magnitude on atoms in benzene than atoms on borazine, the colours on the charge distribution visualisation is much darker. &lt;br /&gt;
|From the colours displayed on the charge distribution visualisation as well as the charge values, it is shown that nitrogen has a relatively large negative charge, while boron has a positive charge. This is due to the difference in electrogenativity between these atoms: nitrogen atoms are more electronegative than boron and tends to attract electrons towards themselves. It is worth noting that the hydrogen atoms do not all have the same charge. The hydrogen atoms bonded to boron have a slightly negative charge, and the ones bonded to nitrogen have a small positive charge. &lt;br /&gt;
&lt;br /&gt;
The fact that the same colour scale was used for both molecules comes in helpful here. It allows the charges on atoms to be compared directly. For example, just from looking at the colours, one can tell that or example, even though both carbon and nitrogen are electronegative, nitrogen is much more electronegative, which is quantitatively shown by Pauling&#039;s electronegativity scale.&amp;lt;ref&amp;gt;http://www.tutor-homework.com/Chemistry_Help/electronegativity_table/electronegativity.html (Accessed: 24.0502018&amp;lt;/ref&amp;gt;&lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
===Comparative MOs of Benzene and Borazine===&lt;br /&gt;
&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot;&lt;br /&gt;
!&lt;br /&gt;
!Benzene&lt;br /&gt;
!Borazine&lt;br /&gt;
!Comparison and Discussion&lt;br /&gt;
|-&lt;br /&gt;
!1st comparative pair&lt;br /&gt;
|[[File:Hyc116_benzene_1st_MO_pair_7.png|200x200px|centre]]&lt;br /&gt;
|[[File:Hyc116_borazine_1st_MO_pair_level9.png|200x200px|centre]]&lt;br /&gt;
|MO 9 of both benzene and borazine are comparable. They both show delocalised molecular orbital with an overall bonding character. There is a nodal plane across the molecular orbitals for both benzene and borazine. For benzene, there is contribution from all the carbon and hydrogen s orbitals. Moreover, the molecular orbitals are symmetric to their counterpart of opposite phase. That is not the case for borazine; they are less symmetric in borazine. Nitrogen atoms are more electronegative than boron atoms and pull electron density towards themselves, resulting in a larger MO. There is contribution from all the boron and nitrogen s orbitals, and three of the hydrogen s orbitals, though not all of them. &lt;br /&gt;
|-&lt;br /&gt;
!2nd comparative pair&lt;br /&gt;
|[[File:Hyc116_benzene_2nd_MO_pair_10.png|200x200px|centre]]&lt;br /&gt;
|[[File:Hyc116_borazine_2nd_MO_pair_level11.png|200x200px|centre]]&lt;br /&gt;
|&lt;br /&gt;
|-&lt;br /&gt;
!3rd comparative pair&lt;br /&gt;
|[[File:Hyc116_benzene_3rd_MO_pair_21.png|200x200px|centre]]&lt;br /&gt;
|[[File:Hyc116_borazine_3rd_MO_pair_level21.png|200x200px|centre]]&lt;br /&gt;
|&lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
===Aromaticity: some theories===&lt;br /&gt;
&lt;br /&gt;
==References==&lt;br /&gt;
{{reflist}}&lt;/div&gt;</summary>
		<author><name>Hyc116</name></author>
	</entry>
	<entry>
		<id>https://chemwiki.ch.ic.ac.uk/index.php?title=MO_hyc116&amp;diff=730180</id>
		<title>MO hyc116</title>
		<link rel="alternate" type="text/html" href="https://chemwiki.ch.ic.ac.uk/index.php?title=MO_hyc116&amp;diff=730180"/>
		<updated>2018-05-24T17:39:06Z</updated>

		<summary type="html">&lt;p&gt;Hyc116: /* References */&lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;==BH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;==&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;Calculation type&amp;lt;/b&amp;gt;: Optimisation&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;Calculation Method&amp;lt;/b&amp;gt;: B3LYP&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;Basis set&amp;lt;/b&amp;gt;: 6-31G(d,p) &lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Summary table&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
[[file:Hyc116_bh3_631g_opt_summarytable.png]]&lt;br /&gt;
&lt;br /&gt;
The above summary table was obtained after the 2nd optimisation of BH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt; (after the initial optimisation using the 3-21G basis set). Notice how the symmetry is incorrect and shown as Cs. This is because the symmetry was manually broken at the beginning by changing the bond length of B-H bonds. The point group was manually adjusted and the molecule was optimised again before the frequency analysis and the new summary table is attached below.&lt;br /&gt;
&lt;br /&gt;
[[file:Hyc116_bh3_correctsummarytable.png]]&lt;br /&gt;
&lt;br /&gt;
The above summary table was obtained from the optimisation after adjusting the symmetry. The point shown in this summary table is D&amp;lt;sub&amp;gt;3h&amp;lt;/sub&amp;gt;, which is the correct for BH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;. &lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Items table&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
Below is the items table taken from the optimisation with the correct point group.&lt;br /&gt;
&lt;br /&gt;
&amp;lt;pre&amp;gt;&lt;br /&gt;
Item               Value     Threshold  Converged?&lt;br /&gt;
 Maximum Force            0.000015     0.000450     YES&lt;br /&gt;
 RMS     Force            0.000010     0.000300     YES&lt;br /&gt;
 Maximum Displacement     0.000058     0.001800     YES&lt;br /&gt;
 RMS     Displacement     0.000038     0.001200     YES&lt;br /&gt;
&amp;lt;/pre&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Frequency log file&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
[[Media:HYC116 BH3 FREQ.LOG]] &lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Frequencies&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;pre&amp;gt;&lt;br /&gt;
Low frequencies ---  -10.3498   -3.4492   -1.2454   -0.0055    0.4779    3.2165&lt;br /&gt;
Low frequencies --- 1162.9519 1213.1527 1213.1554&lt;br /&gt;
&amp;lt;/pre&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;jmol of BH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;&#039;&#039;&#039;&lt;br /&gt;
&amp;lt;jmol&amp;gt;&amp;lt;jmolApplet&amp;gt;&lt;br /&gt;
  &amp;lt;title&amp;gt;optimised BH3&amp;lt;/title&amp;gt;&lt;br /&gt;
  &amp;lt;color&amp;gt;black&amp;lt;/color&amp;gt;&lt;br /&gt;
  &amp;lt;size&amp;gt;200&amp;lt;/size&amp;gt;&lt;br /&gt;
  &amp;lt;uploadedFileContents&amp;gt;HYC116_BH3_FREQ.LOG&amp;lt;/uploadedFileContents&amp;gt;&lt;br /&gt;
&amp;lt;/jmolApplet&amp;gt;&amp;lt;/jmol&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
===Vibrational spectrum===&lt;br /&gt;
&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot;&lt;br /&gt;
!wavenumber (cm&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;)&lt;br /&gt;
!Intensity (arbitrary units)&lt;br /&gt;
!symmetry&lt;br /&gt;
!IR active?&lt;br /&gt;
!type&lt;br /&gt;
|-&lt;br /&gt;
|1163&lt;br /&gt;
|93&lt;br /&gt;
|A&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;&#039; &#039;&lt;br /&gt;
|Yes&lt;br /&gt;
|Out of plane bend&lt;br /&gt;
|-&lt;br /&gt;
|1213&lt;br /&gt;
|14&lt;br /&gt;
|E&#039;&lt;br /&gt;
|Very slight&lt;br /&gt;
|Bend&lt;br /&gt;
|-&lt;br /&gt;
|1213&lt;br /&gt;
|14&lt;br /&gt;
|E&#039;&lt;br /&gt;
|Very slight&lt;br /&gt;
|Bend&lt;br /&gt;
|-&lt;br /&gt;
|2582&lt;br /&gt;
|0&lt;br /&gt;
|A&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;&#039;&lt;br /&gt;
|No&lt;br /&gt;
|Symmetric stretch&lt;br /&gt;
|-&lt;br /&gt;
|2716&lt;br /&gt;
|126&lt;br /&gt;
|E&#039;&lt;br /&gt;
|Yes&lt;br /&gt;
|Asymmetric stretch&lt;br /&gt;
|-&lt;br /&gt;
|2716&lt;br /&gt;
|126&lt;br /&gt;
|E&#039;&lt;br /&gt;
|Yes&lt;br /&gt;
|Asymmetric stretch&lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;IR spectrum&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
[[file:Hyc116_ir_bh3.png|400*600]]&lt;br /&gt;
&lt;br /&gt;
There are only three peaks on the IR spectrum of BH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;, despite that there are 6 vibrational modes for the molecule. As shown in the table above, the symmetric stretching mode with A1 symmetry at 2582 cm&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt; is not IR active; naturally, that vibrational mode doesn’t give a peak on the IR spectrum. As shown from the table, two pairs of vibrational modes, the bond angle deformation/bend at 1213 cm&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt; and the asymmetric bond stretch at 2716 cm&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;, are degenerate with the symmetry label E. This means that they have the same energy, and hence give the same wavenumber on the IR spectrum. Each pair of degenerate vibrational modes give rise to one peak. This leaves three peaks, as confirmed by the IR spectrum above.&lt;br /&gt;
&lt;br /&gt;
===Molecular orbitals of BH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;===&lt;br /&gt;
&lt;br /&gt;
[[file:hyc116_bh3_MO_diagram.png]]&lt;br /&gt;
&lt;br /&gt;
The above molecular orbital diagram was taken from Dr Patricia Hunt&#039;s &amp;lt;i&amp;gt;Lecture 4 Tutorial Problem Model Answers&amp;lt;/i&amp;gt;. . Diagrams of the &amp;quot;real&amp;quot; MOs were obtained from Gaussian.&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
There is no significant difference between the LCAO MOs and the real ones. Features such as orbital phases are shown clearly on both the LCAO MOs and the real MOs, illustrating the bonding/anti-bonding characters of the molecular orbitals. This suggests that the the qualitative MO theory is highly accurate and useful when studying the molecular orbitals of molecules.&lt;br /&gt;
&lt;br /&gt;
==Associated energies: ammonium borane==&lt;br /&gt;
&lt;br /&gt;
===NH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;===&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;Calculation type&amp;lt;/b&amp;gt;: Optimisation&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;Calculation Method&amp;lt;/b&amp;gt;: B3LYP&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;Basis set&amp;lt;/b&amp;gt;: 6-31G(d,p) &lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Summary table&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
[[file:Hyc116_nh3_631g_summarytable.png]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Items table&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;pre&amp;gt;&lt;br /&gt;
Item               Value     Threshold  Converged?&lt;br /&gt;
 Maximum Force            0.000006     0.000450     YES&lt;br /&gt;
 RMS     Force            0.000004     0.000300     YES&lt;br /&gt;
 Maximum Displacement     0.000012     0.001800     YES&lt;br /&gt;
 RMS     Displacement     0.000008     0.001200     YES&lt;br /&gt;
&amp;lt;/pre&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Frequency log file&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
[[Media:HYC116_NH3_FREQ.LOG]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Frequencies&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;pre&amp;gt;&lt;br /&gt;
Low frequencies ---   -8.5646   -8.5588   -0.0047    0.0454    0.1784   26.4183&lt;br /&gt;
Low frequencies --- 1089.7603 1694.1865 1694.1865&lt;br /&gt;
&amp;lt;/pre&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;jmol of NH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;&#039;&#039;&#039;&lt;br /&gt;
&amp;lt;jmol&amp;gt;&amp;lt;jmolApplet&amp;gt;&lt;br /&gt;
  &amp;lt;title&amp;gt;optimised NH3&amp;lt;/title&amp;gt;&lt;br /&gt;
  &amp;lt;color&amp;gt;black&amp;lt;/color&amp;gt;&lt;br /&gt;
  &amp;lt;size&amp;gt;200&amp;lt;/size&amp;gt;&lt;br /&gt;
  &amp;lt;uploadedFileContents&amp;gt;HYC116_NH3_FREQ.LOG&amp;lt;/uploadedFileContents&amp;gt;&lt;br /&gt;
&amp;lt;/jmolApplet&amp;gt;&amp;lt;/jmol&amp;gt;&lt;br /&gt;
&lt;br /&gt;
===NH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;BH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;===&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;Calculation type&amp;lt;/b&amp;gt;: Optimisation&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;Calculation Method&amp;lt;/b&amp;gt;: B3LYP&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;Basis set&amp;lt;/b&amp;gt;: 6-31G(d,p) &lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Summary table&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
[[file:Hyc116_nh3bh3_631g_summarytable.png]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Items table&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;pre&amp;gt;&lt;br /&gt;
Item               Value     Threshold  Converged?&lt;br /&gt;
 Maximum Force            0.000123     0.000450     YES&lt;br /&gt;
 RMS     Force            0.000058     0.000300     YES&lt;br /&gt;
 Maximum Displacement     0.000515     0.001800     YES&lt;br /&gt;
 RMS     Displacement     0.000296     0.001200     YES&lt;br /&gt;
&amp;lt;/pre&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Frequency log file&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
[[Media:HYC116_NH3BH3_FREQ.LOG]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Frequencies&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;pre&amp;gt;&lt;br /&gt;
Low frequencies ---   -0.0014   -0.0011   -0.0006    6.9624   20.4518   43.5542&lt;br /&gt;
Low frequencies ---  266.4530  632.2458  639.0504&lt;br /&gt;
&amp;lt;/pre&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;jmol of NH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;BH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;&#039;&#039;&#039;&lt;br /&gt;
&amp;lt;jmol&amp;gt;&amp;lt;jmolApplet&amp;gt;&lt;br /&gt;
  &amp;lt;title&amp;gt;optimised NH3BH3&amp;lt;/title&amp;gt;&lt;br /&gt;
  &amp;lt;color&amp;gt;black&amp;lt;/color&amp;gt;&lt;br /&gt;
  &amp;lt;size&amp;gt;200&amp;lt;/size&amp;gt;&lt;br /&gt;
  &amp;lt;uploadedFileContents&amp;gt;HYC116_NH3BH3_FREQ.LOG&amp;lt;/uploadedFileContents&amp;gt;&lt;br /&gt;
&amp;lt;/jmolApplet&amp;gt;&amp;lt;/jmol&amp;gt;&lt;br /&gt;
&lt;br /&gt;
===Association energy===&lt;br /&gt;
&lt;br /&gt;
E(BH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;) (using the optimisation with the correct symmetry) = -26.61532363 a.u. = &amp;lt;b&amp;gt;-26.61532 a.u. (5 d.p.)&amp;lt;/b&amp;gt;&lt;br /&gt;
&lt;br /&gt;
E(NH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;) = -56.55776873 a.u. = &amp;lt;b&amp;gt;-56.55777 a.u. (5 d.p.)&amp;lt;/b&amp;gt;&lt;br /&gt;
&lt;br /&gt;
E(NH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;BH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;) = -83.22468893 a.u. = &amp;lt;b&amp;gt;-83.22469 a.u. (5 d.p.)&amp;lt;/b&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
Carrying out calculations using numbers which has already been rounded up can possibly result in errors in the last digit. Hence, here the calculations were carried out using the numbers provided from the optimisations (i.e. with more decimal places than necessary); the answer was then rounded up to the desired accuracy. &lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
ΔE = E(NH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;BH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;)-[E(NH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;)+E(BH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;)]&lt;br /&gt;
&lt;br /&gt;
ΔE = -83.22468893 - (-56.55776873 + -26.61532363) = -0.05159657 a.u. &lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;ΔE = -0.05160 a.u. (5 d.p.)&amp;lt;/b&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Converting energy from a.u. to kJ/mol&#039;&#039;&#039;&lt;br /&gt;
An atomic unit for energy is Hartree, which is equal to 2625.5 kJ/mol. &lt;br /&gt;
&lt;br /&gt;
So ΔE in kJ/mol = -0.05159657 * 2625.5 = -135.466794535 kJ/mol&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;ΔE = -135 kJ/mol (nearest integer)&amp;lt;/b&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
The energy difference calculated above comes from the formation of the B-N dative bond. It is a relatively weak bond. According to a bond energy data sheet provided by the University of California,  the bond energy of the C-C bond of an ethane molecule is 368 kJ/mol. This is a fair comparison to the NH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;BH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt; molecule as the two molecules have the same structure, only with the carbon atoms on ethane swapped for Boron and Nitrogen in NH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;BH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;&lt;br /&gt;
&lt;br /&gt;
==Using a mixture of basis-sets and pseudo-potentials==&lt;br /&gt;
&lt;br /&gt;
===BBr&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;===&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;Calculation type&amp;lt;/b&amp;gt;: Optimisation&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;Calculation Method&amp;lt;/b&amp;gt;: B3LYP&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;Basis set&amp;lt;/b&amp;gt;: Boron: 6-31G(d,p) ; Br: LANL2DZ&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
Larger calculations are often sent to a web-server to run on a high-performance computer instead of a desktop. In order to experience and learn to use a web-server, the optimisation and the frequency analysis for BBr&amp;lt;sub&amp;gt;3&amp;lt;/sub were both sent and done on a server instead of the desktop. The calculation results were downloaded from the web-server once they were finished.   &lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Summary table&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
[[file:Hyc116_bbr3_opt_summarytable.png]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Items table&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;pre&amp;gt;&lt;br /&gt;
Item               Value     Threshold  Converged?&lt;br /&gt;
 Maximum Force            0.000008     0.000450     YES&lt;br /&gt;
 RMS     Force            0.000005     0.000300     YES&lt;br /&gt;
 Maximum Displacement     0.000036     0.001800     YES&lt;br /&gt;
 RMS     Displacement     0.000023     0.001200     YES&lt;br /&gt;
&amp;lt;/pre&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Frequency log file&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
[[Media:Hyc116_bbr3_freq.log]]&lt;br /&gt;
&lt;br /&gt;
Attached above is the frequency file saved onto the computer from the SCAN server portal. The frequency file was also published on the chemistry database DSpace. {{DOI|10042/202442}}&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Frequencies&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;pre&amp;gt;&lt;br /&gt;
Low frequencies ---   -0.0137   -0.0064   -0.0046    2.4315    2.4315    4.8421&lt;br /&gt;
Low frequencies ---  155.9631  155.9651  267.7052&lt;br /&gt;
&amp;lt;/pre&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;jmol of BBr&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;&#039;&#039;&#039;&lt;br /&gt;
&amp;lt;jmol&amp;gt;&amp;lt;jmolApplet&amp;gt;&lt;br /&gt;
  &amp;lt;title&amp;gt;optimised BBr3&amp;lt;/title&amp;gt;&lt;br /&gt;
  &amp;lt;color&amp;gt;black&amp;lt;/color&amp;gt;&lt;br /&gt;
  &amp;lt;size&amp;gt;200&amp;lt;/size&amp;gt;&lt;br /&gt;
  &amp;lt;uploadedFileContents&amp;gt;Hyc116_bbr3_freq.log&amp;lt;/uploadedFileContents&amp;gt;&lt;br /&gt;
&amp;lt;/jmolApplet&amp;gt;&amp;lt;/jmol&amp;gt;&lt;br /&gt;
&lt;br /&gt;
==Aromaticity==&lt;br /&gt;
&lt;br /&gt;
===Benzene===&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;Calculation type&amp;lt;/b&amp;gt;: Optimisation&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;Calculation Method&amp;lt;/b&amp;gt;: B3LYP&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;Basis set&amp;lt;/b&amp;gt;: 6-31G(d,p) &lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Summary table&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
[[file:Hyc116_c6h6_summarytable.png]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Items table&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;pre&amp;gt;&lt;br /&gt;
Item               Value     Threshold  Converged?&lt;br /&gt;
 Maximum Force            0.000193     0.000450     YES&lt;br /&gt;
 RMS     Force            0.000079     0.000300     YES&lt;br /&gt;
 Maximum Displacement     0.000830     0.001800     YES&lt;br /&gt;
 RMS     Displacement     0.000294     0.001200     YES&lt;br /&gt;
&amp;lt;/pre&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Frequency log file&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
[[Media:HYC116_C6H6_FREQ.LOG]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Frequencies&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;pre&amp;gt;&lt;br /&gt;
Low frequencies ---   -3.5606   -3.5606   -0.0089   -0.0043   -0.0043   10.0905&lt;br /&gt;
Low frequencies ---  413.9582  413.9582  621.1416&lt;br /&gt;
&amp;lt;/pre&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;jmol of C&amp;lt;sub&amp;gt;6&amp;lt;/sub&amp;gt;H&amp;lt;sub&amp;gt;6&amp;lt;/sub&amp;gt;&#039;&#039;&#039;&lt;br /&gt;
&amp;lt;jmol&amp;gt;&amp;lt;jmolApplet&amp;gt;&lt;br /&gt;
  &amp;lt;title&amp;gt;optimised Benzene&amp;lt;/title&amp;gt;&lt;br /&gt;
  &amp;lt;color&amp;gt;black&amp;lt;/color&amp;gt;&lt;br /&gt;
  &amp;lt;size&amp;gt;200&amp;lt;/size&amp;gt;&lt;br /&gt;
  &amp;lt;uploadedFileContents&amp;gt;HYC116_C6H6_FREQ.LOG&amp;lt;/uploadedFileContents&amp;gt;&lt;br /&gt;
&amp;lt;/jmolApplet&amp;gt;&amp;lt;/jmol&amp;gt;&lt;br /&gt;
&lt;br /&gt;
===Borazine===&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;Calculation type&amp;lt;/b&amp;gt;: Optimisation&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;Calculation Method&amp;lt;/b&amp;gt;: B3LYP&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;Basis set&amp;lt;/b&amp;gt;: 6-31G(d,p) &lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Summary table&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
[[file:Hyc116_borazine_summarytable.png]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Items table&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;pre&amp;gt;&lt;br /&gt;
Item               Value     Threshold  Converged?&lt;br /&gt;
 Maximum Force            0.000085     0.000450     YES&lt;br /&gt;
 RMS     Force            0.000033     0.000300     YES&lt;br /&gt;
 Maximum Displacement     0.000250     0.001800     YES&lt;br /&gt;
 RMS     Displacement     0.000074     0.001200     YES&lt;br /&gt;
&amp;lt;/pre&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Frequency log file&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
[[Media:HYC116_BORAZINE_FREQ.LOG]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Frequencies&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;pre&amp;gt;&lt;br /&gt;
Low frequencies ---  -12.6626  -12.6626   -8.9272   -0.0211   -0.0104   -0.0104&lt;br /&gt;
Low frequencies ---  289.1112  289.1112  403.8613&lt;br /&gt;
&amp;lt;/pre&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;jmol of Borazine&#039;&#039;&#039;&lt;br /&gt;
&amp;lt;jmol&amp;gt;&amp;lt;jmolApplet&amp;gt;&lt;br /&gt;
  &amp;lt;title&amp;gt;optimised Borazine&amp;lt;/title&amp;gt;&lt;br /&gt;
  &amp;lt;color&amp;gt;black&amp;lt;/color&amp;gt;&lt;br /&gt;
  &amp;lt;size&amp;gt;200&amp;lt;/size&amp;gt;&lt;br /&gt;
  &amp;lt;uploadedFileContents&amp;gt;HYC116_BORAZINE_FREQ.LOG&amp;lt;/uploadedFileContents&amp;gt;&lt;br /&gt;
&amp;lt;/jmolApplet&amp;gt;&amp;lt;/jmol&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
===Charge distribution===&lt;br /&gt;
&lt;br /&gt;
An NBO charge analysis was carried out on both the optimised benzene and borazine. Visualisations of the charge distribution are shown in the table below, with the colour range going from -1.102 to 1.102 for both molecule. This large scale was chosen as it allows direct comparison of the charge on any atoms in these two molecules and shows the relative magnitude of charges on all these atoms. Negative charges are shown in red, and positive charges are shown in green. A neutral charge is displayed in black, so the smaller a charge is (positive or negative), the darker its colour representation is. Larger charges are shown in brighter colours. The charges are also displayed on the atoms as numbers with a neutral charge being zero. Negative charges are shown as negative number and positive charges are shown as positive numbers. &lt;br /&gt;
&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot;&lt;br /&gt;
!&lt;br /&gt;
!Benzene&lt;br /&gt;
!Borazine&lt;br /&gt;
|-&lt;br /&gt;
!Visualisation of charge distribution&lt;br /&gt;
|[[File:Hyc116_benzene_charge_distribution1.png|500x500px|thumb|centre|Charge distribution of Benzene visualisation]]&lt;br /&gt;
|[[File:Hyc116_borazine_charge_distribution1.png|500x500px|thumb|centre|Charge distribution of Borazine visualisation]]&lt;br /&gt;
|-&lt;br /&gt;
!Charge &lt;br /&gt;
|Carbon: -0.239&lt;br /&gt;
&lt;br /&gt;
Hydrogen: 0.239&lt;br /&gt;
|Nitrogen: -1.102 &lt;br /&gt;
&lt;br /&gt;
Boron: 0.747&lt;br /&gt;
&lt;br /&gt;
Hydrogen (bonded to N): 0.432&lt;br /&gt;
&lt;br /&gt;
Hydrogen (bonded to B): -0.077&lt;br /&gt;
|-&lt;br /&gt;
!Discussion&lt;br /&gt;
|From the visualisation, it is shown that there is a slightly negative charge on the carbon atoms, and a positive charge of the same magnitude on the hydrogen atoms. All the carbon atoms have the same charge as they are in identical environments. The same applies to all the hydrogen atoms. This is due to the highly symmetrical structure of benzene. Since the same colour scale was used for both benzene and borazine, and the charges are much smaller in magnitude on atoms in benzene than atoms on borazine, the colours on the charge distribution visualisation is much darker. &lt;br /&gt;
|From the colours displayed on the charge distribution visualisation as well as the charge values, it is shown that nitrogen has a relatively large negative charge, while boron has a positive charge. This is due to the difference in electrogenativity between these atoms: nitrogen atoms are more electronegative than boron and tends to attract electrons towards themselves. It is worth noting that the hydrogen atoms do not all have the same charge. The hydrogen atoms bonded to boron have a slightly negative charge, and the ones bonded to nitrogen have a small positive charge. &lt;br /&gt;
&lt;br /&gt;
The fact that the same colour scale was used for both molecules comes in helpful here. It allows the charges on atoms to be compared directly. For example, just from looking at the colours, one can tell that or example, even though both carbon and nitrogen are electronegative, nitrogen is much more electronegative, which is quantitatively shown by Pauling&#039;s electronegativity scale.&lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
===Comparative MOs of Benzene and Borazine===&lt;br /&gt;
&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot;&lt;br /&gt;
!&lt;br /&gt;
!Benzene&lt;br /&gt;
!Borazine&lt;br /&gt;
!Comparison and Discussion&lt;br /&gt;
|-&lt;br /&gt;
!1st comparative pair&lt;br /&gt;
|[[File:Hyc116_benzene_1st_MO_pair_7.png|200x200px|centre]]&lt;br /&gt;
|[[File:Hyc116_borazine_1st_MO_pair_level9.png|200x200px|centre]]&lt;br /&gt;
|MO 9 of both benzene and borazine are comparable. They both show delocalised molecular orbital with an overall bonding character. There is a nodal plane across the molecular orbitals for both benzene and borazine. For benzene, there is contribution from all the carbon and hydrogen s orbitals. Moreover, the molecular orbitals are symmetric to their counterpart of opposite phase. That is not the case for borazine; they are less symmetric in borazine. Nitrogen atoms are more electronegative than boron atoms and pull electron density towards themselves, resulting in a larger MO. There is contribution from all the boron and nitrogen s orbitals, and three of the hydrogen s orbitals, though not all of them. &lt;br /&gt;
|-&lt;br /&gt;
!2nd comparative pair&lt;br /&gt;
|[[File:Hyc116_benzene_2nd_MO_pair_10.png|200x200px|centre]]&lt;br /&gt;
|[[File:Hyc116_borazine_2nd_MO_pair_level11.png|200x200px|centre]]&lt;br /&gt;
|&lt;br /&gt;
|-&lt;br /&gt;
!3rd comparative pair&lt;br /&gt;
|[[File:Hyc116_benzene_3rd_MO_pair_21.png|200x200px|centre]]&lt;br /&gt;
|[[File:Hyc116_borazine_3rd_MO_pair_level21.png|200x200px|centre]]&lt;br /&gt;
|&lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
===Aromaticity: some theories===&lt;br /&gt;
&lt;br /&gt;
==References==&lt;/div&gt;</summary>
		<author><name>Hyc116</name></author>
	</entry>
	<entry>
		<id>https://chemwiki.ch.ic.ac.uk/index.php?title=MO_hyc116&amp;diff=730178</id>
		<title>MO hyc116</title>
		<link rel="alternate" type="text/html" href="https://chemwiki.ch.ic.ac.uk/index.php?title=MO_hyc116&amp;diff=730178"/>
		<updated>2018-05-24T17:38:48Z</updated>

		<summary type="html">&lt;p&gt;Hyc116: &lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;==BH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;==&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;Calculation type&amp;lt;/b&amp;gt;: Optimisation&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;Calculation Method&amp;lt;/b&amp;gt;: B3LYP&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;Basis set&amp;lt;/b&amp;gt;: 6-31G(d,p) &lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Summary table&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
[[file:Hyc116_bh3_631g_opt_summarytable.png]]&lt;br /&gt;
&lt;br /&gt;
The above summary table was obtained after the 2nd optimisation of BH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt; (after the initial optimisation using the 3-21G basis set). Notice how the symmetry is incorrect and shown as Cs. This is because the symmetry was manually broken at the beginning by changing the bond length of B-H bonds. The point group was manually adjusted and the molecule was optimised again before the frequency analysis and the new summary table is attached below.&lt;br /&gt;
&lt;br /&gt;
[[file:Hyc116_bh3_correctsummarytable.png]]&lt;br /&gt;
&lt;br /&gt;
The above summary table was obtained from the optimisation after adjusting the symmetry. The point shown in this summary table is D&amp;lt;sub&amp;gt;3h&amp;lt;/sub&amp;gt;, which is the correct for BH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;. &lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Items table&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
Below is the items table taken from the optimisation with the correct point group.&lt;br /&gt;
&lt;br /&gt;
&amp;lt;pre&amp;gt;&lt;br /&gt;
Item               Value     Threshold  Converged?&lt;br /&gt;
 Maximum Force            0.000015     0.000450     YES&lt;br /&gt;
 RMS     Force            0.000010     0.000300     YES&lt;br /&gt;
 Maximum Displacement     0.000058     0.001800     YES&lt;br /&gt;
 RMS     Displacement     0.000038     0.001200     YES&lt;br /&gt;
&amp;lt;/pre&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Frequency log file&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
[[Media:HYC116 BH3 FREQ.LOG]] &lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Frequencies&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;pre&amp;gt;&lt;br /&gt;
Low frequencies ---  -10.3498   -3.4492   -1.2454   -0.0055    0.4779    3.2165&lt;br /&gt;
Low frequencies --- 1162.9519 1213.1527 1213.1554&lt;br /&gt;
&amp;lt;/pre&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;jmol of BH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;&#039;&#039;&#039;&lt;br /&gt;
&amp;lt;jmol&amp;gt;&amp;lt;jmolApplet&amp;gt;&lt;br /&gt;
  &amp;lt;title&amp;gt;optimised BH3&amp;lt;/title&amp;gt;&lt;br /&gt;
  &amp;lt;color&amp;gt;black&amp;lt;/color&amp;gt;&lt;br /&gt;
  &amp;lt;size&amp;gt;200&amp;lt;/size&amp;gt;&lt;br /&gt;
  &amp;lt;uploadedFileContents&amp;gt;HYC116_BH3_FREQ.LOG&amp;lt;/uploadedFileContents&amp;gt;&lt;br /&gt;
&amp;lt;/jmolApplet&amp;gt;&amp;lt;/jmol&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
===Vibrational spectrum===&lt;br /&gt;
&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot;&lt;br /&gt;
!wavenumber (cm&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;)&lt;br /&gt;
!Intensity (arbitrary units)&lt;br /&gt;
!symmetry&lt;br /&gt;
!IR active?&lt;br /&gt;
!type&lt;br /&gt;
|-&lt;br /&gt;
|1163&lt;br /&gt;
|93&lt;br /&gt;
|A&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;&#039; &#039;&lt;br /&gt;
|Yes&lt;br /&gt;
|Out of plane bend&lt;br /&gt;
|-&lt;br /&gt;
|1213&lt;br /&gt;
|14&lt;br /&gt;
|E&#039;&lt;br /&gt;
|Very slight&lt;br /&gt;
|Bend&lt;br /&gt;
|-&lt;br /&gt;
|1213&lt;br /&gt;
|14&lt;br /&gt;
|E&#039;&lt;br /&gt;
|Very slight&lt;br /&gt;
|Bend&lt;br /&gt;
|-&lt;br /&gt;
|2582&lt;br /&gt;
|0&lt;br /&gt;
|A&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;&#039;&lt;br /&gt;
|No&lt;br /&gt;
|Symmetric stretch&lt;br /&gt;
|-&lt;br /&gt;
|2716&lt;br /&gt;
|126&lt;br /&gt;
|E&#039;&lt;br /&gt;
|Yes&lt;br /&gt;
|Asymmetric stretch&lt;br /&gt;
|-&lt;br /&gt;
|2716&lt;br /&gt;
|126&lt;br /&gt;
|E&#039;&lt;br /&gt;
|Yes&lt;br /&gt;
|Asymmetric stretch&lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;IR spectrum&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
[[file:Hyc116_ir_bh3.png|400*600]]&lt;br /&gt;
&lt;br /&gt;
There are only three peaks on the IR spectrum of BH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;, despite that there are 6 vibrational modes for the molecule. As shown in the table above, the symmetric stretching mode with A1 symmetry at 2582 cm&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt; is not IR active; naturally, that vibrational mode doesn’t give a peak on the IR spectrum. As shown from the table, two pairs of vibrational modes, the bond angle deformation/bend at 1213 cm&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt; and the asymmetric bond stretch at 2716 cm&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;, are degenerate with the symmetry label E. This means that they have the same energy, and hence give the same wavenumber on the IR spectrum. Each pair of degenerate vibrational modes give rise to one peak. This leaves three peaks, as confirmed by the IR spectrum above.&lt;br /&gt;
&lt;br /&gt;
===Molecular orbitals of BH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;===&lt;br /&gt;
&lt;br /&gt;
[[file:hyc116_bh3_MO_diagram.png]]&lt;br /&gt;
&lt;br /&gt;
The above molecular orbital diagram was taken from Dr Patricia Hunt&#039;s &amp;lt;i&amp;gt;Lecture 4 Tutorial Problem Model Answers&amp;lt;/i&amp;gt;. . Diagrams of the &amp;quot;real&amp;quot; MOs were obtained from Gaussian.&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
There is no significant difference between the LCAO MOs and the real ones. Features such as orbital phases are shown clearly on both the LCAO MOs and the real MOs, illustrating the bonding/anti-bonding characters of the molecular orbitals. This suggests that the the qualitative MO theory is highly accurate and useful when studying the molecular orbitals of molecules.&lt;br /&gt;
&lt;br /&gt;
==Associated energies: ammonium borane==&lt;br /&gt;
&lt;br /&gt;
===NH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;===&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;Calculation type&amp;lt;/b&amp;gt;: Optimisation&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;Calculation Method&amp;lt;/b&amp;gt;: B3LYP&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;Basis set&amp;lt;/b&amp;gt;: 6-31G(d,p) &lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Summary table&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
[[file:Hyc116_nh3_631g_summarytable.png]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Items table&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;pre&amp;gt;&lt;br /&gt;
Item               Value     Threshold  Converged?&lt;br /&gt;
 Maximum Force            0.000006     0.000450     YES&lt;br /&gt;
 RMS     Force            0.000004     0.000300     YES&lt;br /&gt;
 Maximum Displacement     0.000012     0.001800     YES&lt;br /&gt;
 RMS     Displacement     0.000008     0.001200     YES&lt;br /&gt;
&amp;lt;/pre&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Frequency log file&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
[[Media:HYC116_NH3_FREQ.LOG]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Frequencies&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;pre&amp;gt;&lt;br /&gt;
Low frequencies ---   -8.5646   -8.5588   -0.0047    0.0454    0.1784   26.4183&lt;br /&gt;
Low frequencies --- 1089.7603 1694.1865 1694.1865&lt;br /&gt;
&amp;lt;/pre&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;jmol of NH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;&#039;&#039;&#039;&lt;br /&gt;
&amp;lt;jmol&amp;gt;&amp;lt;jmolApplet&amp;gt;&lt;br /&gt;
  &amp;lt;title&amp;gt;optimised NH3&amp;lt;/title&amp;gt;&lt;br /&gt;
  &amp;lt;color&amp;gt;black&amp;lt;/color&amp;gt;&lt;br /&gt;
  &amp;lt;size&amp;gt;200&amp;lt;/size&amp;gt;&lt;br /&gt;
  &amp;lt;uploadedFileContents&amp;gt;HYC116_NH3_FREQ.LOG&amp;lt;/uploadedFileContents&amp;gt;&lt;br /&gt;
&amp;lt;/jmolApplet&amp;gt;&amp;lt;/jmol&amp;gt;&lt;br /&gt;
&lt;br /&gt;
===NH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;BH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;===&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;Calculation type&amp;lt;/b&amp;gt;: Optimisation&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;Calculation Method&amp;lt;/b&amp;gt;: B3LYP&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;Basis set&amp;lt;/b&amp;gt;: 6-31G(d,p) &lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Summary table&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
[[file:Hyc116_nh3bh3_631g_summarytable.png]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Items table&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;pre&amp;gt;&lt;br /&gt;
Item               Value     Threshold  Converged?&lt;br /&gt;
 Maximum Force            0.000123     0.000450     YES&lt;br /&gt;
 RMS     Force            0.000058     0.000300     YES&lt;br /&gt;
 Maximum Displacement     0.000515     0.001800     YES&lt;br /&gt;
 RMS     Displacement     0.000296     0.001200     YES&lt;br /&gt;
&amp;lt;/pre&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Frequency log file&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
[[Media:HYC116_NH3BH3_FREQ.LOG]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Frequencies&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;pre&amp;gt;&lt;br /&gt;
Low frequencies ---   -0.0014   -0.0011   -0.0006    6.9624   20.4518   43.5542&lt;br /&gt;
Low frequencies ---  266.4530  632.2458  639.0504&lt;br /&gt;
&amp;lt;/pre&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;jmol of NH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;BH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;&#039;&#039;&#039;&lt;br /&gt;
&amp;lt;jmol&amp;gt;&amp;lt;jmolApplet&amp;gt;&lt;br /&gt;
  &amp;lt;title&amp;gt;optimised NH3BH3&amp;lt;/title&amp;gt;&lt;br /&gt;
  &amp;lt;color&amp;gt;black&amp;lt;/color&amp;gt;&lt;br /&gt;
  &amp;lt;size&amp;gt;200&amp;lt;/size&amp;gt;&lt;br /&gt;
  &amp;lt;uploadedFileContents&amp;gt;HYC116_NH3BH3_FREQ.LOG&amp;lt;/uploadedFileContents&amp;gt;&lt;br /&gt;
&amp;lt;/jmolApplet&amp;gt;&amp;lt;/jmol&amp;gt;&lt;br /&gt;
&lt;br /&gt;
===Association energy===&lt;br /&gt;
&lt;br /&gt;
E(BH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;) (using the optimisation with the correct symmetry) = -26.61532363 a.u. = &amp;lt;b&amp;gt;-26.61532 a.u. (5 d.p.)&amp;lt;/b&amp;gt;&lt;br /&gt;
&lt;br /&gt;
E(NH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;) = -56.55776873 a.u. = &amp;lt;b&amp;gt;-56.55777 a.u. (5 d.p.)&amp;lt;/b&amp;gt;&lt;br /&gt;
&lt;br /&gt;
E(NH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;BH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;) = -83.22468893 a.u. = &amp;lt;b&amp;gt;-83.22469 a.u. (5 d.p.)&amp;lt;/b&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
Carrying out calculations using numbers which has already been rounded up can possibly result in errors in the last digit. Hence, here the calculations were carried out using the numbers provided from the optimisations (i.e. with more decimal places than necessary); the answer was then rounded up to the desired accuracy. &lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
ΔE = E(NH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;BH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;)-[E(NH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;)+E(BH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;)]&lt;br /&gt;
&lt;br /&gt;
ΔE = -83.22468893 - (-56.55776873 + -26.61532363) = -0.05159657 a.u. &lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;ΔE = -0.05160 a.u. (5 d.p.)&amp;lt;/b&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Converting energy from a.u. to kJ/mol&#039;&#039;&#039;&lt;br /&gt;
An atomic unit for energy is Hartree, which is equal to 2625.5 kJ/mol. &lt;br /&gt;
&lt;br /&gt;
So ΔE in kJ/mol = -0.05159657 * 2625.5 = -135.466794535 kJ/mol&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;ΔE = -135 kJ/mol (nearest integer)&amp;lt;/b&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
The energy difference calculated above comes from the formation of the B-N dative bond. It is a relatively weak bond. According to a bond energy data sheet provided by the University of California,  the bond energy of the C-C bond of an ethane molecule is 368 kJ/mol. This is a fair comparison to the NH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;BH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt; molecule as the two molecules have the same structure, only with the carbon atoms on ethane swapped for Boron and Nitrogen in NH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;BH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;&lt;br /&gt;
&lt;br /&gt;
==Using a mixture of basis-sets and pseudo-potentials==&lt;br /&gt;
&lt;br /&gt;
===BBr&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;===&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;Calculation type&amp;lt;/b&amp;gt;: Optimisation&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;Calculation Method&amp;lt;/b&amp;gt;: B3LYP&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;Basis set&amp;lt;/b&amp;gt;: Boron: 6-31G(d,p) ; Br: LANL2DZ&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
Larger calculations are often sent to a web-server to run on a high-performance computer instead of a desktop. In order to experience and learn to use a web-server, the optimisation and the frequency analysis for BBr&amp;lt;sub&amp;gt;3&amp;lt;/sub were both sent and done on a server instead of the desktop. The calculation results were downloaded from the web-server once they were finished.   &lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Summary table&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
[[file:Hyc116_bbr3_opt_summarytable.png]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Items table&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;pre&amp;gt;&lt;br /&gt;
Item               Value     Threshold  Converged?&lt;br /&gt;
 Maximum Force            0.000008     0.000450     YES&lt;br /&gt;
 RMS     Force            0.000005     0.000300     YES&lt;br /&gt;
 Maximum Displacement     0.000036     0.001800     YES&lt;br /&gt;
 RMS     Displacement     0.000023     0.001200     YES&lt;br /&gt;
&amp;lt;/pre&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Frequency log file&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
[[Media:Hyc116_bbr3_freq.log]]&lt;br /&gt;
&lt;br /&gt;
Attached above is the frequency file saved onto the computer from the SCAN server portal. The frequency file was also published on the chemistry database DSpace. {{DOI|10042/202442}}&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Frequencies&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;pre&amp;gt;&lt;br /&gt;
Low frequencies ---   -0.0137   -0.0064   -0.0046    2.4315    2.4315    4.8421&lt;br /&gt;
Low frequencies ---  155.9631  155.9651  267.7052&lt;br /&gt;
&amp;lt;/pre&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;jmol of BBr&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;&#039;&#039;&#039;&lt;br /&gt;
&amp;lt;jmol&amp;gt;&amp;lt;jmolApplet&amp;gt;&lt;br /&gt;
  &amp;lt;title&amp;gt;optimised BBr3&amp;lt;/title&amp;gt;&lt;br /&gt;
  &amp;lt;color&amp;gt;black&amp;lt;/color&amp;gt;&lt;br /&gt;
  &amp;lt;size&amp;gt;200&amp;lt;/size&amp;gt;&lt;br /&gt;
  &amp;lt;uploadedFileContents&amp;gt;Hyc116_bbr3_freq.log&amp;lt;/uploadedFileContents&amp;gt;&lt;br /&gt;
&amp;lt;/jmolApplet&amp;gt;&amp;lt;/jmol&amp;gt;&lt;br /&gt;
&lt;br /&gt;
==Aromaticity==&lt;br /&gt;
&lt;br /&gt;
===Benzene===&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;Calculation type&amp;lt;/b&amp;gt;: Optimisation&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;Calculation Method&amp;lt;/b&amp;gt;: B3LYP&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;Basis set&amp;lt;/b&amp;gt;: 6-31G(d,p) &lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Summary table&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
[[file:Hyc116_c6h6_summarytable.png]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Items table&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;pre&amp;gt;&lt;br /&gt;
Item               Value     Threshold  Converged?&lt;br /&gt;
 Maximum Force            0.000193     0.000450     YES&lt;br /&gt;
 RMS     Force            0.000079     0.000300     YES&lt;br /&gt;
 Maximum Displacement     0.000830     0.001800     YES&lt;br /&gt;
 RMS     Displacement     0.000294     0.001200     YES&lt;br /&gt;
&amp;lt;/pre&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Frequency log file&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
[[Media:HYC116_C6H6_FREQ.LOG]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Frequencies&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;pre&amp;gt;&lt;br /&gt;
Low frequencies ---   -3.5606   -3.5606   -0.0089   -0.0043   -0.0043   10.0905&lt;br /&gt;
Low frequencies ---  413.9582  413.9582  621.1416&lt;br /&gt;
&amp;lt;/pre&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;jmol of C&amp;lt;sub&amp;gt;6&amp;lt;/sub&amp;gt;H&amp;lt;sub&amp;gt;6&amp;lt;/sub&amp;gt;&#039;&#039;&#039;&lt;br /&gt;
&amp;lt;jmol&amp;gt;&amp;lt;jmolApplet&amp;gt;&lt;br /&gt;
  &amp;lt;title&amp;gt;optimised Benzene&amp;lt;/title&amp;gt;&lt;br /&gt;
  &amp;lt;color&amp;gt;black&amp;lt;/color&amp;gt;&lt;br /&gt;
  &amp;lt;size&amp;gt;200&amp;lt;/size&amp;gt;&lt;br /&gt;
  &amp;lt;uploadedFileContents&amp;gt;HYC116_C6H6_FREQ.LOG&amp;lt;/uploadedFileContents&amp;gt;&lt;br /&gt;
&amp;lt;/jmolApplet&amp;gt;&amp;lt;/jmol&amp;gt;&lt;br /&gt;
&lt;br /&gt;
===Borazine===&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;Calculation type&amp;lt;/b&amp;gt;: Optimisation&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;Calculation Method&amp;lt;/b&amp;gt;: B3LYP&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;Basis set&amp;lt;/b&amp;gt;: 6-31G(d,p) &lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Summary table&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
[[file:Hyc116_borazine_summarytable.png]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Items table&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;pre&amp;gt;&lt;br /&gt;
Item               Value     Threshold  Converged?&lt;br /&gt;
 Maximum Force            0.000085     0.000450     YES&lt;br /&gt;
 RMS     Force            0.000033     0.000300     YES&lt;br /&gt;
 Maximum Displacement     0.000250     0.001800     YES&lt;br /&gt;
 RMS     Displacement     0.000074     0.001200     YES&lt;br /&gt;
&amp;lt;/pre&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Frequency log file&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
[[Media:HYC116_BORAZINE_FREQ.LOG]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Frequencies&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;pre&amp;gt;&lt;br /&gt;
Low frequencies ---  -12.6626  -12.6626   -8.9272   -0.0211   -0.0104   -0.0104&lt;br /&gt;
Low frequencies ---  289.1112  289.1112  403.8613&lt;br /&gt;
&amp;lt;/pre&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;jmol of Borazine&#039;&#039;&#039;&lt;br /&gt;
&amp;lt;jmol&amp;gt;&amp;lt;jmolApplet&amp;gt;&lt;br /&gt;
  &amp;lt;title&amp;gt;optimised Borazine&amp;lt;/title&amp;gt;&lt;br /&gt;
  &amp;lt;color&amp;gt;black&amp;lt;/color&amp;gt;&lt;br /&gt;
  &amp;lt;size&amp;gt;200&amp;lt;/size&amp;gt;&lt;br /&gt;
  &amp;lt;uploadedFileContents&amp;gt;HYC116_BORAZINE_FREQ.LOG&amp;lt;/uploadedFileContents&amp;gt;&lt;br /&gt;
&amp;lt;/jmolApplet&amp;gt;&amp;lt;/jmol&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
===Charge distribution===&lt;br /&gt;
&lt;br /&gt;
An NBO charge analysis was carried out on both the optimised benzene and borazine. Visualisations of the charge distribution are shown in the table below, with the colour range going from -1.102 to 1.102 for both molecule. This large scale was chosen as it allows direct comparison of the charge on any atoms in these two molecules and shows the relative magnitude of charges on all these atoms. Negative charges are shown in red, and positive charges are shown in green. A neutral charge is displayed in black, so the smaller a charge is (positive or negative), the darker its colour representation is. Larger charges are shown in brighter colours. The charges are also displayed on the atoms as numbers with a neutral charge being zero. Negative charges are shown as negative number and positive charges are shown as positive numbers. &lt;br /&gt;
&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot;&lt;br /&gt;
!&lt;br /&gt;
!Benzene&lt;br /&gt;
!Borazine&lt;br /&gt;
|-&lt;br /&gt;
!Visualisation of charge distribution&lt;br /&gt;
|[[File:Hyc116_benzene_charge_distribution1.png|500x500px|thumb|centre|Charge distribution of Benzene visualisation]]&lt;br /&gt;
|[[File:Hyc116_borazine_charge_distribution1.png|500x500px|thumb|centre|Charge distribution of Borazine visualisation]]&lt;br /&gt;
|-&lt;br /&gt;
!Charge &lt;br /&gt;
|Carbon: -0.239&lt;br /&gt;
&lt;br /&gt;
Hydrogen: 0.239&lt;br /&gt;
|Nitrogen: -1.102 &lt;br /&gt;
&lt;br /&gt;
Boron: 0.747&lt;br /&gt;
&lt;br /&gt;
Hydrogen (bonded to N): 0.432&lt;br /&gt;
&lt;br /&gt;
Hydrogen (bonded to B): -0.077&lt;br /&gt;
|-&lt;br /&gt;
!Discussion&lt;br /&gt;
|From the visualisation, it is shown that there is a slightly negative charge on the carbon atoms, and a positive charge of the same magnitude on the hydrogen atoms. All the carbon atoms have the same charge as they are in identical environments. The same applies to all the hydrogen atoms. This is due to the highly symmetrical structure of benzene. Since the same colour scale was used for both benzene and borazine, and the charges are much smaller in magnitude on atoms in benzene than atoms on borazine, the colours on the charge distribution visualisation is much darker. &lt;br /&gt;
|From the colours displayed on the charge distribution visualisation as well as the charge values, it is shown that nitrogen has a relatively large negative charge, while boron has a positive charge. This is due to the difference in electrogenativity between these atoms: nitrogen atoms are more electronegative than boron and tends to attract electrons towards themselves. It is worth noting that the hydrogen atoms do not all have the same charge. The hydrogen atoms bonded to boron have a slightly negative charge, and the ones bonded to nitrogen have a small positive charge. &lt;br /&gt;
&lt;br /&gt;
The fact that the same colour scale was used for both molecules comes in helpful here. It allows the charges on atoms to be compared directly. For example, just from looking at the colours, one can tell that or example, even though both carbon and nitrogen are electronegative, nitrogen is much more electronegative, which is quantitatively shown by Pauling&#039;s electronegativity scale.&lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
===Comparative MOs of Benzene and Borazine===&lt;br /&gt;
&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot;&lt;br /&gt;
!&lt;br /&gt;
!Benzene&lt;br /&gt;
!Borazine&lt;br /&gt;
!Comparison and Discussion&lt;br /&gt;
|-&lt;br /&gt;
!1st comparative pair&lt;br /&gt;
|[[File:Hyc116_benzene_1st_MO_pair_7.png|200x200px|centre]]&lt;br /&gt;
|[[File:Hyc116_borazine_1st_MO_pair_level9.png|200x200px|centre]]&lt;br /&gt;
|MO 9 of both benzene and borazine are comparable. They both show delocalised molecular orbital with an overall bonding character. There is a nodal plane across the molecular orbitals for both benzene and borazine. For benzene, there is contribution from all the carbon and hydrogen s orbitals. Moreover, the molecular orbitals are symmetric to their counterpart of opposite phase. That is not the case for borazine; they are less symmetric in borazine. Nitrogen atoms are more electronegative than boron atoms and pull electron density towards themselves, resulting in a larger MO. There is contribution from all the boron and nitrogen s orbitals, and three of the hydrogen s orbitals, though not all of them. &lt;br /&gt;
|-&lt;br /&gt;
!2nd comparative pair&lt;br /&gt;
|[[File:Hyc116_benzene_2nd_MO_pair_10.png|200x200px|centre]]&lt;br /&gt;
|[[File:Hyc116_borazine_2nd_MO_pair_level11.png|200x200px|centre]]&lt;br /&gt;
|&lt;br /&gt;
|-&lt;br /&gt;
!3rd comparative pair&lt;br /&gt;
|[[File:Hyc116_benzene_3rd_MO_pair_21.png|200x200px|centre]]&lt;br /&gt;
|[[File:Hyc116_borazine_3rd_MO_pair_level21.png|200x200px|centre]]&lt;br /&gt;
|&lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
===Aromaticity: some theories===&lt;br /&gt;
&lt;br /&gt;
==References==&lt;br /&gt;
&lt;br /&gt;
===asdf===&lt;/div&gt;</summary>
		<author><name>Hyc116</name></author>
	</entry>
	<entry>
		<id>https://chemwiki.ch.ic.ac.uk/index.php?title=MO_hyc116&amp;diff=730177</id>
		<title>MO hyc116</title>
		<link rel="alternate" type="text/html" href="https://chemwiki.ch.ic.ac.uk/index.php?title=MO_hyc116&amp;diff=730177"/>
		<updated>2018-05-24T17:38:29Z</updated>

		<summary type="html">&lt;p&gt;Hyc116: &lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;==BH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;==&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;Calculation type&amp;lt;/b&amp;gt;: Optimisation&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;Calculation Method&amp;lt;/b&amp;gt;: B3LYP&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;Basis set&amp;lt;/b&amp;gt;: 6-31G(d,p) &lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Summary table&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
[[file:Hyc116_bh3_631g_opt_summarytable.png]]&lt;br /&gt;
&lt;br /&gt;
The above summary table was obtained after the 2nd optimisation of BH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt; (after the initial optimisation using the 3-21G basis set). Notice how the symmetry is incorrect and shown as Cs. This is because the symmetry was manually broken at the beginning by changing the bond length of B-H bonds. The point group was manually adjusted and the molecule was optimised again before the frequency analysis and the new summary table is attached below.&lt;br /&gt;
&lt;br /&gt;
[[file:Hyc116_bh3_correctsummarytable.png]]&lt;br /&gt;
&lt;br /&gt;
The above summary table was obtained from the optimisation after adjusting the symmetry. The point shown in this summary table is D&amp;lt;sub&amp;gt;3h&amp;lt;/sub&amp;gt;, which is the correct for BH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;. &lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Items table&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
Below is the items table taken from the optimisation with the correct point group.&lt;br /&gt;
&lt;br /&gt;
&amp;lt;pre&amp;gt;&lt;br /&gt;
Item               Value     Threshold  Converged?&lt;br /&gt;
 Maximum Force            0.000015     0.000450     YES&lt;br /&gt;
 RMS     Force            0.000010     0.000300     YES&lt;br /&gt;
 Maximum Displacement     0.000058     0.001800     YES&lt;br /&gt;
 RMS     Displacement     0.000038     0.001200     YES&lt;br /&gt;
&amp;lt;/pre&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Frequency log file&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
[[Media:HYC116 BH3 FREQ.LOG]] &lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Frequencies&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;pre&amp;gt;&lt;br /&gt;
Low frequencies ---  -10.3498   -3.4492   -1.2454   -0.0055    0.4779    3.2165&lt;br /&gt;
Low frequencies --- 1162.9519 1213.1527 1213.1554&lt;br /&gt;
&amp;lt;/pre&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;jmol of BH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;&#039;&#039;&#039;&lt;br /&gt;
&amp;lt;jmol&amp;gt;&amp;lt;jmolApplet&amp;gt;&lt;br /&gt;
  &amp;lt;title&amp;gt;optimised BH3&amp;lt;/title&amp;gt;&lt;br /&gt;
  &amp;lt;color&amp;gt;black&amp;lt;/color&amp;gt;&lt;br /&gt;
  &amp;lt;size&amp;gt;200&amp;lt;/size&amp;gt;&lt;br /&gt;
  &amp;lt;uploadedFileContents&amp;gt;HYC116_BH3_FREQ.LOG&amp;lt;/uploadedFileContents&amp;gt;&lt;br /&gt;
&amp;lt;/jmolApplet&amp;gt;&amp;lt;/jmol&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
===Vibrational spectrum===&lt;br /&gt;
&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot;&lt;br /&gt;
!wavenumber (cm&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;)&lt;br /&gt;
!Intensity (arbitrary units)&lt;br /&gt;
!symmetry&lt;br /&gt;
!IR active?&lt;br /&gt;
!type&lt;br /&gt;
|-&lt;br /&gt;
|1163&lt;br /&gt;
|93&lt;br /&gt;
|A&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;&#039; &#039;&lt;br /&gt;
|Yes&lt;br /&gt;
|Out of plane bend&lt;br /&gt;
|-&lt;br /&gt;
|1213&lt;br /&gt;
|14&lt;br /&gt;
|E&#039;&lt;br /&gt;
|Very slight&lt;br /&gt;
|Bend&lt;br /&gt;
|-&lt;br /&gt;
|1213&lt;br /&gt;
|14&lt;br /&gt;
|E&#039;&lt;br /&gt;
|Very slight&lt;br /&gt;
|Bend&lt;br /&gt;
|-&lt;br /&gt;
|2582&lt;br /&gt;
|0&lt;br /&gt;
|A&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;&#039;&lt;br /&gt;
|No&lt;br /&gt;
|Symmetric stretch&lt;br /&gt;
|-&lt;br /&gt;
|2716&lt;br /&gt;
|126&lt;br /&gt;
|E&#039;&lt;br /&gt;
|Yes&lt;br /&gt;
|Asymmetric stretch&lt;br /&gt;
|-&lt;br /&gt;
|2716&lt;br /&gt;
|126&lt;br /&gt;
|E&#039;&lt;br /&gt;
|Yes&lt;br /&gt;
|Asymmetric stretch&lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;IR spectrum&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
[[file:Hyc116_ir_bh3.png|400*600]]&lt;br /&gt;
&lt;br /&gt;
There are only three peaks on the IR spectrum of BH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;, despite that there are 6 vibrational modes for the molecule. As shown in the table above, the symmetric stretching mode with A1 symmetry at 2582 cm&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt; is not IR active; naturally, that vibrational mode doesn’t give a peak on the IR spectrum. As shown from the table, two pairs of vibrational modes, the bond angle deformation/bend at 1213 cm&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt; and the asymmetric bond stretch at 2716 cm&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;, are degenerate with the symmetry label E. This means that they have the same energy, and hence give the same wavenumber on the IR spectrum. Each pair of degenerate vibrational modes give rise to one peak. This leaves three peaks, as confirmed by the IR spectrum above.&lt;br /&gt;
&lt;br /&gt;
===Molecular orbitals of BH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;===&lt;br /&gt;
&lt;br /&gt;
[[file:hyc116_bh3_MO_diagram.png]]&lt;br /&gt;
&lt;br /&gt;
The above molecular orbital diagram was taken from Dr Patricia Hunt&#039;s &amp;lt;i&amp;gt;Lecture 4 Tutorial Problem Model Answers&amp;lt;/i&amp;gt;. . Diagrams of the &amp;quot;real&amp;quot; MOs were obtained from Gaussian.&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
There is no significant difference between the LCAO MOs and the real ones. Features such as orbital phases are shown clearly on both the LCAO MOs and the real MOs, illustrating the bonding/anti-bonding characters of the molecular orbitals. This suggests that the the qualitative MO theory is highly accurate and useful when studying the molecular orbitals of molecules.&lt;br /&gt;
&lt;br /&gt;
==Associated energies: ammonium borane==&lt;br /&gt;
&lt;br /&gt;
===NH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;===&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;Calculation type&amp;lt;/b&amp;gt;: Optimisation&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;Calculation Method&amp;lt;/b&amp;gt;: B3LYP&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;Basis set&amp;lt;/b&amp;gt;: 6-31G(d,p) &lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Summary table&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
[[file:Hyc116_nh3_631g_summarytable.png]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Items table&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;pre&amp;gt;&lt;br /&gt;
Item               Value     Threshold  Converged?&lt;br /&gt;
 Maximum Force            0.000006     0.000450     YES&lt;br /&gt;
 RMS     Force            0.000004     0.000300     YES&lt;br /&gt;
 Maximum Displacement     0.000012     0.001800     YES&lt;br /&gt;
 RMS     Displacement     0.000008     0.001200     YES&lt;br /&gt;
&amp;lt;/pre&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Frequency log file&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
[[Media:HYC116_NH3_FREQ.LOG]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Frequencies&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;pre&amp;gt;&lt;br /&gt;
Low frequencies ---   -8.5646   -8.5588   -0.0047    0.0454    0.1784   26.4183&lt;br /&gt;
Low frequencies --- 1089.7603 1694.1865 1694.1865&lt;br /&gt;
&amp;lt;/pre&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;jmol of NH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;&#039;&#039;&#039;&lt;br /&gt;
&amp;lt;jmol&amp;gt;&amp;lt;jmolApplet&amp;gt;&lt;br /&gt;
  &amp;lt;title&amp;gt;optimised NH3&amp;lt;/title&amp;gt;&lt;br /&gt;
  &amp;lt;color&amp;gt;black&amp;lt;/color&amp;gt;&lt;br /&gt;
  &amp;lt;size&amp;gt;200&amp;lt;/size&amp;gt;&lt;br /&gt;
  &amp;lt;uploadedFileContents&amp;gt;HYC116_NH3_FREQ.LOG&amp;lt;/uploadedFileContents&amp;gt;&lt;br /&gt;
&amp;lt;/jmolApplet&amp;gt;&amp;lt;/jmol&amp;gt;&lt;br /&gt;
&lt;br /&gt;
===NH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;BH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;===&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;Calculation type&amp;lt;/b&amp;gt;: Optimisation&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;Calculation Method&amp;lt;/b&amp;gt;: B3LYP&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;Basis set&amp;lt;/b&amp;gt;: 6-31G(d,p) &lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Summary table&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
[[file:Hyc116_nh3bh3_631g_summarytable.png]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Items table&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;pre&amp;gt;&lt;br /&gt;
Item               Value     Threshold  Converged?&lt;br /&gt;
 Maximum Force            0.000123     0.000450     YES&lt;br /&gt;
 RMS     Force            0.000058     0.000300     YES&lt;br /&gt;
 Maximum Displacement     0.000515     0.001800     YES&lt;br /&gt;
 RMS     Displacement     0.000296     0.001200     YES&lt;br /&gt;
&amp;lt;/pre&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Frequency log file&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
[[Media:HYC116_NH3BH3_FREQ.LOG]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Frequencies&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;pre&amp;gt;&lt;br /&gt;
Low frequencies ---   -0.0014   -0.0011   -0.0006    6.9624   20.4518   43.5542&lt;br /&gt;
Low frequencies ---  266.4530  632.2458  639.0504&lt;br /&gt;
&amp;lt;/pre&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;jmol of NH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;BH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;&#039;&#039;&#039;&lt;br /&gt;
&amp;lt;jmol&amp;gt;&amp;lt;jmolApplet&amp;gt;&lt;br /&gt;
  &amp;lt;title&amp;gt;optimised NH3BH3&amp;lt;/title&amp;gt;&lt;br /&gt;
  &amp;lt;color&amp;gt;black&amp;lt;/color&amp;gt;&lt;br /&gt;
  &amp;lt;size&amp;gt;200&amp;lt;/size&amp;gt;&lt;br /&gt;
  &amp;lt;uploadedFileContents&amp;gt;HYC116_NH3BH3_FREQ.LOG&amp;lt;/uploadedFileContents&amp;gt;&lt;br /&gt;
&amp;lt;/jmolApplet&amp;gt;&amp;lt;/jmol&amp;gt;&lt;br /&gt;
&lt;br /&gt;
===Association energy===&lt;br /&gt;
&lt;br /&gt;
E(BH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;) (using the optimisation with the correct symmetry) = -26.61532363 a.u. = &amp;lt;b&amp;gt;-26.61532 a.u. (5 d.p.)&amp;lt;/b&amp;gt;&lt;br /&gt;
&lt;br /&gt;
E(NH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;) = -56.55776873 a.u. = &amp;lt;b&amp;gt;-56.55777 a.u. (5 d.p.)&amp;lt;/b&amp;gt;&lt;br /&gt;
&lt;br /&gt;
E(NH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;BH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;) = -83.22468893 a.u. = &amp;lt;b&amp;gt;-83.22469 a.u. (5 d.p.)&amp;lt;/b&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
Carrying out calculations using numbers which has already been rounded up can possibly result in errors in the last digit. Hence, here the calculations were carried out using the numbers provided from the optimisations (i.e. with more decimal places than necessary); the answer was then rounded up to the desired accuracy. &lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
ΔE = E(NH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;BH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;)-[E(NH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;)+E(BH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;)]&lt;br /&gt;
&lt;br /&gt;
ΔE = -83.22468893 - (-56.55776873 + -26.61532363) = -0.05159657 a.u. &lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;ΔE = -0.05160 a.u. (5 d.p.)&amp;lt;/b&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Converting energy from a.u. to kJ/mol&#039;&#039;&#039;&lt;br /&gt;
An atomic unit for energy is Hartree, which is equal to 2625.5 kJ/mol. &lt;br /&gt;
&lt;br /&gt;
So ΔE in kJ/mol = -0.05159657 * 2625.5 = -135.466794535 kJ/mol&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;ΔE = -135 kJ/mol (nearest integer)&amp;lt;/b&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
The energy difference calculated above comes from the formation of the B-N dative bond. It is a relatively weak bond. According to a bond energy data sheet provided by the University of California,  the bond energy of the C-C bond of an ethane molecule is 368 kJ/mol. This is a fair comparison to the NH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;BH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt; molecule as the two molecules have the same structure, only with the carbon atoms on ethane swapped for Boron and Nitrogen in NH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;BH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;&lt;br /&gt;
&lt;br /&gt;
==Using a mixture of basis-sets and pseudo-potentials==&lt;br /&gt;
&lt;br /&gt;
===BBr&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;===&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;Calculation type&amp;lt;/b&amp;gt;: Optimisation&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;Calculation Method&amp;lt;/b&amp;gt;: B3LYP&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;Basis set&amp;lt;/b&amp;gt;: Boron: 6-31G(d,p) ; Br: LANL2DZ&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
Larger calculations are often sent to a web-server to run on a high-performance computer instead of a desktop. In order to experience and learn to use a web-server, the optimisation and the frequency analysis for BBr&amp;lt;sub&amp;gt;3&amp;lt;/sub were both sent and done on a server instead of the desktop. The calculation results were downloaded from the web-server once they were finished.   &lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Summary table&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
[[file:Hyc116_bbr3_opt_summarytable.png]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Items table&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;pre&amp;gt;&lt;br /&gt;
Item               Value     Threshold  Converged?&lt;br /&gt;
 Maximum Force            0.000008     0.000450     YES&lt;br /&gt;
 RMS     Force            0.000005     0.000300     YES&lt;br /&gt;
 Maximum Displacement     0.000036     0.001800     YES&lt;br /&gt;
 RMS     Displacement     0.000023     0.001200     YES&lt;br /&gt;
&amp;lt;/pre&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Frequency log file&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
[[Media:Hyc116_bbr3_freq.log]]&lt;br /&gt;
&lt;br /&gt;
Attached above is the frequency file saved onto the computer from the SCAN server portal. The frequency file was also published on the chemistry database DSpace. {{DOI|10042/202442}}&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Frequencies&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;pre&amp;gt;&lt;br /&gt;
Low frequencies ---   -0.0137   -0.0064   -0.0046    2.4315    2.4315    4.8421&lt;br /&gt;
Low frequencies ---  155.9631  155.9651  267.7052&lt;br /&gt;
&amp;lt;/pre&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;jmol of BBr&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;&#039;&#039;&#039;&lt;br /&gt;
&amp;lt;jmol&amp;gt;&amp;lt;jmolApplet&amp;gt;&lt;br /&gt;
  &amp;lt;title&amp;gt;optimised BBr3&amp;lt;/title&amp;gt;&lt;br /&gt;
  &amp;lt;color&amp;gt;black&amp;lt;/color&amp;gt;&lt;br /&gt;
  &amp;lt;size&amp;gt;200&amp;lt;/size&amp;gt;&lt;br /&gt;
  &amp;lt;uploadedFileContents&amp;gt;Hyc116_bbr3_freq.log&amp;lt;/uploadedFileContents&amp;gt;&lt;br /&gt;
&amp;lt;/jmolApplet&amp;gt;&amp;lt;/jmol&amp;gt;&lt;br /&gt;
&lt;br /&gt;
==Aromaticity==&lt;br /&gt;
&lt;br /&gt;
===Benzene===&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;Calculation type&amp;lt;/b&amp;gt;: Optimisation&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;Calculation Method&amp;lt;/b&amp;gt;: B3LYP&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;Basis set&amp;lt;/b&amp;gt;: 6-31G(d,p) &lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Summary table&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
[[file:Hyc116_c6h6_summarytable.png]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Items table&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;pre&amp;gt;&lt;br /&gt;
Item               Value     Threshold  Converged?&lt;br /&gt;
 Maximum Force            0.000193     0.000450     YES&lt;br /&gt;
 RMS     Force            0.000079     0.000300     YES&lt;br /&gt;
 Maximum Displacement     0.000830     0.001800     YES&lt;br /&gt;
 RMS     Displacement     0.000294     0.001200     YES&lt;br /&gt;
&amp;lt;/pre&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Frequency log file&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
[[Media:HYC116_C6H6_FREQ.LOG]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Frequencies&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;pre&amp;gt;&lt;br /&gt;
Low frequencies ---   -3.5606   -3.5606   -0.0089   -0.0043   -0.0043   10.0905&lt;br /&gt;
Low frequencies ---  413.9582  413.9582  621.1416&lt;br /&gt;
&amp;lt;/pre&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;jmol of C&amp;lt;sub&amp;gt;6&amp;lt;/sub&amp;gt;H&amp;lt;sub&amp;gt;6&amp;lt;/sub&amp;gt;&#039;&#039;&#039;&lt;br /&gt;
&amp;lt;jmol&amp;gt;&amp;lt;jmolApplet&amp;gt;&lt;br /&gt;
  &amp;lt;title&amp;gt;optimised Benzene&amp;lt;/title&amp;gt;&lt;br /&gt;
  &amp;lt;color&amp;gt;black&amp;lt;/color&amp;gt;&lt;br /&gt;
  &amp;lt;size&amp;gt;200&amp;lt;/size&amp;gt;&lt;br /&gt;
  &amp;lt;uploadedFileContents&amp;gt;HYC116_C6H6_FREQ.LOG&amp;lt;/uploadedFileContents&amp;gt;&lt;br /&gt;
&amp;lt;/jmolApplet&amp;gt;&amp;lt;/jmol&amp;gt;&lt;br /&gt;
&lt;br /&gt;
===Borazine===&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;Calculation type&amp;lt;/b&amp;gt;: Optimisation&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;Calculation Method&amp;lt;/b&amp;gt;: B3LYP&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;Basis set&amp;lt;/b&amp;gt;: 6-31G(d,p) &lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Summary table&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
[[file:Hyc116_borazine_summarytable.png]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Items table&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;pre&amp;gt;&lt;br /&gt;
Item               Value     Threshold  Converged?&lt;br /&gt;
 Maximum Force            0.000085     0.000450     YES&lt;br /&gt;
 RMS     Force            0.000033     0.000300     YES&lt;br /&gt;
 Maximum Displacement     0.000250     0.001800     YES&lt;br /&gt;
 RMS     Displacement     0.000074     0.001200     YES&lt;br /&gt;
&amp;lt;/pre&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Frequency log file&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
[[Media:HYC116_BORAZINE_FREQ.LOG]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Frequencies&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;pre&amp;gt;&lt;br /&gt;
Low frequencies ---  -12.6626  -12.6626   -8.9272   -0.0211   -0.0104   -0.0104&lt;br /&gt;
Low frequencies ---  289.1112  289.1112  403.8613&lt;br /&gt;
&amp;lt;/pre&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;jmol of Borazine&#039;&#039;&#039;&lt;br /&gt;
&amp;lt;jmol&amp;gt;&amp;lt;jmolApplet&amp;gt;&lt;br /&gt;
  &amp;lt;title&amp;gt;optimised Borazine&amp;lt;/title&amp;gt;&lt;br /&gt;
  &amp;lt;color&amp;gt;black&amp;lt;/color&amp;gt;&lt;br /&gt;
  &amp;lt;size&amp;gt;200&amp;lt;/size&amp;gt;&lt;br /&gt;
  &amp;lt;uploadedFileContents&amp;gt;HYC116_BORAZINE_FREQ.LOG&amp;lt;/uploadedFileContents&amp;gt;&lt;br /&gt;
&amp;lt;/jmolApplet&amp;gt;&amp;lt;/jmol&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
===Charge distribution===&lt;br /&gt;
&lt;br /&gt;
An NBO charge analysis was carried out on both the optimised benzene and borazine. Visualisations of the charge distribution are shown in the table below, with the colour range going from -1.102 to 1.102 for both molecule. This large scale was chosen as it allows direct comparison of the charge on any atoms in these two molecules and shows the relative magnitude of charges on all these atoms. Negative charges are shown in red, and positive charges are shown in green. A neutral charge is displayed in black, so the smaller a charge is (positive or negative), the darker its colour representation is. Larger charges are shown in brighter colours. The charges are also displayed on the atoms as numbers with a neutral charge being zero. Negative charges are shown as negative number and positive charges are shown as positive numbers. &lt;br /&gt;
&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot;&lt;br /&gt;
!&lt;br /&gt;
!Benzene&lt;br /&gt;
!Borazine&lt;br /&gt;
|-&lt;br /&gt;
!Visualisation of charge distribution&lt;br /&gt;
|[[File:Hyc116_benzene_charge_distribution1.png|500x500px|thumb|centre|Charge distribution of Benzene visualisation]]&lt;br /&gt;
|[[File:Hyc116_borazine_charge_distribution1.png|500x500px|thumb|centre|Charge distribution of Borazine visualisation]]&lt;br /&gt;
|-&lt;br /&gt;
!Charge &lt;br /&gt;
|Carbon: -0.239&lt;br /&gt;
&lt;br /&gt;
Hydrogen: 0.239&lt;br /&gt;
|Nitrogen: -1.102 &lt;br /&gt;
&lt;br /&gt;
Boron: 0.747&lt;br /&gt;
&lt;br /&gt;
Hydrogen (bonded to N): 0.432&lt;br /&gt;
&lt;br /&gt;
Hydrogen (bonded to B): -0.077&lt;br /&gt;
|-&lt;br /&gt;
!Discussion&lt;br /&gt;
|From the visualisation, it is shown that there is a slightly negative charge on the carbon atoms, and a positive charge of the same magnitude on the hydrogen atoms. All the carbon atoms have the same charge as they are in identical environments. The same applies to all the hydrogen atoms. This is due to the highly symmetrical structure of benzene. Since the same colour scale was used for both benzene and borazine, and the charges are much smaller in magnitude on atoms in benzene than atoms on borazine, the colours on the charge distribution visualisation is much darker. &lt;br /&gt;
|From the colours displayed on the charge distribution visualisation as well as the charge values, it is shown that nitrogen has a relatively large negative charge, while boron has a positive charge. This is due to the difference in electrogenativity between these atoms: nitrogen atoms are more electronegative than boron and tends to attract electrons towards themselves. It is worth noting that the hydrogen atoms do not all have the same charge. The hydrogen atoms bonded to boron have a slightly negative charge, and the ones bonded to nitrogen have a small positive charge. &lt;br /&gt;
&lt;br /&gt;
The fact that the same colour scale was used for both molecules comes in helpful here. It allows the charges on atoms to be compared directly. For example, just from looking at the colours, one can tell that or example, even though both carbon and nitrogen are electronegative, nitrogen is much more electronegative, which is quantitatively shown by Pauling&#039;s electronegativity scale.&lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
===Comparative MOs of Benzene and Borazine===&lt;br /&gt;
&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot;&lt;br /&gt;
!&lt;br /&gt;
!Benzene&lt;br /&gt;
!Borazine&lt;br /&gt;
!Comparison and Discussion&lt;br /&gt;
|-&lt;br /&gt;
!1st comparative pair&lt;br /&gt;
|[[File:Hyc116_benzene_1st_MO_pair_7.png|200x200px|centre]]&lt;br /&gt;
|[[File:Hyc116_borazine_1st_MO_pair_level9.png|200x200px|centre]]&lt;br /&gt;
|MO 9 of both benzene and borazine are comparable. They both show delocalised molecular orbital with an overall bonding character. There is a nodal plane across the molecular orbitals for both benzene and borazine. For benzene, there is contribution from all the carbon and hydrogen s orbitals. Moreover, the molecular orbitals are symmetric to their counterpart of opposite phase. That is not the case for borazine; they are less symmetric in borazine. Nitrogen atoms are more electronegative than boron atoms and pull electron density towards themselves, resulting in a larger MO. There is contribution from all the boron and nitrogen s orbitals, and three of the hydrogen s orbitals, though not all of them. &lt;br /&gt;
|-&lt;br /&gt;
!2nd comparative pair&lt;br /&gt;
|[[File:Hyc116_benzene_2nd_MO_pair_10.png|200x200px|centre]]&lt;br /&gt;
|[[File:Hyc116_borazine_2nd_MO_pair_level11.png|200x200px|centre]]&lt;br /&gt;
|&lt;br /&gt;
|-&lt;br /&gt;
!3rd comparative pair&lt;br /&gt;
|[[File:Hyc116_benzene_3rd_MO_pair_21.png|200x200px|centre]]&lt;br /&gt;
|[[File:Hyc116_borazine_3rd_MO_pair_level21.png|200x200px|centre]]&lt;br /&gt;
|&lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
===Aromaticity: some theories===&lt;br /&gt;
&lt;br /&gt;
==References==&lt;/div&gt;</summary>
		<author><name>Hyc116</name></author>
	</entry>
	<entry>
		<id>https://chemwiki.ch.ic.ac.uk/index.php?title=MO_hyc116&amp;diff=730172</id>
		<title>MO hyc116</title>
		<link rel="alternate" type="text/html" href="https://chemwiki.ch.ic.ac.uk/index.php?title=MO_hyc116&amp;diff=730172"/>
		<updated>2018-05-24T17:37:53Z</updated>

		<summary type="html">&lt;p&gt;Hyc116: &lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;==BH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;==&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;Calculation type&amp;lt;/b&amp;gt;: Optimisation&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;Calculation Method&amp;lt;/b&amp;gt;: B3LYP&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;Basis set&amp;lt;/b&amp;gt;: 6-31G(d,p) &lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Summary table&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
[[file:Hyc116_bh3_631g_opt_summarytable.png]]&lt;br /&gt;
&lt;br /&gt;
The above summary table was obtained after the 2nd optimisation of BH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt; (after the initial optimisation using the 3-21G basis set). Notice how the symmetry is incorrect and shown as Cs. This is because the symmetry was manually broken at the beginning by changing the bond length of B-H bonds. The point group was manually adjusted and the molecule was optimised again before the frequency analysis and the new summary table is attached below.&lt;br /&gt;
&lt;br /&gt;
[[file:Hyc116_bh3_correctsummarytable.png]]&lt;br /&gt;
&lt;br /&gt;
The above summary table was obtained from the optimisation after adjusting the symmetry. The point shown in this summary table is D&amp;lt;sub&amp;gt;3h&amp;lt;/sub&amp;gt;, which is the correct for BH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;. &lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Items table&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
Below is the items table taken from the optimisation with the correct point group.&lt;br /&gt;
&lt;br /&gt;
&amp;lt;pre&amp;gt;&lt;br /&gt;
Item               Value     Threshold  Converged?&lt;br /&gt;
 Maximum Force            0.000015     0.000450     YES&lt;br /&gt;
 RMS     Force            0.000010     0.000300     YES&lt;br /&gt;
 Maximum Displacement     0.000058     0.001800     YES&lt;br /&gt;
 RMS     Displacement     0.000038     0.001200     YES&lt;br /&gt;
&amp;lt;/pre&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Frequency log file&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
[[Media:HYC116 BH3 FREQ.LOG]] &lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Frequencies&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;pre&amp;gt;&lt;br /&gt;
Low frequencies ---  -10.3498   -3.4492   -1.2454   -0.0055    0.4779    3.2165&lt;br /&gt;
Low frequencies --- 1162.9519 1213.1527 1213.1554&lt;br /&gt;
&amp;lt;/pre&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;jmol of BH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;&#039;&#039;&#039;&lt;br /&gt;
&amp;lt;jmol&amp;gt;&amp;lt;jmolApplet&amp;gt;&lt;br /&gt;
  &amp;lt;title&amp;gt;optimised BH3&amp;lt;/title&amp;gt;&lt;br /&gt;
  &amp;lt;color&amp;gt;black&amp;lt;/color&amp;gt;&lt;br /&gt;
  &amp;lt;size&amp;gt;200&amp;lt;/size&amp;gt;&lt;br /&gt;
  &amp;lt;uploadedFileContents&amp;gt;HYC116_BH3_FREQ.LOG&amp;lt;/uploadedFileContents&amp;gt;&lt;br /&gt;
&amp;lt;/jmolApplet&amp;gt;&amp;lt;/jmol&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
===Vibrational spectrum===&lt;br /&gt;
&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot;&lt;br /&gt;
!wavenumber (cm&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;)&lt;br /&gt;
!Intensity (arbitrary units)&lt;br /&gt;
!symmetry&lt;br /&gt;
!IR active?&lt;br /&gt;
!type&lt;br /&gt;
|-&lt;br /&gt;
|1163&lt;br /&gt;
|93&lt;br /&gt;
|A&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;&#039; &#039;&lt;br /&gt;
|Yes&lt;br /&gt;
|Out of plane bend&lt;br /&gt;
|-&lt;br /&gt;
|1213&lt;br /&gt;
|14&lt;br /&gt;
|E&#039;&lt;br /&gt;
|Very slight&lt;br /&gt;
|Bend&lt;br /&gt;
|-&lt;br /&gt;
|1213&lt;br /&gt;
|14&lt;br /&gt;
|E&#039;&lt;br /&gt;
|Very slight&lt;br /&gt;
|Bend&lt;br /&gt;
|-&lt;br /&gt;
|2582&lt;br /&gt;
|0&lt;br /&gt;
|A&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;&#039;&lt;br /&gt;
|No&lt;br /&gt;
|Symmetric stretch&lt;br /&gt;
|-&lt;br /&gt;
|2716&lt;br /&gt;
|126&lt;br /&gt;
|E&#039;&lt;br /&gt;
|Yes&lt;br /&gt;
|Asymmetric stretch&lt;br /&gt;
|-&lt;br /&gt;
|2716&lt;br /&gt;
|126&lt;br /&gt;
|E&#039;&lt;br /&gt;
|Yes&lt;br /&gt;
|Asymmetric stretch&lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;IR spectrum&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
[[file:Hyc116_ir_bh3.png|400*600]]&lt;br /&gt;
&lt;br /&gt;
There are only three peaks on the IR spectrum of BH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;, despite that there are 6 vibrational modes for the molecule. As shown in the table above, the symmetric stretching mode with A1 symmetry at 2582 cm&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt; is not IR active; naturally, that vibrational mode doesn’t give a peak on the IR spectrum. As shown from the table, two pairs of vibrational modes, the bond angle deformation/bend at 1213 cm&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt; and the asymmetric bond stretch at 2716 cm&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;, are degenerate with the symmetry label E. This means that they have the same energy, and hence give the same wavenumber on the IR spectrum. Each pair of degenerate vibrational modes give rise to one peak. This leaves three peaks, as confirmed by the IR spectrum above.&lt;br /&gt;
&lt;br /&gt;
===Molecular orbitals of BH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;===&lt;br /&gt;
&lt;br /&gt;
[[file:hyc116_bh3_MO_diagram.png]]&lt;br /&gt;
&lt;br /&gt;
The above molecular orbital diagram was taken from Dr Patricia Hunt&#039;s &amp;lt;i&amp;gt;Lecture 4 Tutorial Problem Model Answers&amp;lt;/i&amp;gt;. . Diagrams of the &amp;quot;real&amp;quot; MOs were obtained from Gaussian.&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
There is no significant difference between the LCAO MOs and the real ones. Features such as orbital phases are shown clearly on both the LCAO MOs and the real MOs, illustrating the bonding/anti-bonding characters of the molecular orbitals. This suggests that the the qualitative MO theory is highly accurate and useful when studying the molecular orbitals of molecules.&lt;br /&gt;
&lt;br /&gt;
==Associated energies: ammonium borane==&lt;br /&gt;
&lt;br /&gt;
===NH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;===&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;Calculation type&amp;lt;/b&amp;gt;: Optimisation&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;Calculation Method&amp;lt;/b&amp;gt;: B3LYP&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;Basis set&amp;lt;/b&amp;gt;: 6-31G(d,p) &lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Summary table&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
[[file:Hyc116_nh3_631g_summarytable.png]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Items table&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;pre&amp;gt;&lt;br /&gt;
Item               Value     Threshold  Converged?&lt;br /&gt;
 Maximum Force            0.000006     0.000450     YES&lt;br /&gt;
 RMS     Force            0.000004     0.000300     YES&lt;br /&gt;
 Maximum Displacement     0.000012     0.001800     YES&lt;br /&gt;
 RMS     Displacement     0.000008     0.001200     YES&lt;br /&gt;
&amp;lt;/pre&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Frequency log file&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
[[Media:HYC116_NH3_FREQ.LOG]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Frequencies&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;pre&amp;gt;&lt;br /&gt;
Low frequencies ---   -8.5646   -8.5588   -0.0047    0.0454    0.1784   26.4183&lt;br /&gt;
Low frequencies --- 1089.7603 1694.1865 1694.1865&lt;br /&gt;
&amp;lt;/pre&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;jmol of NH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;&#039;&#039;&#039;&lt;br /&gt;
&amp;lt;jmol&amp;gt;&amp;lt;jmolApplet&amp;gt;&lt;br /&gt;
  &amp;lt;title&amp;gt;optimised NH3&amp;lt;/title&amp;gt;&lt;br /&gt;
  &amp;lt;color&amp;gt;black&amp;lt;/color&amp;gt;&lt;br /&gt;
  &amp;lt;size&amp;gt;200&amp;lt;/size&amp;gt;&lt;br /&gt;
  &amp;lt;uploadedFileContents&amp;gt;HYC116_NH3_FREQ.LOG&amp;lt;/uploadedFileContents&amp;gt;&lt;br /&gt;
&amp;lt;/jmolApplet&amp;gt;&amp;lt;/jmol&amp;gt;&lt;br /&gt;
&lt;br /&gt;
===NH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;BH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;===&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;Calculation type&amp;lt;/b&amp;gt;: Optimisation&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;Calculation Method&amp;lt;/b&amp;gt;: B3LYP&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;Basis set&amp;lt;/b&amp;gt;: 6-31G(d,p) &lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Summary table&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
[[file:Hyc116_nh3bh3_631g_summarytable.png]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Items table&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;pre&amp;gt;&lt;br /&gt;
Item               Value     Threshold  Converged?&lt;br /&gt;
 Maximum Force            0.000123     0.000450     YES&lt;br /&gt;
 RMS     Force            0.000058     0.000300     YES&lt;br /&gt;
 Maximum Displacement     0.000515     0.001800     YES&lt;br /&gt;
 RMS     Displacement     0.000296     0.001200     YES&lt;br /&gt;
&amp;lt;/pre&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Frequency log file&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
[[Media:HYC116_NH3BH3_FREQ.LOG]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Frequencies&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;pre&amp;gt;&lt;br /&gt;
Low frequencies ---   -0.0014   -0.0011   -0.0006    6.9624   20.4518   43.5542&lt;br /&gt;
Low frequencies ---  266.4530  632.2458  639.0504&lt;br /&gt;
&amp;lt;/pre&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;jmol of NH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;BH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;&#039;&#039;&#039;&lt;br /&gt;
&amp;lt;jmol&amp;gt;&amp;lt;jmolApplet&amp;gt;&lt;br /&gt;
  &amp;lt;title&amp;gt;optimised NH3BH3&amp;lt;/title&amp;gt;&lt;br /&gt;
  &amp;lt;color&amp;gt;black&amp;lt;/color&amp;gt;&lt;br /&gt;
  &amp;lt;size&amp;gt;200&amp;lt;/size&amp;gt;&lt;br /&gt;
  &amp;lt;uploadedFileContents&amp;gt;HYC116_NH3BH3_FREQ.LOG&amp;lt;/uploadedFileContents&amp;gt;&lt;br /&gt;
&amp;lt;/jmolApplet&amp;gt;&amp;lt;/jmol&amp;gt;&lt;br /&gt;
&lt;br /&gt;
===Association energy===&lt;br /&gt;
&lt;br /&gt;
E(BH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;) (using the optimisation with the correct symmetry) = -26.61532363 a.u. = &amp;lt;b&amp;gt;-26.61532 a.u. (5 d.p.)&amp;lt;/b&amp;gt;&lt;br /&gt;
&lt;br /&gt;
E(NH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;) = -56.55776873 a.u. = &amp;lt;b&amp;gt;-56.55777 a.u. (5 d.p.)&amp;lt;/b&amp;gt;&lt;br /&gt;
&lt;br /&gt;
E(NH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;BH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;) = -83.22468893 a.u. = &amp;lt;b&amp;gt;-83.22469 a.u. (5 d.p.)&amp;lt;/b&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
Carrying out calculations using numbers which has already been rounded up can possibly result in errors in the last digit. Hence, here the calculations were carried out using the numbers provided from the optimisations (i.e. with more decimal places than necessary); the answer was then rounded up to the desired accuracy. &lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
ΔE = E(NH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;BH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;)-[E(NH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;)+E(BH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;)]&lt;br /&gt;
&lt;br /&gt;
ΔE = -83.22468893 - (-56.55776873 + -26.61532363) = -0.05159657 a.u. &lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;ΔE = -0.05160 a.u. (5 d.p.)&amp;lt;/b&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Converting energy from a.u. to kJ/mol&#039;&#039;&#039;&lt;br /&gt;
An atomic unit for energy is Hartree, which is equal to 2625.5 kJ/mol. &lt;br /&gt;
&lt;br /&gt;
So ΔE in kJ/mol = -0.05159657 * 2625.5 = -135.466794535 kJ/mol&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;ΔE = -135 kJ/mol (nearest integer)&amp;lt;/b&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
The energy difference calculated above comes from the formation of the B-N dative bond. It is a relatively weak bond. According to a bond energy data sheet provided by the University of California,  the bond energy of the C-C bond of an ethane molecule is 368 kJ/mol. This is a fair comparison to the NH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;BH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt; molecule as the two molecules have the same structure, only with the carbon atoms on ethane swapped for Boron and Nitrogen in NH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;BH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;&lt;br /&gt;
&lt;br /&gt;
==Using a mixture of basis-sets and pseudo-potentials==&lt;br /&gt;
&lt;br /&gt;
===BBr&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;===&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;Calculation type&amp;lt;/b&amp;gt;: Optimisation&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;Calculation Method&amp;lt;/b&amp;gt;: B3LYP&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;Basis set&amp;lt;/b&amp;gt;: Boron: 6-31G(d,p) ; Br: LANL2DZ&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
Larger calculations are often sent to a web-server to run on a high-performance computer instead of a desktop. In order to experience and learn to use a web-server, the optimisation and the frequency analysis for BBr&amp;lt;sub&amp;gt;3&amp;lt;/sub were both sent and done on a server instead of the desktop. The calculation results were downloaded from the web-server once they were finished.   &lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Summary table&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
[[file:Hyc116_bbr3_opt_summarytable.png]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Items table&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;pre&amp;gt;&lt;br /&gt;
Item               Value     Threshold  Converged?&lt;br /&gt;
 Maximum Force            0.000008     0.000450     YES&lt;br /&gt;
 RMS     Force            0.000005     0.000300     YES&lt;br /&gt;
 Maximum Displacement     0.000036     0.001800     YES&lt;br /&gt;
 RMS     Displacement     0.000023     0.001200     YES&lt;br /&gt;
&amp;lt;/pre&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Frequency log file&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
[[Media:Hyc116_bbr3_freq.log]]&lt;br /&gt;
&lt;br /&gt;
Attached above is the frequency file saved onto the computer from the SCAN server portal. The frequency file was also published on the chemistry database DSpace. {{DOI|10042/202442}}&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Frequencies&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;pre&amp;gt;&lt;br /&gt;
Low frequencies ---   -0.0137   -0.0064   -0.0046    2.4315    2.4315    4.8421&lt;br /&gt;
Low frequencies ---  155.9631  155.9651  267.7052&lt;br /&gt;
&amp;lt;/pre&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;jmol of BBr&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;&#039;&#039;&#039;&lt;br /&gt;
&amp;lt;jmol&amp;gt;&amp;lt;jmolApplet&amp;gt;&lt;br /&gt;
  &amp;lt;title&amp;gt;optimised BBr3&amp;lt;/title&amp;gt;&lt;br /&gt;
  &amp;lt;color&amp;gt;black&amp;lt;/color&amp;gt;&lt;br /&gt;
  &amp;lt;size&amp;gt;200&amp;lt;/size&amp;gt;&lt;br /&gt;
  &amp;lt;uploadedFileContents&amp;gt;Hyc116_bbr3_freq.log&amp;lt;/uploadedFileContents&amp;gt;&lt;br /&gt;
&amp;lt;/jmolApplet&amp;gt;&amp;lt;/jmol&amp;gt;&lt;br /&gt;
&lt;br /&gt;
==Aromaticity==&lt;br /&gt;
&lt;br /&gt;
===Benzene===&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;Calculation type&amp;lt;/b&amp;gt;: Optimisation&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;Calculation Method&amp;lt;/b&amp;gt;: B3LYP&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;Basis set&amp;lt;/b&amp;gt;: 6-31G(d,p) &lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Summary table&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
[[file:Hyc116_c6h6_summarytable.png]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Items table&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;pre&amp;gt;&lt;br /&gt;
Item               Value     Threshold  Converged?&lt;br /&gt;
 Maximum Force            0.000193     0.000450     YES&lt;br /&gt;
 RMS     Force            0.000079     0.000300     YES&lt;br /&gt;
 Maximum Displacement     0.000830     0.001800     YES&lt;br /&gt;
 RMS     Displacement     0.000294     0.001200     YES&lt;br /&gt;
&amp;lt;/pre&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Frequency log file&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
[[Media:HYC116_C6H6_FREQ.LOG]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Frequencies&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;pre&amp;gt;&lt;br /&gt;
Low frequencies ---   -3.5606   -3.5606   -0.0089   -0.0043   -0.0043   10.0905&lt;br /&gt;
Low frequencies ---  413.9582  413.9582  621.1416&lt;br /&gt;
&amp;lt;/pre&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;jmol of C&amp;lt;sub&amp;gt;6&amp;lt;/sub&amp;gt;H&amp;lt;sub&amp;gt;6&amp;lt;/sub&amp;gt;&#039;&#039;&#039;&lt;br /&gt;
&amp;lt;jmol&amp;gt;&amp;lt;jmolApplet&amp;gt;&lt;br /&gt;
  &amp;lt;title&amp;gt;optimised Benzene&amp;lt;/title&amp;gt;&lt;br /&gt;
  &amp;lt;color&amp;gt;black&amp;lt;/color&amp;gt;&lt;br /&gt;
  &amp;lt;size&amp;gt;200&amp;lt;/size&amp;gt;&lt;br /&gt;
  &amp;lt;uploadedFileContents&amp;gt;HYC116_C6H6_FREQ.LOG&amp;lt;/uploadedFileContents&amp;gt;&lt;br /&gt;
&amp;lt;/jmolApplet&amp;gt;&amp;lt;/jmol&amp;gt;&lt;br /&gt;
&lt;br /&gt;
===Borazine===&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;Calculation type&amp;lt;/b&amp;gt;: Optimisation&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;Calculation Method&amp;lt;/b&amp;gt;: B3LYP&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;Basis set&amp;lt;/b&amp;gt;: 6-31G(d,p) &lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Summary table&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
[[file:Hyc116_borazine_summarytable.png]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Items table&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;pre&amp;gt;&lt;br /&gt;
Item               Value     Threshold  Converged?&lt;br /&gt;
 Maximum Force            0.000085     0.000450     YES&lt;br /&gt;
 RMS     Force            0.000033     0.000300     YES&lt;br /&gt;
 Maximum Displacement     0.000250     0.001800     YES&lt;br /&gt;
 RMS     Displacement     0.000074     0.001200     YES&lt;br /&gt;
&amp;lt;/pre&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Frequency log file&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
[[Media:HYC116_BORAZINE_FREQ.LOG]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Frequencies&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;pre&amp;gt;&lt;br /&gt;
Low frequencies ---  -12.6626  -12.6626   -8.9272   -0.0211   -0.0104   -0.0104&lt;br /&gt;
Low frequencies ---  289.1112  289.1112  403.8613&lt;br /&gt;
&amp;lt;/pre&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;jmol of Borazine&#039;&#039;&#039;&lt;br /&gt;
&amp;lt;jmol&amp;gt;&amp;lt;jmolApplet&amp;gt;&lt;br /&gt;
  &amp;lt;title&amp;gt;optimised Borazine&amp;lt;/title&amp;gt;&lt;br /&gt;
  &amp;lt;color&amp;gt;black&amp;lt;/color&amp;gt;&lt;br /&gt;
  &amp;lt;size&amp;gt;200&amp;lt;/size&amp;gt;&lt;br /&gt;
  &amp;lt;uploadedFileContents&amp;gt;HYC116_BORAZINE_FREQ.LOG&amp;lt;/uploadedFileContents&amp;gt;&lt;br /&gt;
&amp;lt;/jmolApplet&amp;gt;&amp;lt;/jmol&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
===Charge distribution===&lt;br /&gt;
&lt;br /&gt;
An NBO charge analysis was carried out on both the optimised benzene and borazine. Visualisations of the charge distribution are shown in the table below, with the colour range going from -1.102 to 1.102 for both molecule. This large scale was chosen as it allows direct comparison of the charge on any atoms in these two molecules and shows the relative magnitude of charges on all these atoms. Negative charges are shown in red, and positive charges are shown in green. A neutral charge is displayed in black, so the smaller a charge is (positive or negative), the darker its colour representation is. Larger charges are shown in brighter colours. The charges are also displayed on the atoms as numbers with a neutral charge being zero. Negative charges are shown as negative number and positive charges are shown as positive numbers. &lt;br /&gt;
&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot;&lt;br /&gt;
!&lt;br /&gt;
!Benzene&lt;br /&gt;
!Borazine&lt;br /&gt;
|-&lt;br /&gt;
!Visualisation of charge distribution&lt;br /&gt;
|[[File:Hyc116_benzene_charge_distribution1.png|500x500px|thumb|centre|Charge distribution of Benzene visualisation]]&lt;br /&gt;
|[[File:Hyc116_borazine_charge_distribution1.png|500x500px|thumb|centre|Charge distribution of Borazine visualisation]]&lt;br /&gt;
|-&lt;br /&gt;
!Charge &lt;br /&gt;
|Carbon: -0.239&lt;br /&gt;
&lt;br /&gt;
Hydrogen: 0.239&lt;br /&gt;
|Nitrogen: -1.102 &lt;br /&gt;
&lt;br /&gt;
Boron: 0.747&lt;br /&gt;
&lt;br /&gt;
Hydrogen (bonded to N): 0.432&lt;br /&gt;
&lt;br /&gt;
Hydrogen (bonded to B): -0.077&lt;br /&gt;
|-&lt;br /&gt;
!Discussion&lt;br /&gt;
|From the visualisation, it is shown that there is a slightly negative charge on the carbon atoms, and a positive charge of the same magnitude on the hydrogen atoms. All the carbon atoms have the same charge as they are in identical environments. The same applies to all the hydrogen atoms. This is due to the highly symmetrical structure of benzene. Since the same colour scale was used for both benzene and borazine, and the charges are much smaller in magnitude on atoms in benzene than atoms on borazine, the colours on the charge distribution visualisation is much darker. &lt;br /&gt;
|From the colours displayed on the charge distribution visualisation as well as the charge values, it is shown that nitrogen has a relatively large negative charge, while boron has a positive charge. This is due to the difference in electrogenativity between these atoms: nitrogen atoms are more electronegative than boron and tends to attract electrons towards themselves. It is worth noting that the hydrogen atoms do not all have the same charge. The hydrogen atoms bonded to boron have a slightly negative charge, and the ones bonded to nitrogen have a small positive charge. &lt;br /&gt;
&lt;br /&gt;
The fact that the same colour scale was used for both molecules comes in helpful here. It allows the charges on atoms to be compared directly. For example, just from looking at the colours, one can tell that or example, even though both carbon and nitrogen are electronegative, nitrogen is much more electronegative, which is quantitatively shown by Pauling&#039;s electronegativity scale.&lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
===Comparative MOs of Benzene and Borazine===&lt;br /&gt;
&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot;&lt;br /&gt;
!&lt;br /&gt;
!Benzene&lt;br /&gt;
!Borazine&lt;br /&gt;
!Comparison and Discussion&lt;br /&gt;
|-&lt;br /&gt;
!1st comparative pair&lt;br /&gt;
|[[File:Hyc116_benzene_1st_MO_pair_7.png|200x200px|centre]]&lt;br /&gt;
|[[File:Hyc116_borazine_1st_MO_pair_level9.png|200x200px|centre]]&lt;br /&gt;
|MO 9 of both benzene and borazine are comparable. They both show delocalised molecular orbital with an overall bonding character. There is a nodal plane across the molecular orbitals for both benzene and borazine. For benzene, there is contribution from all the carbon and hydrogen s orbitals. Moreover, the molecular orbitals are symmetric to their counterpart of opposite phase. That is not the case for borazine; they are less symmetric in borazine. Nitrogen atoms are more electronegative than boron atoms and pull electron density towards themselves, resulting in a larger MO. There is contribution from all the boron and nitrogen s orbitals, and three of the hydrogen s orbitals, though not all of them. &lt;br /&gt;
|-&lt;br /&gt;
!2nd comparative pair&lt;br /&gt;
|[[File:Hyc116_benzene_2nd_MO_pair_10.png|200x200px|centre]]&lt;br /&gt;
|[[File:Hyc116_borazine_2nd_MO_pair_level11.png|200x200px|centre]]&lt;br /&gt;
|&lt;br /&gt;
|-&lt;br /&gt;
!3rd comparative pair&lt;br /&gt;
|[[File:Hyc116_benzene_3rd_MO_pair_21.png|200x200px|centre]]&lt;br /&gt;
|[[File:Hyc116_borazine_3rd_MO_pair_level21.png|200x200px|centre]]&lt;br /&gt;
|&lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
===Aromaticity: some theories===&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
== References ==&lt;/div&gt;</summary>
		<author><name>Hyc116</name></author>
	</entry>
	<entry>
		<id>https://chemwiki.ch.ic.ac.uk/index.php?title=MO_hyc116&amp;diff=730169</id>
		<title>MO hyc116</title>
		<link rel="alternate" type="text/html" href="https://chemwiki.ch.ic.ac.uk/index.php?title=MO_hyc116&amp;diff=730169"/>
		<updated>2018-05-24T17:37:05Z</updated>

		<summary type="html">&lt;p&gt;Hyc116: &lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;==BH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;==&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;Calculation type&amp;lt;/b&amp;gt;: Optimisation&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;Calculation Method&amp;lt;/b&amp;gt;: B3LYP&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;Basis set&amp;lt;/b&amp;gt;: 6-31G(d,p) &lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Summary table&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
[[file:Hyc116_bh3_631g_opt_summarytable.png]]&lt;br /&gt;
&lt;br /&gt;
The above summary table was obtained after the 2nd optimisation of BH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt; (after the initial optimisation using the 3-21G basis set). Notice how the symmetry is incorrect and shown as Cs. This is because the symmetry was manually broken at the beginning by changing the bond length of B-H bonds. The point group was manually adjusted and the molecule was optimised again before the frequency analysis and the new summary table is attached below.&lt;br /&gt;
&lt;br /&gt;
[[file:Hyc116_bh3_correctsummarytable.png]]&lt;br /&gt;
&lt;br /&gt;
The above summary table was obtained from the optimisation after adjusting the symmetry. The point shown in this summary table is D&amp;lt;sub&amp;gt;3h&amp;lt;/sub&amp;gt;, which is the correct for BH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;. &lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Items table&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
Below is the items table taken from the optimisation with the correct point group.&lt;br /&gt;
&lt;br /&gt;
&amp;lt;pre&amp;gt;&lt;br /&gt;
Item               Value     Threshold  Converged?&lt;br /&gt;
 Maximum Force            0.000015     0.000450     YES&lt;br /&gt;
 RMS     Force            0.000010     0.000300     YES&lt;br /&gt;
 Maximum Displacement     0.000058     0.001800     YES&lt;br /&gt;
 RMS     Displacement     0.000038     0.001200     YES&lt;br /&gt;
&amp;lt;/pre&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Frequency log file&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
[[Media:HYC116 BH3 FREQ.LOG]] &lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Frequencies&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;pre&amp;gt;&lt;br /&gt;
Low frequencies ---  -10.3498   -3.4492   -1.2454   -0.0055    0.4779    3.2165&lt;br /&gt;
Low frequencies --- 1162.9519 1213.1527 1213.1554&lt;br /&gt;
&amp;lt;/pre&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;jmol of BH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;&#039;&#039;&#039;&lt;br /&gt;
&amp;lt;jmol&amp;gt;&amp;lt;jmolApplet&amp;gt;&lt;br /&gt;
  &amp;lt;title&amp;gt;optimised BH3&amp;lt;/title&amp;gt;&lt;br /&gt;
  &amp;lt;color&amp;gt;black&amp;lt;/color&amp;gt;&lt;br /&gt;
  &amp;lt;size&amp;gt;200&amp;lt;/size&amp;gt;&lt;br /&gt;
  &amp;lt;uploadedFileContents&amp;gt;HYC116_BH3_FREQ.LOG&amp;lt;/uploadedFileContents&amp;gt;&lt;br /&gt;
&amp;lt;/jmolApplet&amp;gt;&amp;lt;/jmol&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
===Vibrational spectrum===&lt;br /&gt;
&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot;&lt;br /&gt;
!wavenumber (cm&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;)&lt;br /&gt;
!Intensity (arbitrary units)&lt;br /&gt;
!symmetry&lt;br /&gt;
!IR active?&lt;br /&gt;
!type&lt;br /&gt;
|-&lt;br /&gt;
|1163&lt;br /&gt;
|93&lt;br /&gt;
|A&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;&#039; &#039;&lt;br /&gt;
|Yes&lt;br /&gt;
|Out of plane bend&lt;br /&gt;
|-&lt;br /&gt;
|1213&lt;br /&gt;
|14&lt;br /&gt;
|E&#039;&lt;br /&gt;
|Very slight&lt;br /&gt;
|Bend&lt;br /&gt;
|-&lt;br /&gt;
|1213&lt;br /&gt;
|14&lt;br /&gt;
|E&#039;&lt;br /&gt;
|Very slight&lt;br /&gt;
|Bend&lt;br /&gt;
|-&lt;br /&gt;
|2582&lt;br /&gt;
|0&lt;br /&gt;
|A&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;&#039;&lt;br /&gt;
|No&lt;br /&gt;
|Symmetric stretch&lt;br /&gt;
|-&lt;br /&gt;
|2716&lt;br /&gt;
|126&lt;br /&gt;
|E&#039;&lt;br /&gt;
|Yes&lt;br /&gt;
|Asymmetric stretch&lt;br /&gt;
|-&lt;br /&gt;
|2716&lt;br /&gt;
|126&lt;br /&gt;
|E&#039;&lt;br /&gt;
|Yes&lt;br /&gt;
|Asymmetric stretch&lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;IR spectrum&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
[[file:Hyc116_ir_bh3.png|400*600]]&lt;br /&gt;
&lt;br /&gt;
There are only three peaks on the IR spectrum of BH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;, despite that there are 6 vibrational modes for the molecule. As shown in the table above, the symmetric stretching mode with A1 symmetry at 2582 cm&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt; is not IR active; naturally, that vibrational mode doesn’t give a peak on the IR spectrum. As shown from the table, two pairs of vibrational modes, the bond angle deformation/bend at 1213 cm&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt; and the asymmetric bond stretch at 2716 cm&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;, are degenerate with the symmetry label E. This means that they have the same energy, and hence give the same wavenumber on the IR spectrum. Each pair of degenerate vibrational modes give rise to one peak. This leaves three peaks, as confirmed by the IR spectrum above.&lt;br /&gt;
&lt;br /&gt;
===Molecular orbitals of BH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;===&lt;br /&gt;
&lt;br /&gt;
[[file:hyc116_bh3_MO_diagram.png]]&lt;br /&gt;
&lt;br /&gt;
The above molecular orbital diagram was taken from Dr Patricia Hunt&#039;s &amp;lt;i&amp;gt;Lecture 4 Tutorial Problem Model Answers&amp;lt;/i&amp;gt;. . Diagrams of the &amp;quot;real&amp;quot; MOs were obtained from Gaussian.&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
There is no significant difference between the LCAO MOs and the real ones. Features such as orbital phases are shown clearly on both the LCAO MOs and the real MOs, illustrating the bonding/anti-bonding characters of the molecular orbitals. This suggests that the the qualitative MO theory is highly accurate and useful when studying the molecular orbitals of molecules.&lt;br /&gt;
&lt;br /&gt;
==Associated energies: ammonium borane==&lt;br /&gt;
&lt;br /&gt;
===NH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;===&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;Calculation type&amp;lt;/b&amp;gt;: Optimisation&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;Calculation Method&amp;lt;/b&amp;gt;: B3LYP&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;Basis set&amp;lt;/b&amp;gt;: 6-31G(d,p) &lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Summary table&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
[[file:Hyc116_nh3_631g_summarytable.png]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Items table&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;pre&amp;gt;&lt;br /&gt;
Item               Value     Threshold  Converged?&lt;br /&gt;
 Maximum Force            0.000006     0.000450     YES&lt;br /&gt;
 RMS     Force            0.000004     0.000300     YES&lt;br /&gt;
 Maximum Displacement     0.000012     0.001800     YES&lt;br /&gt;
 RMS     Displacement     0.000008     0.001200     YES&lt;br /&gt;
&amp;lt;/pre&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Frequency log file&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
[[Media:HYC116_NH3_FREQ.LOG]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Frequencies&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;pre&amp;gt;&lt;br /&gt;
Low frequencies ---   -8.5646   -8.5588   -0.0047    0.0454    0.1784   26.4183&lt;br /&gt;
Low frequencies --- 1089.7603 1694.1865 1694.1865&lt;br /&gt;
&amp;lt;/pre&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;jmol of NH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;&#039;&#039;&#039;&lt;br /&gt;
&amp;lt;jmol&amp;gt;&amp;lt;jmolApplet&amp;gt;&lt;br /&gt;
  &amp;lt;title&amp;gt;optimised NH3&amp;lt;/title&amp;gt;&lt;br /&gt;
  &amp;lt;color&amp;gt;black&amp;lt;/color&amp;gt;&lt;br /&gt;
  &amp;lt;size&amp;gt;200&amp;lt;/size&amp;gt;&lt;br /&gt;
  &amp;lt;uploadedFileContents&amp;gt;HYC116_NH3_FREQ.LOG&amp;lt;/uploadedFileContents&amp;gt;&lt;br /&gt;
&amp;lt;/jmolApplet&amp;gt;&amp;lt;/jmol&amp;gt;&lt;br /&gt;
&lt;br /&gt;
===NH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;BH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;===&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;Calculation type&amp;lt;/b&amp;gt;: Optimisation&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;Calculation Method&amp;lt;/b&amp;gt;: B3LYP&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;Basis set&amp;lt;/b&amp;gt;: 6-31G(d,p) &lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Summary table&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
[[file:Hyc116_nh3bh3_631g_summarytable.png]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Items table&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;pre&amp;gt;&lt;br /&gt;
Item               Value     Threshold  Converged?&lt;br /&gt;
 Maximum Force            0.000123     0.000450     YES&lt;br /&gt;
 RMS     Force            0.000058     0.000300     YES&lt;br /&gt;
 Maximum Displacement     0.000515     0.001800     YES&lt;br /&gt;
 RMS     Displacement     0.000296     0.001200     YES&lt;br /&gt;
&amp;lt;/pre&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Frequency log file&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
[[Media:HYC116_NH3BH3_FREQ.LOG]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Frequencies&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;pre&amp;gt;&lt;br /&gt;
Low frequencies ---   -0.0014   -0.0011   -0.0006    6.9624   20.4518   43.5542&lt;br /&gt;
Low frequencies ---  266.4530  632.2458  639.0504&lt;br /&gt;
&amp;lt;/pre&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;jmol of NH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;BH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;&#039;&#039;&#039;&lt;br /&gt;
&amp;lt;jmol&amp;gt;&amp;lt;jmolApplet&amp;gt;&lt;br /&gt;
  &amp;lt;title&amp;gt;optimised NH3BH3&amp;lt;/title&amp;gt;&lt;br /&gt;
  &amp;lt;color&amp;gt;black&amp;lt;/color&amp;gt;&lt;br /&gt;
  &amp;lt;size&amp;gt;200&amp;lt;/size&amp;gt;&lt;br /&gt;
  &amp;lt;uploadedFileContents&amp;gt;HYC116_NH3BH3_FREQ.LOG&amp;lt;/uploadedFileContents&amp;gt;&lt;br /&gt;
&amp;lt;/jmolApplet&amp;gt;&amp;lt;/jmol&amp;gt;&lt;br /&gt;
&lt;br /&gt;
===Association energy===&lt;br /&gt;
&lt;br /&gt;
E(BH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;) (using the optimisation with the correct symmetry) = -26.61532363 a.u. = &amp;lt;b&amp;gt;-26.61532 a.u. (5 d.p.)&amp;lt;/b&amp;gt;&lt;br /&gt;
&lt;br /&gt;
E(NH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;) = -56.55776873 a.u. = &amp;lt;b&amp;gt;-56.55777 a.u. (5 d.p.)&amp;lt;/b&amp;gt;&lt;br /&gt;
&lt;br /&gt;
E(NH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;BH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;) = -83.22468893 a.u. = &amp;lt;b&amp;gt;-83.22469 a.u. (5 d.p.)&amp;lt;/b&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
Carrying out calculations using numbers which has already been rounded up can possibly result in errors in the last digit. Hence, here the calculations were carried out using the numbers provided from the optimisations (i.e. with more decimal places than necessary); the answer was then rounded up to the desired accuracy. &lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
ΔE = E(NH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;BH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;)-[E(NH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;)+E(BH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;)]&lt;br /&gt;
&lt;br /&gt;
ΔE = -83.22468893 - (-56.55776873 + -26.61532363) = -0.05159657 a.u. &lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;ΔE = -0.05160 a.u. (5 d.p.)&amp;lt;/b&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Converting energy from a.u. to kJ/mol&#039;&#039;&#039;&lt;br /&gt;
An atomic unit for energy is Hartree, which is equal to 2625.5 kJ/mol. &lt;br /&gt;
&lt;br /&gt;
So ΔE in kJ/mol = -0.05159657 * 2625.5 = -135.466794535 kJ/mol&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;ΔE = -135 kJ/mol (nearest integer)&amp;lt;/b&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
The energy difference calculated above comes from the formation of the B-N dative bond. It is a relatively weak bond. According to a bond energy data sheet provided by the University of California,  the bond energy of the C-C bond of an ethane molecule is 368 kJ/mol. This is a fair comparison to the NH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;BH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt; molecule as the two molecules have the same structure, only with the carbon atoms on ethane swapped for Boron and Nitrogen in NH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;BH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;&lt;br /&gt;
&lt;br /&gt;
==Using a mixture of basis-sets and pseudo-potentials==&lt;br /&gt;
&lt;br /&gt;
===BBr&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;===&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;Calculation type&amp;lt;/b&amp;gt;: Optimisation&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;Calculation Method&amp;lt;/b&amp;gt;: B3LYP&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;Basis set&amp;lt;/b&amp;gt;: Boron: 6-31G(d,p) ; Br: LANL2DZ&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
Larger calculations are often sent to a web-server to run on a high-performance computer instead of a desktop. In order to experience and learn to use a web-server, the optimisation and the frequency analysis for BBr&amp;lt;sub&amp;gt;3&amp;lt;/sub were both sent and done on a server instead of the desktop. The calculation results were downloaded from the web-server once they were finished.   &lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Summary table&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
[[file:Hyc116_bbr3_opt_summarytable.png]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Items table&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;pre&amp;gt;&lt;br /&gt;
Item               Value     Threshold  Converged?&lt;br /&gt;
 Maximum Force            0.000008     0.000450     YES&lt;br /&gt;
 RMS     Force            0.000005     0.000300     YES&lt;br /&gt;
 Maximum Displacement     0.000036     0.001800     YES&lt;br /&gt;
 RMS     Displacement     0.000023     0.001200     YES&lt;br /&gt;
&amp;lt;/pre&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Frequency log file&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
[[Media:Hyc116_bbr3_freq.log]]&lt;br /&gt;
&lt;br /&gt;
Attached above is the frequency file saved onto the computer from the SCAN server portal. The frequency file was also published on the chemistry database DSpace. {{DOI|10042/202442}}&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Frequencies&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;pre&amp;gt;&lt;br /&gt;
Low frequencies ---   -0.0137   -0.0064   -0.0046    2.4315    2.4315    4.8421&lt;br /&gt;
Low frequencies ---  155.9631  155.9651  267.7052&lt;br /&gt;
&amp;lt;/pre&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;jmol of BBr&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;&#039;&#039;&#039;&lt;br /&gt;
&amp;lt;jmol&amp;gt;&amp;lt;jmolApplet&amp;gt;&lt;br /&gt;
  &amp;lt;title&amp;gt;optimised BBr3&amp;lt;/title&amp;gt;&lt;br /&gt;
  &amp;lt;color&amp;gt;black&amp;lt;/color&amp;gt;&lt;br /&gt;
  &amp;lt;size&amp;gt;200&amp;lt;/size&amp;gt;&lt;br /&gt;
  &amp;lt;uploadedFileContents&amp;gt;Hyc116_bbr3_freq.log&amp;lt;/uploadedFileContents&amp;gt;&lt;br /&gt;
&amp;lt;/jmolApplet&amp;gt;&amp;lt;/jmol&amp;gt;&lt;br /&gt;
&lt;br /&gt;
==Aromaticity==&lt;br /&gt;
&lt;br /&gt;
===Benzene===&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;Calculation type&amp;lt;/b&amp;gt;: Optimisation&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;Calculation Method&amp;lt;/b&amp;gt;: B3LYP&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;Basis set&amp;lt;/b&amp;gt;: 6-31G(d,p) &lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Summary table&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
[[file:Hyc116_c6h6_summarytable.png]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Items table&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;pre&amp;gt;&lt;br /&gt;
Item               Value     Threshold  Converged?&lt;br /&gt;
 Maximum Force            0.000193     0.000450     YES&lt;br /&gt;
 RMS     Force            0.000079     0.000300     YES&lt;br /&gt;
 Maximum Displacement     0.000830     0.001800     YES&lt;br /&gt;
 RMS     Displacement     0.000294     0.001200     YES&lt;br /&gt;
&amp;lt;/pre&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Frequency log file&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
[[Media:HYC116_C6H6_FREQ.LOG]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Frequencies&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;pre&amp;gt;&lt;br /&gt;
Low frequencies ---   -3.5606   -3.5606   -0.0089   -0.0043   -0.0043   10.0905&lt;br /&gt;
Low frequencies ---  413.9582  413.9582  621.1416&lt;br /&gt;
&amp;lt;/pre&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;jmol of C&amp;lt;sub&amp;gt;6&amp;lt;/sub&amp;gt;H&amp;lt;sub&amp;gt;6&amp;lt;/sub&amp;gt;&#039;&#039;&#039;&lt;br /&gt;
&amp;lt;jmol&amp;gt;&amp;lt;jmolApplet&amp;gt;&lt;br /&gt;
  &amp;lt;title&amp;gt;optimised Benzene&amp;lt;/title&amp;gt;&lt;br /&gt;
  &amp;lt;color&amp;gt;black&amp;lt;/color&amp;gt;&lt;br /&gt;
  &amp;lt;size&amp;gt;200&amp;lt;/size&amp;gt;&lt;br /&gt;
  &amp;lt;uploadedFileContents&amp;gt;HYC116_C6H6_FREQ.LOG&amp;lt;/uploadedFileContents&amp;gt;&lt;br /&gt;
&amp;lt;/jmolApplet&amp;gt;&amp;lt;/jmol&amp;gt;&lt;br /&gt;
&lt;br /&gt;
===Borazine===&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;Calculation type&amp;lt;/b&amp;gt;: Optimisation&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;Calculation Method&amp;lt;/b&amp;gt;: B3LYP&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;Basis set&amp;lt;/b&amp;gt;: 6-31G(d,p) &lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Summary table&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
[[file:Hyc116_borazine_summarytable.png]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Items table&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;pre&amp;gt;&lt;br /&gt;
Item               Value     Threshold  Converged?&lt;br /&gt;
 Maximum Force            0.000085     0.000450     YES&lt;br /&gt;
 RMS     Force            0.000033     0.000300     YES&lt;br /&gt;
 Maximum Displacement     0.000250     0.001800     YES&lt;br /&gt;
 RMS     Displacement     0.000074     0.001200     YES&lt;br /&gt;
&amp;lt;/pre&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Frequency log file&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
[[Media:HYC116_BORAZINE_FREQ.LOG]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Frequencies&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;pre&amp;gt;&lt;br /&gt;
Low frequencies ---  -12.6626  -12.6626   -8.9272   -0.0211   -0.0104   -0.0104&lt;br /&gt;
Low frequencies ---  289.1112  289.1112  403.8613&lt;br /&gt;
&amp;lt;/pre&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;jmol of Borazine&#039;&#039;&#039;&lt;br /&gt;
&amp;lt;jmol&amp;gt;&amp;lt;jmolApplet&amp;gt;&lt;br /&gt;
  &amp;lt;title&amp;gt;optimised Borazine&amp;lt;/title&amp;gt;&lt;br /&gt;
  &amp;lt;color&amp;gt;black&amp;lt;/color&amp;gt;&lt;br /&gt;
  &amp;lt;size&amp;gt;200&amp;lt;/size&amp;gt;&lt;br /&gt;
  &amp;lt;uploadedFileContents&amp;gt;HYC116_BORAZINE_FREQ.LOG&amp;lt;/uploadedFileContents&amp;gt;&lt;br /&gt;
&amp;lt;/jmolApplet&amp;gt;&amp;lt;/jmol&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
===Charge distribution===&lt;br /&gt;
&lt;br /&gt;
An NBO charge analysis was carried out on both the optimised benzene and borazine. Visualisations of the charge distribution are shown in the table below, with the colour range going from -1.102 to 1.102 for both molecule. This large scale was chosen as it allows direct comparison of the charge on any atoms in these two molecules and shows the relative magnitude of charges on all these atoms. Negative charges are shown in red, and positive charges are shown in green. A neutral charge is displayed in black, so the smaller a charge is (positive or negative), the darker its colour representation is. Larger charges are shown in brighter colours. The charges are also displayed on the atoms as numbers with a neutral charge being zero. Negative charges are shown as negative number and positive charges are shown as positive numbers. &lt;br /&gt;
&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot;&lt;br /&gt;
!&lt;br /&gt;
!Benzene&lt;br /&gt;
!Borazine&lt;br /&gt;
|-&lt;br /&gt;
!Visualisation of charge distribution&lt;br /&gt;
|[[File:Hyc116_benzene_charge_distribution1.png|500x500px|thumb|centre|Charge distribution of Benzene visualisation]]&lt;br /&gt;
|[[File:Hyc116_borazine_charge_distribution1.png|500x500px|thumb|centre|Charge distribution of Borazine visualisation]]&lt;br /&gt;
|-&lt;br /&gt;
!Charge &lt;br /&gt;
|Carbon: -0.239&lt;br /&gt;
&lt;br /&gt;
Hydrogen: 0.239&lt;br /&gt;
|Nitrogen: -1.102 &lt;br /&gt;
&lt;br /&gt;
Boron: 0.747&lt;br /&gt;
&lt;br /&gt;
Hydrogen (bonded to N): 0.432&lt;br /&gt;
&lt;br /&gt;
Hydrogen (bonded to B): -0.077&lt;br /&gt;
|-&lt;br /&gt;
!Discussion&lt;br /&gt;
|From the visualisation, it is shown that there is a slightly negative charge on the carbon atoms, and a positive charge of the same magnitude on the hydrogen atoms. All the carbon atoms have the same charge as they are in identical environments. The same applies to all the hydrogen atoms. This is due to the highly symmetrical structure of benzene. Since the same colour scale was used for both benzene and borazine, and the charges are much smaller in magnitude on atoms in benzene than atoms on borazine, the colours on the charge distribution visualisation is much darker. &lt;br /&gt;
|From the colours displayed on the charge distribution visualisation as well as the charge values, it is shown that nitrogen has a relatively large negative charge, while boron has a positive charge. This is due to the difference in electrogenativity between these atoms: nitrogen atoms are more electronegative than boron and tends to attract electrons towards themselves. It is worth noting that the hydrogen atoms do not all have the same charge. The hydrogen atoms bonded to boron have a slightly negative charge, and the ones bonded to nitrogen have a small positive charge. &lt;br /&gt;
&lt;br /&gt;
The fact that the same colour scale was used for both molecules comes in helpful here. It allows the charges on atoms to be compared directly. For example, just from looking at the colours, one can tell that or example, even though both carbon and nitrogen are electronegative, nitrogen is much more electronegative, which is quantitatively shown by Pauling&#039;s electronegativity scale.&lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
===Comparative MOs of Benzene and Borazine===&lt;br /&gt;
&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot;&lt;br /&gt;
!&lt;br /&gt;
!Benzene&lt;br /&gt;
!Borazine&lt;br /&gt;
!Comparison and Discussion&lt;br /&gt;
|-&lt;br /&gt;
!1st comparative pair&lt;br /&gt;
|[[File:Hyc116_benzene_1st_MO_pair_7.png|200x200px|centre]]&lt;br /&gt;
|[[File:Hyc116_borazine_1st_MO_pair_level9.png|200x200px|centre]]&lt;br /&gt;
|MO 9 of both benzene and borazine are comparable. They both show delocalised molecular orbital with an overall bonding character. There is a nodal plane across the molecular orbitals for both benzene and borazine. For benzene, there is contribution from all the carbon and hydrogen s orbitals. Moreover, the molecular orbitals are symmetric to their counterpart of opposite phase. That is not the case for borazine; they are less symmetric in borazine. Nitrogen atoms are more electronegative than boron atoms and pull electron density towards themselves, resulting in a larger MO. There is contribution from all the boron and nitrogen s orbitals, and three of the hydrogen s orbitals, though not all of them. &lt;br /&gt;
|-&lt;br /&gt;
!2nd comparative pair&lt;br /&gt;
|[[File:Hyc116_benzene_2nd_MO_pair_10.png|200x200px|centre]]&lt;br /&gt;
|[[File:Hyc116_borazine_2nd_MO_pair_level11.png|200x200px|centre]]&lt;br /&gt;
|&lt;br /&gt;
|-&lt;br /&gt;
!3rd comparative pair&lt;br /&gt;
|[[File:Hyc116_benzene_3rd_MO_pair_21.png|200x200px|centre]]&lt;br /&gt;
|[[File:Hyc116_borazine_3rd_MO_pair_level21.png|200x200px|centre]]&lt;br /&gt;
|&lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
===Aromaticity: some theories===&lt;br /&gt;
&lt;br /&gt;
== References ==&lt;/div&gt;</summary>
		<author><name>Hyc116</name></author>
	</entry>
	<entry>
		<id>https://chemwiki.ch.ic.ac.uk/index.php?title=MO_hyc116&amp;diff=730165</id>
		<title>MO hyc116</title>
		<link rel="alternate" type="text/html" href="https://chemwiki.ch.ic.ac.uk/index.php?title=MO_hyc116&amp;diff=730165"/>
		<updated>2018-05-24T17:35:53Z</updated>

		<summary type="html">&lt;p&gt;Hyc116: &lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;==BH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;==&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;Calculation type&amp;lt;/b&amp;gt;: Optimisation&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;Calculation Method&amp;lt;/b&amp;gt;: B3LYP&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;Basis set&amp;lt;/b&amp;gt;: 6-31G(d,p) &lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Summary table&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
[[file:Hyc116_bh3_631g_opt_summarytable.png]]&lt;br /&gt;
&lt;br /&gt;
The above summary table was obtained after the 2nd optimisation of BH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt; (after the initial optimisation using the 3-21G basis set). Notice how the symmetry is incorrect and shown as Cs. This is because the symmetry was manually broken at the beginning by changing the bond length of B-H bonds. The point group was manually adjusted and the molecule was optimised again before the frequency analysis and the new summary table is attached below.&lt;br /&gt;
&lt;br /&gt;
[[file:Hyc116_bh3_correctsummarytable.png]]&lt;br /&gt;
&lt;br /&gt;
The above summary table was obtained from the optimisation after adjusting the symmetry. The point shown in this summary table is D&amp;lt;sub&amp;gt;3h&amp;lt;/sub&amp;gt;, which is the correct for BH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;. &lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Items table&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
Below is the items table taken from the optimisation with the correct point group.&lt;br /&gt;
&lt;br /&gt;
&amp;lt;pre&amp;gt;&lt;br /&gt;
Item               Value     Threshold  Converged?&lt;br /&gt;
 Maximum Force            0.000015     0.000450     YES&lt;br /&gt;
 RMS     Force            0.000010     0.000300     YES&lt;br /&gt;
 Maximum Displacement     0.000058     0.001800     YES&lt;br /&gt;
 RMS     Displacement     0.000038     0.001200     YES&lt;br /&gt;
&amp;lt;/pre&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Frequency log file&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
[[Media:HYC116 BH3 FREQ.LOG]] &lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Frequencies&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;pre&amp;gt;&lt;br /&gt;
Low frequencies ---  -10.3498   -3.4492   -1.2454   -0.0055    0.4779    3.2165&lt;br /&gt;
Low frequencies --- 1162.9519 1213.1527 1213.1554&lt;br /&gt;
&amp;lt;/pre&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;jmol of BH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;&#039;&#039;&#039;&lt;br /&gt;
&amp;lt;jmol&amp;gt;&amp;lt;jmolApplet&amp;gt;&lt;br /&gt;
  &amp;lt;title&amp;gt;optimised BH3&amp;lt;/title&amp;gt;&lt;br /&gt;
  &amp;lt;color&amp;gt;black&amp;lt;/color&amp;gt;&lt;br /&gt;
  &amp;lt;size&amp;gt;200&amp;lt;/size&amp;gt;&lt;br /&gt;
  &amp;lt;uploadedFileContents&amp;gt;HYC116_BH3_FREQ.LOG&amp;lt;/uploadedFileContents&amp;gt;&lt;br /&gt;
&amp;lt;/jmolApplet&amp;gt;&amp;lt;/jmol&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
===Vibrational spectrum===&lt;br /&gt;
&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot;&lt;br /&gt;
!wavenumber (cm&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;)&lt;br /&gt;
!Intensity (arbitrary units)&lt;br /&gt;
!symmetry&lt;br /&gt;
!IR active?&lt;br /&gt;
!type&lt;br /&gt;
|-&lt;br /&gt;
|1163&lt;br /&gt;
|93&lt;br /&gt;
|A&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;&#039; &#039;&lt;br /&gt;
|Yes&lt;br /&gt;
|Out of plane bend&lt;br /&gt;
|-&lt;br /&gt;
|1213&lt;br /&gt;
|14&lt;br /&gt;
|E&#039;&lt;br /&gt;
|Very slight&lt;br /&gt;
|Bend&lt;br /&gt;
|-&lt;br /&gt;
|1213&lt;br /&gt;
|14&lt;br /&gt;
|E&#039;&lt;br /&gt;
|Very slight&lt;br /&gt;
|Bend&lt;br /&gt;
|-&lt;br /&gt;
|2582&lt;br /&gt;
|0&lt;br /&gt;
|A&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;&#039;&lt;br /&gt;
|No&lt;br /&gt;
|Symmetric stretch&lt;br /&gt;
|-&lt;br /&gt;
|2716&lt;br /&gt;
|126&lt;br /&gt;
|E&#039;&lt;br /&gt;
|Yes&lt;br /&gt;
|Asymmetric stretch&lt;br /&gt;
|-&lt;br /&gt;
|2716&lt;br /&gt;
|126&lt;br /&gt;
|E&#039;&lt;br /&gt;
|Yes&lt;br /&gt;
|Asymmetric stretch&lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;IR spectrum&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
[[file:Hyc116_ir_bh3.png|400*600]]&lt;br /&gt;
&lt;br /&gt;
There are only three peaks on the IR spectrum of BH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;, despite that there are 6 vibrational modes for the molecule. As shown in the table above, the symmetric stretching mode with A1 symmetry at 2582 cm&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt; is not IR active; naturally, that vibrational mode doesn’t give a peak on the IR spectrum. As shown from the table, two pairs of vibrational modes, the bond angle deformation/bend at 1213 cm&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt; and the asymmetric bond stretch at 2716 cm&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;, are degenerate with the symmetry label E. This means that they have the same energy, and hence give the same wavenumber on the IR spectrum. Each pair of degenerate vibrational modes give rise to one peak. This leaves three peaks, as confirmed by the IR spectrum above.&lt;br /&gt;
&lt;br /&gt;
===Molecular orbitals of BH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;===&lt;br /&gt;
&lt;br /&gt;
[[file:hyc116_bh3_MO_diagram.png]]&lt;br /&gt;
&lt;br /&gt;
The above molecular orbital diagram was taken from Dr Patricia Hunt&#039;s &amp;lt;i&amp;gt;Lecture 4 Tutorial Problem Model Answers&amp;lt;/i&amp;gt;. . Diagrams of the &amp;quot;real&amp;quot; MOs were obtained from Gaussian.&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
There is no significant difference between the LCAO MOs and the real ones. Features such as orbital phases are shown clearly on both the LCAO MOs and the real MOs, illustrating the bonding/anti-bonding characters of the molecular orbitals. This suggests that the the qualitative MO theory is highly accurate and useful when studying the molecular orbitals of molecules.&lt;br /&gt;
&lt;br /&gt;
==Associated energies: ammonium borane==&lt;br /&gt;
&lt;br /&gt;
===NH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;===&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;Calculation type&amp;lt;/b&amp;gt;: Optimisation&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;Calculation Method&amp;lt;/b&amp;gt;: B3LYP&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;Basis set&amp;lt;/b&amp;gt;: 6-31G(d,p) &lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Summary table&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
[[file:Hyc116_nh3_631g_summarytable.png]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Items table&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;pre&amp;gt;&lt;br /&gt;
Item               Value     Threshold  Converged?&lt;br /&gt;
 Maximum Force            0.000006     0.000450     YES&lt;br /&gt;
 RMS     Force            0.000004     0.000300     YES&lt;br /&gt;
 Maximum Displacement     0.000012     0.001800     YES&lt;br /&gt;
 RMS     Displacement     0.000008     0.001200     YES&lt;br /&gt;
&amp;lt;/pre&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Frequency log file&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
[[Media:HYC116_NH3_FREQ.LOG]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Frequencies&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;pre&amp;gt;&lt;br /&gt;
Low frequencies ---   -8.5646   -8.5588   -0.0047    0.0454    0.1784   26.4183&lt;br /&gt;
Low frequencies --- 1089.7603 1694.1865 1694.1865&lt;br /&gt;
&amp;lt;/pre&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;jmol of NH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;&#039;&#039;&#039;&lt;br /&gt;
&amp;lt;jmol&amp;gt;&amp;lt;jmolApplet&amp;gt;&lt;br /&gt;
  &amp;lt;title&amp;gt;optimised NH3&amp;lt;/title&amp;gt;&lt;br /&gt;
  &amp;lt;color&amp;gt;black&amp;lt;/color&amp;gt;&lt;br /&gt;
  &amp;lt;size&amp;gt;200&amp;lt;/size&amp;gt;&lt;br /&gt;
  &amp;lt;uploadedFileContents&amp;gt;HYC116_NH3_FREQ.LOG&amp;lt;/uploadedFileContents&amp;gt;&lt;br /&gt;
&amp;lt;/jmolApplet&amp;gt;&amp;lt;/jmol&amp;gt;&lt;br /&gt;
&lt;br /&gt;
===NH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;BH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;===&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;Calculation type&amp;lt;/b&amp;gt;: Optimisation&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;Calculation Method&amp;lt;/b&amp;gt;: B3LYP&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;Basis set&amp;lt;/b&amp;gt;: 6-31G(d,p) &lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Summary table&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
[[file:Hyc116_nh3bh3_631g_summarytable.png]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Items table&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;pre&amp;gt;&lt;br /&gt;
Item               Value     Threshold  Converged?&lt;br /&gt;
 Maximum Force            0.000123     0.000450     YES&lt;br /&gt;
 RMS     Force            0.000058     0.000300     YES&lt;br /&gt;
 Maximum Displacement     0.000515     0.001800     YES&lt;br /&gt;
 RMS     Displacement     0.000296     0.001200     YES&lt;br /&gt;
&amp;lt;/pre&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Frequency log file&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
[[Media:HYC116_NH3BH3_FREQ.LOG]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Frequencies&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;pre&amp;gt;&lt;br /&gt;
Low frequencies ---   -0.0014   -0.0011   -0.0006    6.9624   20.4518   43.5542&lt;br /&gt;
Low frequencies ---  266.4530  632.2458  639.0504&lt;br /&gt;
&amp;lt;/pre&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;jmol of NH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;BH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;&#039;&#039;&#039;&lt;br /&gt;
&amp;lt;jmol&amp;gt;&amp;lt;jmolApplet&amp;gt;&lt;br /&gt;
  &amp;lt;title&amp;gt;optimised NH3BH3&amp;lt;/title&amp;gt;&lt;br /&gt;
  &amp;lt;color&amp;gt;black&amp;lt;/color&amp;gt;&lt;br /&gt;
  &amp;lt;size&amp;gt;200&amp;lt;/size&amp;gt;&lt;br /&gt;
  &amp;lt;uploadedFileContents&amp;gt;HYC116_NH3BH3_FREQ.LOG&amp;lt;/uploadedFileContents&amp;gt;&lt;br /&gt;
&amp;lt;/jmolApplet&amp;gt;&amp;lt;/jmol&amp;gt;&lt;br /&gt;
&lt;br /&gt;
===Association energy===&lt;br /&gt;
&lt;br /&gt;
E(BH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;) (using the optimisation with the correct symmetry) = -26.61532363 a.u. = &amp;lt;b&amp;gt;-26.61532 a.u. (5 d.p.)&amp;lt;/b&amp;gt;&lt;br /&gt;
&lt;br /&gt;
E(NH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;) = -56.55776873 a.u. = &amp;lt;b&amp;gt;-56.55777 a.u. (5 d.p.)&amp;lt;/b&amp;gt;&lt;br /&gt;
&lt;br /&gt;
E(NH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;BH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;) = -83.22468893 a.u. = &amp;lt;b&amp;gt;-83.22469 a.u. (5 d.p.)&amp;lt;/b&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
Carrying out calculations using numbers which has already been rounded up can possibly result in errors in the last digit. Hence, here the calculations were carried out using the numbers provided from the optimisations (i.e. with more decimal places than necessary); the answer was then rounded up to the desired accuracy. &lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
ΔE = E(NH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;BH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;)-[E(NH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;)+E(BH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;)]&lt;br /&gt;
&lt;br /&gt;
ΔE = -83.22468893 - (-56.55776873 + -26.61532363) = -0.05159657 a.u. &lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;ΔE = -0.05160 a.u. (5 d.p.)&amp;lt;/b&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Converting energy from a.u. to kJ/mol&#039;&#039;&#039;&lt;br /&gt;
An atomic unit for energy is Hartree, which is equal to 2625.5 kJ/mol. &lt;br /&gt;
&lt;br /&gt;
So ΔE in kJ/mol = -0.05159657 * 2625.5 = -135.466794535 kJ/mol&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;ΔE = -135 kJ/mol (nearest integer)&amp;lt;/b&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
The energy difference calculated above comes from the formation of the B-N dative bond. It is a relatively weak bond. According to a bond energy data sheet provided by the University of California,  the bond energy of the C-C bond of an ethane molecule is 368 kJ/mol. This is a fair comparison to the NH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;BH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt; molecule as the two molecules have the same structure, only with the carbon atoms on ethane swapped for Boron and Nitrogen in NH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;BH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;&lt;br /&gt;
&lt;br /&gt;
==Using a mixture of basis-sets and pseudo-potentials==&lt;br /&gt;
&lt;br /&gt;
===BBr&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;===&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;Calculation type&amp;lt;/b&amp;gt;: Optimisation&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;Calculation Method&amp;lt;/b&amp;gt;: B3LYP&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;Basis set&amp;lt;/b&amp;gt;: Boron: 6-31G(d,p) ; Br: LANL2DZ&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
Larger calculations are often sent to a web-server to run on a high-performance computer instead of a desktop. In order to experience and learn to use a web-server, the optimisation and the frequency analysis for BBr&amp;lt;sub&amp;gt;3&amp;lt;/sub were both sent and done on a server instead of the desktop. The calculation results were downloaded from the web-server once they were finished.   &lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Summary table&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
[[file:Hyc116_bbr3_opt_summarytable.png]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Items table&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;pre&amp;gt;&lt;br /&gt;
Item               Value     Threshold  Converged?&lt;br /&gt;
 Maximum Force            0.000008     0.000450     YES&lt;br /&gt;
 RMS     Force            0.000005     0.000300     YES&lt;br /&gt;
 Maximum Displacement     0.000036     0.001800     YES&lt;br /&gt;
 RMS     Displacement     0.000023     0.001200     YES&lt;br /&gt;
&amp;lt;/pre&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Frequency log file&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
[[Media:Hyc116_bbr3_freq.log]]&lt;br /&gt;
&lt;br /&gt;
Attached above is the frequency file saved onto the computer from the SCAN server portal. The frequency file was also published on the chemistry database DSpace. {{DOI|10042/202442}}&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Frequencies&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;pre&amp;gt;&lt;br /&gt;
Low frequencies ---   -0.0137   -0.0064   -0.0046    2.4315    2.4315    4.8421&lt;br /&gt;
Low frequencies ---  155.9631  155.9651  267.7052&lt;br /&gt;
&amp;lt;/pre&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;jmol of BBr&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;&#039;&#039;&#039;&lt;br /&gt;
&amp;lt;jmol&amp;gt;&amp;lt;jmolApplet&amp;gt;&lt;br /&gt;
  &amp;lt;title&amp;gt;optimised BBr3&amp;lt;/title&amp;gt;&lt;br /&gt;
  &amp;lt;color&amp;gt;black&amp;lt;/color&amp;gt;&lt;br /&gt;
  &amp;lt;size&amp;gt;200&amp;lt;/size&amp;gt;&lt;br /&gt;
  &amp;lt;uploadedFileContents&amp;gt;Hyc116_bbr3_freq.log&amp;lt;/uploadedFileContents&amp;gt;&lt;br /&gt;
&amp;lt;/jmolApplet&amp;gt;&amp;lt;/jmol&amp;gt;&lt;br /&gt;
&lt;br /&gt;
==Aromaticity==&lt;br /&gt;
&lt;br /&gt;
===Benzene===&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;Calculation type&amp;lt;/b&amp;gt;: Optimisation&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;Calculation Method&amp;lt;/b&amp;gt;: B3LYP&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;Basis set&amp;lt;/b&amp;gt;: 6-31G(d,p) &lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Summary table&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
[[file:Hyc116_c6h6_summarytable.png]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Items table&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;pre&amp;gt;&lt;br /&gt;
Item               Value     Threshold  Converged?&lt;br /&gt;
 Maximum Force            0.000193     0.000450     YES&lt;br /&gt;
 RMS     Force            0.000079     0.000300     YES&lt;br /&gt;
 Maximum Displacement     0.000830     0.001800     YES&lt;br /&gt;
 RMS     Displacement     0.000294     0.001200     YES&lt;br /&gt;
&amp;lt;/pre&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Frequency log file&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
[[Media:HYC116_C6H6_FREQ.LOG]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Frequencies&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;pre&amp;gt;&lt;br /&gt;
Low frequencies ---   -3.5606   -3.5606   -0.0089   -0.0043   -0.0043   10.0905&lt;br /&gt;
Low frequencies ---  413.9582  413.9582  621.1416&lt;br /&gt;
&amp;lt;/pre&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;jmol of C&amp;lt;sub&amp;gt;6&amp;lt;/sub&amp;gt;H&amp;lt;sub&amp;gt;6&amp;lt;/sub&amp;gt;&#039;&#039;&#039;&lt;br /&gt;
&amp;lt;jmol&amp;gt;&amp;lt;jmolApplet&amp;gt;&lt;br /&gt;
  &amp;lt;title&amp;gt;optimised Benzene&amp;lt;/title&amp;gt;&lt;br /&gt;
  &amp;lt;color&amp;gt;black&amp;lt;/color&amp;gt;&lt;br /&gt;
  &amp;lt;size&amp;gt;200&amp;lt;/size&amp;gt;&lt;br /&gt;
  &amp;lt;uploadedFileContents&amp;gt;HYC116_C6H6_FREQ.LOG&amp;lt;/uploadedFileContents&amp;gt;&lt;br /&gt;
&amp;lt;/jmolApplet&amp;gt;&amp;lt;/jmol&amp;gt;&lt;br /&gt;
&lt;br /&gt;
===Borazine===&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;Calculation type&amp;lt;/b&amp;gt;: Optimisation&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;Calculation Method&amp;lt;/b&amp;gt;: B3LYP&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;Basis set&amp;lt;/b&amp;gt;: 6-31G(d,p) &lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Summary table&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
[[file:Hyc116_borazine_summarytable.png]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Items table&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;pre&amp;gt;&lt;br /&gt;
Item               Value     Threshold  Converged?&lt;br /&gt;
 Maximum Force            0.000085     0.000450     YES&lt;br /&gt;
 RMS     Force            0.000033     0.000300     YES&lt;br /&gt;
 Maximum Displacement     0.000250     0.001800     YES&lt;br /&gt;
 RMS     Displacement     0.000074     0.001200     YES&lt;br /&gt;
&amp;lt;/pre&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Frequency log file&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
[[Media:HYC116_BORAZINE_FREQ.LOG]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Frequencies&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;pre&amp;gt;&lt;br /&gt;
Low frequencies ---  -12.6626  -12.6626   -8.9272   -0.0211   -0.0104   -0.0104&lt;br /&gt;
Low frequencies ---  289.1112  289.1112  403.8613&lt;br /&gt;
&amp;lt;/pre&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;jmol of Borazine&#039;&#039;&#039;&lt;br /&gt;
&amp;lt;jmol&amp;gt;&amp;lt;jmolApplet&amp;gt;&lt;br /&gt;
  &amp;lt;title&amp;gt;optimised Borazine&amp;lt;/title&amp;gt;&lt;br /&gt;
  &amp;lt;color&amp;gt;black&amp;lt;/color&amp;gt;&lt;br /&gt;
  &amp;lt;size&amp;gt;200&amp;lt;/size&amp;gt;&lt;br /&gt;
  &amp;lt;uploadedFileContents&amp;gt;HYC116_BORAZINE_FREQ.LOG&amp;lt;/uploadedFileContents&amp;gt;&lt;br /&gt;
&amp;lt;/jmolApplet&amp;gt;&amp;lt;/jmol&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
===Charge distribution===&lt;br /&gt;
&lt;br /&gt;
An NBO charge analysis was carried out on both the optimised benzene and borazine. Visualisations of the charge distribution are shown in the table below, with the colour range going from -1.102 to 1.102 for both molecule. This large scale was chosen as it allows direct comparison of the charge on any atoms in these two molecules and shows the relative magnitude of charges on all these atoms. Negative charges are shown in red, and positive charges are shown in green. A neutral charge is displayed in black, so the smaller a charge is (positive or negative), the darker its colour representation is. Larger charges are shown in brighter colours. The charges are also displayed on the atoms as numbers with a neutral charge being zero. Negative charges are shown as negative number and positive charges are shown as positive numbers. &lt;br /&gt;
&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot;&lt;br /&gt;
!&lt;br /&gt;
!Benzene&lt;br /&gt;
!Borazine&lt;br /&gt;
|-&lt;br /&gt;
!Visualisation of charge distribution&lt;br /&gt;
|[[File:Hyc116_benzene_charge_distribution1.png|500x500px|thumb|centre|Charge distribution of Benzene visualisation]]&lt;br /&gt;
|[[File:Hyc116_borazine_charge_distribution1.png|500x500px|thumb|centre|Charge distribution of Borazine visualisation]]&lt;br /&gt;
|-&lt;br /&gt;
!Charge &lt;br /&gt;
|Carbon: -0.239&lt;br /&gt;
&lt;br /&gt;
Hydrogen: 0.239&lt;br /&gt;
|Nitrogen: -1.102 &lt;br /&gt;
&lt;br /&gt;
Boron: 0.747&lt;br /&gt;
&lt;br /&gt;
Hydrogen (bonded to N): 0.432&lt;br /&gt;
&lt;br /&gt;
Hydrogen (bonded to B): -0.077&lt;br /&gt;
|-&lt;br /&gt;
!Discussion&lt;br /&gt;
|From the visualisation, it is shown that there is a slightly negative charge on the carbon atoms, and a positive charge of the same magnitude on the hydrogen atoms. All the carbon atoms have the same charge as they are in identical environments. The same applies to all the hydrogen atoms. This is due to the highly symmetrical structure of benzene. Since the same colour scale was used for both benzene and borazine, and the charges are much smaller in magnitude on atoms in benzene than atoms on borazine, the colours on the charge distribution visualisation is much darker. &lt;br /&gt;
|From the colours displayed on the charge distribution visualisation as well as the charge values, it is shown that nitrogen has a relatively large negative charge, while boron has a positive charge. This is due to the difference in electrogenativity between these atoms: nitrogen atoms are more electronegative than boron and tends to attract electrons towards themselves. It is worth noting that the hydrogen atoms do not all have the same charge. The hydrogen atoms bonded to boron have a slightly negative charge, and the ones bonded to nitrogen have a small positive charge. &lt;br /&gt;
&lt;br /&gt;
The fact that the same colour scale was used for both molecules comes in helpful here. It allows the charges on atoms to be compared directly. For example, just from looking at the colours, one can tell that or example, even though both carbon and nitrogen are electronegative, nitrogen is much more electronegative, which is quantitatively shown by Pauling&#039;s electronegativity scale.&lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
===Comparative MOs of Benzene and Borazine===&lt;br /&gt;
&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot;&lt;br /&gt;
!&lt;br /&gt;
!Benzene&lt;br /&gt;
!Borazine&lt;br /&gt;
!Comparison and Discussion&lt;br /&gt;
|-&lt;br /&gt;
!1st comparative pair&lt;br /&gt;
|[[File:Hyc116_benzene_1st_MO_pair_7.png|200x200px|centre]]&lt;br /&gt;
|[[File:Hyc116_borazine_1st_MO_pair_level9.png|200x200px|centre]]&lt;br /&gt;
|MO 9 of both benzene and borazine are comparable. They both show delocalised molecular orbital with an overall bonding character. There is a nodal plane across the molecular orbitals for both benzene and borazine. For benzene, there is contribution from all the carbon and hydrogen s orbitals. Moreover, the molecular orbitals are symmetric to their counterpart of opposite phase. That is not the case for borazine; they are less symmetric in borazine. Nitrogen atoms are more electronegative than boron atoms and pull electron density towards themselves, resulting in a larger MO. There is contribution from all the boron and nitrogen s orbitals, and three of the hydrogen s orbitals, though not all of them. &lt;br /&gt;
|-&lt;br /&gt;
!2nd comparative pair&lt;br /&gt;
|[[File:Hyc116_benzene_2nd_MO_pair_10.png|200x200px|centre]]&lt;br /&gt;
|[[File:Hyc116_borazine_2nd_MO_pair_level11.png|200x200px|centre]]&lt;br /&gt;
|&lt;br /&gt;
|-&lt;br /&gt;
!3rd comparative pair&lt;br /&gt;
|[[File:Hyc116_benzene_3rd_MO_pair_21.png|200x200px|centre]]&lt;br /&gt;
|[[File:Hyc116_borazine_3rd_MO_pair_level21.png|200x200px|centre]]&lt;br /&gt;
|&lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
===Aromaticity: some theories===&lt;br /&gt;
==References==&lt;/div&gt;</summary>
		<author><name>Hyc116</name></author>
	</entry>
	<entry>
		<id>https://chemwiki.ch.ic.ac.uk/index.php?title=MO_hyc116&amp;diff=730164</id>
		<title>MO hyc116</title>
		<link rel="alternate" type="text/html" href="https://chemwiki.ch.ic.ac.uk/index.php?title=MO_hyc116&amp;diff=730164"/>
		<updated>2018-05-24T17:35:31Z</updated>

		<summary type="html">&lt;p&gt;Hyc116: &lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;==BH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;==&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;Calculation type&amp;lt;/b&amp;gt;: Optimisation&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;Calculation Method&amp;lt;/b&amp;gt;: B3LYP&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;Basis set&amp;lt;/b&amp;gt;: 6-31G(d,p) &lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Summary table&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
[[file:Hyc116_bh3_631g_opt_summarytable.png]]&lt;br /&gt;
&lt;br /&gt;
The above summary table was obtained after the 2nd optimisation of BH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt; (after the initial optimisation using the 3-21G basis set). Notice how the symmetry is incorrect and shown as Cs. This is because the symmetry was manually broken at the beginning by changing the bond length of B-H bonds. The point group was manually adjusted and the molecule was optimised again before the frequency analysis and the new summary table is attached below.&lt;br /&gt;
&lt;br /&gt;
[[file:Hyc116_bh3_correctsummarytable.png]]&lt;br /&gt;
&lt;br /&gt;
The above summary table was obtained from the optimisation after adjusting the symmetry. The point shown in this summary table is D&amp;lt;sub&amp;gt;3h&amp;lt;/sub&amp;gt;, which is the correct for BH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;. &lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Items table&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
Below is the items table taken from the optimisation with the correct point group.&lt;br /&gt;
&lt;br /&gt;
&amp;lt;pre&amp;gt;&lt;br /&gt;
Item               Value     Threshold  Converged?&lt;br /&gt;
 Maximum Force            0.000015     0.000450     YES&lt;br /&gt;
 RMS     Force            0.000010     0.000300     YES&lt;br /&gt;
 Maximum Displacement     0.000058     0.001800     YES&lt;br /&gt;
 RMS     Displacement     0.000038     0.001200     YES&lt;br /&gt;
&amp;lt;/pre&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Frequency log file&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
[[Media:HYC116 BH3 FREQ.LOG]] &lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Frequencies&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;pre&amp;gt;&lt;br /&gt;
Low frequencies ---  -10.3498   -3.4492   -1.2454   -0.0055    0.4779    3.2165&lt;br /&gt;
Low frequencies --- 1162.9519 1213.1527 1213.1554&lt;br /&gt;
&amp;lt;/pre&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;jmol of BH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;&#039;&#039;&#039;&lt;br /&gt;
&amp;lt;jmol&amp;gt;&amp;lt;jmolApplet&amp;gt;&lt;br /&gt;
  &amp;lt;title&amp;gt;optimised BH3&amp;lt;/title&amp;gt;&lt;br /&gt;
  &amp;lt;color&amp;gt;black&amp;lt;/color&amp;gt;&lt;br /&gt;
  &amp;lt;size&amp;gt;200&amp;lt;/size&amp;gt;&lt;br /&gt;
  &amp;lt;uploadedFileContents&amp;gt;HYC116_BH3_FREQ.LOG&amp;lt;/uploadedFileContents&amp;gt;&lt;br /&gt;
&amp;lt;/jmolApplet&amp;gt;&amp;lt;/jmol&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
===Vibrational spectrum===&lt;br /&gt;
&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot;&lt;br /&gt;
!wavenumber (cm&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;)&lt;br /&gt;
!Intensity (arbitrary units)&lt;br /&gt;
!symmetry&lt;br /&gt;
!IR active?&lt;br /&gt;
!type&lt;br /&gt;
|-&lt;br /&gt;
|1163&lt;br /&gt;
|93&lt;br /&gt;
|A&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;&#039; &#039;&lt;br /&gt;
|Yes&lt;br /&gt;
|Out of plane bend&lt;br /&gt;
|-&lt;br /&gt;
|1213&lt;br /&gt;
|14&lt;br /&gt;
|E&#039;&lt;br /&gt;
|Very slight&lt;br /&gt;
|Bend&lt;br /&gt;
|-&lt;br /&gt;
|1213&lt;br /&gt;
|14&lt;br /&gt;
|E&#039;&lt;br /&gt;
|Very slight&lt;br /&gt;
|Bend&lt;br /&gt;
|-&lt;br /&gt;
|2582&lt;br /&gt;
|0&lt;br /&gt;
|A&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;&#039;&lt;br /&gt;
|No&lt;br /&gt;
|Symmetric stretch&lt;br /&gt;
|-&lt;br /&gt;
|2716&lt;br /&gt;
|126&lt;br /&gt;
|E&#039;&lt;br /&gt;
|Yes&lt;br /&gt;
|Asymmetric stretch&lt;br /&gt;
|-&lt;br /&gt;
|2716&lt;br /&gt;
|126&lt;br /&gt;
|E&#039;&lt;br /&gt;
|Yes&lt;br /&gt;
|Asymmetric stretch&lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;IR spectrum&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
[[file:Hyc116_ir_bh3.png|400*600]]&lt;br /&gt;
&lt;br /&gt;
There are only three peaks on the IR spectrum of BH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;, despite that there are 6 vibrational modes for the molecule. As shown in the table above, the symmetric stretching mode with A1 symmetry at 2582 cm&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt; is not IR active; naturally, that vibrational mode doesn’t give a peak on the IR spectrum. As shown from the table, two pairs of vibrational modes, the bond angle deformation/bend at 1213 cm&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt; and the asymmetric bond stretch at 2716 cm&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;, are degenerate with the symmetry label E. This means that they have the same energy, and hence give the same wavenumber on the IR spectrum. Each pair of degenerate vibrational modes give rise to one peak. This leaves three peaks, as confirmed by the IR spectrum above.&lt;br /&gt;
&lt;br /&gt;
===Molecular orbitals of BH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;===&lt;br /&gt;
&lt;br /&gt;
[[file:hyc116_bh3_MO_diagram.png]]&lt;br /&gt;
&lt;br /&gt;
The above molecular orbital diagram was taken from Dr Patricia Hunt&#039;s &amp;lt;i&amp;gt;Lecture 4 Tutorial Problem Model Answers&amp;lt;/i&amp;gt;. . Diagrams of the &amp;quot;real&amp;quot; MOs were obtained from Gaussian.&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
There is no significant difference between the LCAO MOs and the real ones. Features such as orbital phases are shown clearly on both the LCAO MOs and the real MOs, illustrating the bonding/anti-bonding characters of the molecular orbitals. This suggests that the the qualitative MO theory is highly accurate and useful when studying the molecular orbitals of molecules.&lt;br /&gt;
&lt;br /&gt;
==Associated energies: ammonium borane==&lt;br /&gt;
&lt;br /&gt;
===NH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;===&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;Calculation type&amp;lt;/b&amp;gt;: Optimisation&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;Calculation Method&amp;lt;/b&amp;gt;: B3LYP&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;Basis set&amp;lt;/b&amp;gt;: 6-31G(d,p) &lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Summary table&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
[[file:Hyc116_nh3_631g_summarytable.png]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Items table&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;pre&amp;gt;&lt;br /&gt;
Item               Value     Threshold  Converged?&lt;br /&gt;
 Maximum Force            0.000006     0.000450     YES&lt;br /&gt;
 RMS     Force            0.000004     0.000300     YES&lt;br /&gt;
 Maximum Displacement     0.000012     0.001800     YES&lt;br /&gt;
 RMS     Displacement     0.000008     0.001200     YES&lt;br /&gt;
&amp;lt;/pre&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Frequency log file&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
[[Media:HYC116_NH3_FREQ.LOG]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Frequencies&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;pre&amp;gt;&lt;br /&gt;
Low frequencies ---   -8.5646   -8.5588   -0.0047    0.0454    0.1784   26.4183&lt;br /&gt;
Low frequencies --- 1089.7603 1694.1865 1694.1865&lt;br /&gt;
&amp;lt;/pre&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;jmol of NH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;&#039;&#039;&#039;&lt;br /&gt;
&amp;lt;jmol&amp;gt;&amp;lt;jmolApplet&amp;gt;&lt;br /&gt;
  &amp;lt;title&amp;gt;optimised NH3&amp;lt;/title&amp;gt;&lt;br /&gt;
  &amp;lt;color&amp;gt;black&amp;lt;/color&amp;gt;&lt;br /&gt;
  &amp;lt;size&amp;gt;200&amp;lt;/size&amp;gt;&lt;br /&gt;
  &amp;lt;uploadedFileContents&amp;gt;HYC116_NH3_FREQ.LOG&amp;lt;/uploadedFileContents&amp;gt;&lt;br /&gt;
&amp;lt;/jmolApplet&amp;gt;&amp;lt;/jmol&amp;gt;&lt;br /&gt;
&lt;br /&gt;
===NH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;BH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;===&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;Calculation type&amp;lt;/b&amp;gt;: Optimisation&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;Calculation Method&amp;lt;/b&amp;gt;: B3LYP&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;Basis set&amp;lt;/b&amp;gt;: 6-31G(d,p) &lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Summary table&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
[[file:Hyc116_nh3bh3_631g_summarytable.png]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Items table&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;pre&amp;gt;&lt;br /&gt;
Item               Value     Threshold  Converged?&lt;br /&gt;
 Maximum Force            0.000123     0.000450     YES&lt;br /&gt;
 RMS     Force            0.000058     0.000300     YES&lt;br /&gt;
 Maximum Displacement     0.000515     0.001800     YES&lt;br /&gt;
 RMS     Displacement     0.000296     0.001200     YES&lt;br /&gt;
&amp;lt;/pre&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Frequency log file&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
[[Media:HYC116_NH3BH3_FREQ.LOG]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Frequencies&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;pre&amp;gt;&lt;br /&gt;
Low frequencies ---   -0.0014   -0.0011   -0.0006    6.9624   20.4518   43.5542&lt;br /&gt;
Low frequencies ---  266.4530  632.2458  639.0504&lt;br /&gt;
&amp;lt;/pre&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;jmol of NH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;BH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;&#039;&#039;&#039;&lt;br /&gt;
&amp;lt;jmol&amp;gt;&amp;lt;jmolApplet&amp;gt;&lt;br /&gt;
  &amp;lt;title&amp;gt;optimised NH3BH3&amp;lt;/title&amp;gt;&lt;br /&gt;
  &amp;lt;color&amp;gt;black&amp;lt;/color&amp;gt;&lt;br /&gt;
  &amp;lt;size&amp;gt;200&amp;lt;/size&amp;gt;&lt;br /&gt;
  &amp;lt;uploadedFileContents&amp;gt;HYC116_NH3BH3_FREQ.LOG&amp;lt;/uploadedFileContents&amp;gt;&lt;br /&gt;
&amp;lt;/jmolApplet&amp;gt;&amp;lt;/jmol&amp;gt;&lt;br /&gt;
&lt;br /&gt;
===Association energy===&lt;br /&gt;
&lt;br /&gt;
E(BH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;) (using the optimisation with the correct symmetry) = -26.61532363 a.u. = &amp;lt;b&amp;gt;-26.61532 a.u. (5 d.p.)&amp;lt;/b&amp;gt;&lt;br /&gt;
&lt;br /&gt;
E(NH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;) = -56.55776873 a.u. = &amp;lt;b&amp;gt;-56.55777 a.u. (5 d.p.)&amp;lt;/b&amp;gt;&lt;br /&gt;
&lt;br /&gt;
E(NH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;BH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;) = -83.22468893 a.u. = &amp;lt;b&amp;gt;-83.22469 a.u. (5 d.p.)&amp;lt;/b&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
Carrying out calculations using numbers which has already been rounded up can possibly result in errors in the last digit. Hence, here the calculations were carried out using the numbers provided from the optimisations (i.e. with more decimal places than necessary); the answer was then rounded up to the desired accuracy. &lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
ΔE = E(NH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;BH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;)-[E(NH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;)+E(BH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;)]&lt;br /&gt;
&lt;br /&gt;
ΔE = -83.22468893 - (-56.55776873 + -26.61532363) = -0.05159657 a.u. &lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;ΔE = -0.05160 a.u. (5 d.p.)&amp;lt;/b&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Converting energy from a.u. to kJ/mol&#039;&#039;&#039;&lt;br /&gt;
An atomic unit for energy is Hartree, which is equal to 2625.5 kJ/mol. &lt;br /&gt;
&lt;br /&gt;
So ΔE in kJ/mol = -0.05159657 * 2625.5 = -135.466794535 kJ/mol&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;ΔE = -135 kJ/mol (nearest integer)&amp;lt;/b&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
The energy difference calculated above comes from the formation of the B-N dative bond. It is a relatively weak bond. According to a bond energy data sheet provided by the University of California,  the bond energy of the C-C bond of an ethane molecule is 368 kJ/mol. This is a fair comparison to the NH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;BH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt; molecule as the two molecules have the same structure, only with the carbon atoms on ethane swapped for Boron and Nitrogen in NH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;BH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;&lt;br /&gt;
&lt;br /&gt;
==Using a mixture of basis-sets and pseudo-potentials==&lt;br /&gt;
&lt;br /&gt;
===BBr&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;===&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;Calculation type&amp;lt;/b&amp;gt;: Optimisation&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;Calculation Method&amp;lt;/b&amp;gt;: B3LYP&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;Basis set&amp;lt;/b&amp;gt;: Boron: 6-31G(d,p) ; Br: LANL2DZ&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
Larger calculations are often sent to a web-server to run on a high-performance computer instead of a desktop. In order to experience and learn to use a web-server, the optimisation and the frequency analysis for BBr&amp;lt;sub&amp;gt;3&amp;lt;/sub were both sent and done on a server instead of the desktop. The calculation results were downloaded from the web-server once they were finished.   &lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Summary table&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
[[file:Hyc116_bbr3_opt_summarytable.png]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Items table&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;pre&amp;gt;&lt;br /&gt;
Item               Value     Threshold  Converged?&lt;br /&gt;
 Maximum Force            0.000008     0.000450     YES&lt;br /&gt;
 RMS     Force            0.000005     0.000300     YES&lt;br /&gt;
 Maximum Displacement     0.000036     0.001800     YES&lt;br /&gt;
 RMS     Displacement     0.000023     0.001200     YES&lt;br /&gt;
&amp;lt;/pre&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Frequency log file&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
[[Media:Hyc116_bbr3_freq.log]]&lt;br /&gt;
&lt;br /&gt;
Attached above is the frequency file saved onto the computer from the SCAN server portal. The frequency file was also published on the chemistry database DSpace. {{DOI|10042/202442}}&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Frequencies&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;pre&amp;gt;&lt;br /&gt;
Low frequencies ---   -0.0137   -0.0064   -0.0046    2.4315    2.4315    4.8421&lt;br /&gt;
Low frequencies ---  155.9631  155.9651  267.7052&lt;br /&gt;
&amp;lt;/pre&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;jmol of BBr&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;&#039;&#039;&#039;&lt;br /&gt;
&amp;lt;jmol&amp;gt;&amp;lt;jmolApplet&amp;gt;&lt;br /&gt;
  &amp;lt;title&amp;gt;optimised BBr3&amp;lt;/title&amp;gt;&lt;br /&gt;
  &amp;lt;color&amp;gt;black&amp;lt;/color&amp;gt;&lt;br /&gt;
  &amp;lt;size&amp;gt;200&amp;lt;/size&amp;gt;&lt;br /&gt;
  &amp;lt;uploadedFileContents&amp;gt;Hyc116_bbr3_freq.log&amp;lt;/uploadedFileContents&amp;gt;&lt;br /&gt;
&amp;lt;/jmolApplet&amp;gt;&amp;lt;/jmol&amp;gt;&lt;br /&gt;
&lt;br /&gt;
==Aromaticity==&lt;br /&gt;
&lt;br /&gt;
===Benzene===&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;Calculation type&amp;lt;/b&amp;gt;: Optimisation&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;Calculation Method&amp;lt;/b&amp;gt;: B3LYP&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;Basis set&amp;lt;/b&amp;gt;: 6-31G(d,p) &lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Summary table&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
[[file:Hyc116_c6h6_summarytable.png]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Items table&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;pre&amp;gt;&lt;br /&gt;
Item               Value     Threshold  Converged?&lt;br /&gt;
 Maximum Force            0.000193     0.000450     YES&lt;br /&gt;
 RMS     Force            0.000079     0.000300     YES&lt;br /&gt;
 Maximum Displacement     0.000830     0.001800     YES&lt;br /&gt;
 RMS     Displacement     0.000294     0.001200     YES&lt;br /&gt;
&amp;lt;/pre&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Frequency log file&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
[[Media:HYC116_C6H6_FREQ.LOG]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Frequencies&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;pre&amp;gt;&lt;br /&gt;
Low frequencies ---   -3.5606   -3.5606   -0.0089   -0.0043   -0.0043   10.0905&lt;br /&gt;
Low frequencies ---  413.9582  413.9582  621.1416&lt;br /&gt;
&amp;lt;/pre&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;jmol of C&amp;lt;sub&amp;gt;6&amp;lt;/sub&amp;gt;H&amp;lt;sub&amp;gt;6&amp;lt;/sub&amp;gt;&#039;&#039;&#039;&lt;br /&gt;
&amp;lt;jmol&amp;gt;&amp;lt;jmolApplet&amp;gt;&lt;br /&gt;
  &amp;lt;title&amp;gt;optimised Benzene&amp;lt;/title&amp;gt;&lt;br /&gt;
  &amp;lt;color&amp;gt;black&amp;lt;/color&amp;gt;&lt;br /&gt;
  &amp;lt;size&amp;gt;200&amp;lt;/size&amp;gt;&lt;br /&gt;
  &amp;lt;uploadedFileContents&amp;gt;HYC116_C6H6_FREQ.LOG&amp;lt;/uploadedFileContents&amp;gt;&lt;br /&gt;
&amp;lt;/jmolApplet&amp;gt;&amp;lt;/jmol&amp;gt;&lt;br /&gt;
&lt;br /&gt;
===Borazine===&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;Calculation type&amp;lt;/b&amp;gt;: Optimisation&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;Calculation Method&amp;lt;/b&amp;gt;: B3LYP&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;Basis set&amp;lt;/b&amp;gt;: 6-31G(d,p) &lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Summary table&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
[[file:Hyc116_borazine_summarytable.png]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Items table&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;pre&amp;gt;&lt;br /&gt;
Item               Value     Threshold  Converged?&lt;br /&gt;
 Maximum Force            0.000085     0.000450     YES&lt;br /&gt;
 RMS     Force            0.000033     0.000300     YES&lt;br /&gt;
 Maximum Displacement     0.000250     0.001800     YES&lt;br /&gt;
 RMS     Displacement     0.000074     0.001200     YES&lt;br /&gt;
&amp;lt;/pre&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Frequency log file&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
[[Media:HYC116_BORAZINE_FREQ.LOG]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Frequencies&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;pre&amp;gt;&lt;br /&gt;
Low frequencies ---  -12.6626  -12.6626   -8.9272   -0.0211   -0.0104   -0.0104&lt;br /&gt;
Low frequencies ---  289.1112  289.1112  403.8613&lt;br /&gt;
&amp;lt;/pre&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;jmol of Borazine&#039;&#039;&#039;&lt;br /&gt;
&amp;lt;jmol&amp;gt;&amp;lt;jmolApplet&amp;gt;&lt;br /&gt;
  &amp;lt;title&amp;gt;optimised Borazine&amp;lt;/title&amp;gt;&lt;br /&gt;
  &amp;lt;color&amp;gt;black&amp;lt;/color&amp;gt;&lt;br /&gt;
  &amp;lt;size&amp;gt;200&amp;lt;/size&amp;gt;&lt;br /&gt;
  &amp;lt;uploadedFileContents&amp;gt;HYC116_BORAZINE_FREQ.LOG&amp;lt;/uploadedFileContents&amp;gt;&lt;br /&gt;
&amp;lt;/jmolApplet&amp;gt;&amp;lt;/jmol&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
===Charge distribution===&lt;br /&gt;
&lt;br /&gt;
An NBO charge analysis was carried out on both the optimised benzene and borazine. Visualisations of the charge distribution are shown in the table below, with the colour range going from -1.102 to 1.102 for both molecule. This large scale was chosen as it allows direct comparison of the charge on any atoms in these two molecules and shows the relative magnitude of charges on all these atoms. Negative charges are shown in red, and positive charges are shown in green. A neutral charge is displayed in black, so the smaller a charge is (positive or negative), the darker its colour representation is. Larger charges are shown in brighter colours. The charges are also displayed on the atoms as numbers with a neutral charge being zero. Negative charges are shown as negative number and positive charges are shown as positive numbers. &lt;br /&gt;
&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot;&lt;br /&gt;
!&lt;br /&gt;
!Benzene&lt;br /&gt;
!Borazine&lt;br /&gt;
|-&lt;br /&gt;
!Visualisation of charge distribution&lt;br /&gt;
|[[File:Hyc116_benzene_charge_distribution1.png|500x500px|thumb|centre|Charge distribution of Benzene visualisation]]&lt;br /&gt;
|[[File:Hyc116_borazine_charge_distribution1.png|500x500px|thumb|centre|Charge distribution of Borazine visualisation]]&lt;br /&gt;
|-&lt;br /&gt;
!Charge &lt;br /&gt;
|Carbon: -0.239&lt;br /&gt;
&lt;br /&gt;
Hydrogen: 0.239&lt;br /&gt;
|Nitrogen: -1.102 &lt;br /&gt;
&lt;br /&gt;
Boron: 0.747&lt;br /&gt;
&lt;br /&gt;
Hydrogen (bonded to N): 0.432&lt;br /&gt;
&lt;br /&gt;
Hydrogen (bonded to B): -0.077&lt;br /&gt;
|-&lt;br /&gt;
!Discussion&lt;br /&gt;
|From the visualisation, it is shown that there is a slightly negative charge on the carbon atoms, and a positive charge of the same magnitude on the hydrogen atoms. All the carbon atoms have the same charge as they are in identical environments. The same applies to all the hydrogen atoms. This is due to the highly symmetrical structure of benzene. Since the same colour scale was used for both benzene and borazine, and the charges are much smaller in magnitude on atoms in benzene than atoms on borazine, the colours on the charge distribution visualisation is much darker. &lt;br /&gt;
|From the colours displayed on the charge distribution visualisation as well as the charge values, it is shown that nitrogen has a relatively large negative charge, while boron has a positive charge. This is due to the difference in electrogenativity between these atoms: nitrogen atoms are more electronegative than boron and tends to attract electrons towards themselves. It is worth noting that the hydrogen atoms do not all have the same charge. The hydrogen atoms bonded to boron have a slightly negative charge, and the ones bonded to nitrogen have a small positive charge. &lt;br /&gt;
&lt;br /&gt;
The fact that the same colour scale was used for both molecules comes in helpful here. It allows the charges on atoms to be compared directly. For example, just from looking at the colours, one can tell that or example, even though both carbon and nitrogen are electronegative, nitrogen is much more electronegative, which is quantitatively shown by Pauling&#039;s electronegativity scale.&lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
===Comparative MOs of Benzene and Borazine===&lt;br /&gt;
&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot;&lt;br /&gt;
!&lt;br /&gt;
!Benzene&lt;br /&gt;
!Borazine&lt;br /&gt;
!Comparison and Discussion&lt;br /&gt;
|-&lt;br /&gt;
!1st comparative pair&lt;br /&gt;
|[[File:Hyc116_benzene_1st_MO_pair_7.png|200x200px|centre]]&lt;br /&gt;
|[[File:Hyc116_borazine_1st_MO_pair_level9.png|200x200px|centre]]&lt;br /&gt;
|MO 9 of both benzene and borazine are comparable. They both show delocalised molecular orbital with an overall bonding character. There is a nodal plane across the molecular orbitals for both benzene and borazine. For benzene, there is contribution from all the carbon and hydrogen s orbitals. Moreover, the molecular orbitals are symmetric to their counterpart of opposite phase. That is not the case for borazine; they are less symmetric in borazine. Nitrogen atoms are more electronegative than boron atoms and pull electron density towards themselves, resulting in a larger MO. There is contribution from all the boron and nitrogen s orbitals, and three of the hydrogen s orbitals, though not all of them. &lt;br /&gt;
|-&lt;br /&gt;
!2nd comparative pair&lt;br /&gt;
|[[File:Hyc116_benzene_2nd_MO_pair_10.png|200x200px|centre]]&lt;br /&gt;
|[[File:Hyc116_borazine_2nd_MO_pair_level11.png|200x200px|centre]]&lt;br /&gt;
|&lt;br /&gt;
|-&lt;br /&gt;
!3rd comparative pair&lt;br /&gt;
|[[File:Hyc116_benzene_3rd_MO_pair_21.png|200x200px|centre]]&lt;br /&gt;
|[[File:Hyc116_borazine_3rd_MO_pair_level21.png|200x200px|centre]]&lt;br /&gt;
|&lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
===Aromaticity: some theories===&lt;br /&gt;
&lt;br /&gt;
==References==&lt;/div&gt;</summary>
		<author><name>Hyc116</name></author>
	</entry>
	<entry>
		<id>https://chemwiki.ch.ic.ac.uk/index.php?title=MO_hyc116&amp;diff=730160</id>
		<title>MO hyc116</title>
		<link rel="alternate" type="text/html" href="https://chemwiki.ch.ic.ac.uk/index.php?title=MO_hyc116&amp;diff=730160"/>
		<updated>2018-05-24T17:33:17Z</updated>

		<summary type="html">&lt;p&gt;Hyc116: &lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;==BH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;==&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;Calculation type&amp;lt;/b&amp;gt;: Optimisation&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;Calculation Method&amp;lt;/b&amp;gt;: B3LYP&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;Basis set&amp;lt;/b&amp;gt;: 6-31G(d,p) &lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Summary table&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
[[file:Hyc116_bh3_631g_opt_summarytable.png]]&lt;br /&gt;
&lt;br /&gt;
The above summary table was obtained after the 2nd optimisation of BH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt; (after the initial optimisation using the 3-21G basis set). Notice how the symmetry is incorrect and shown as Cs. This is because the symmetry was manually broken at the beginning by changing the bond length of B-H bonds. The point group was manually adjusted and the molecule was optimised again before the frequency analysis and the new summary table is attached below.&lt;br /&gt;
&lt;br /&gt;
[[file:Hyc116_bh3_correctsummarytable.png]]&lt;br /&gt;
&lt;br /&gt;
The above summary table was obtained from the optimisation after adjusting the symmetry. The point shown in this summary table is D&amp;lt;sub&amp;gt;3h&amp;lt;/sub&amp;gt;, which is the correct for BH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;. &lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Items table&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
Below is the items table taken from the optimisation with the correct point group.&lt;br /&gt;
&lt;br /&gt;
&amp;lt;pre&amp;gt;&lt;br /&gt;
Item               Value     Threshold  Converged?&lt;br /&gt;
 Maximum Force            0.000015     0.000450     YES&lt;br /&gt;
 RMS     Force            0.000010     0.000300     YES&lt;br /&gt;
 Maximum Displacement     0.000058     0.001800     YES&lt;br /&gt;
 RMS     Displacement     0.000038     0.001200     YES&lt;br /&gt;
&amp;lt;/pre&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Frequency log file&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
[[Media:HYC116 BH3 FREQ.LOG]] &lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Frequencies&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;pre&amp;gt;&lt;br /&gt;
Low frequencies ---  -10.3498   -3.4492   -1.2454   -0.0055    0.4779    3.2165&lt;br /&gt;
Low frequencies --- 1162.9519 1213.1527 1213.1554&lt;br /&gt;
&amp;lt;/pre&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;jmol of BH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;&#039;&#039;&#039;&lt;br /&gt;
&amp;lt;jmol&amp;gt;&amp;lt;jmolApplet&amp;gt;&lt;br /&gt;
  &amp;lt;title&amp;gt;optimised BH3&amp;lt;/title&amp;gt;&lt;br /&gt;
  &amp;lt;color&amp;gt;black&amp;lt;/color&amp;gt;&lt;br /&gt;
  &amp;lt;size&amp;gt;200&amp;lt;/size&amp;gt;&lt;br /&gt;
  &amp;lt;uploadedFileContents&amp;gt;HYC116_BH3_FREQ.LOG&amp;lt;/uploadedFileContents&amp;gt;&lt;br /&gt;
&amp;lt;/jmolApplet&amp;gt;&amp;lt;/jmol&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
===Vibrational spectrum===&lt;br /&gt;
&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot;&lt;br /&gt;
!wavenumber (cm&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;)&lt;br /&gt;
!Intensity (arbitrary units)&lt;br /&gt;
!symmetry&lt;br /&gt;
!IR active?&lt;br /&gt;
!type&lt;br /&gt;
|-&lt;br /&gt;
|1163&lt;br /&gt;
|93&lt;br /&gt;
|A&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;&#039; &#039;&lt;br /&gt;
|Yes&lt;br /&gt;
|Out of plane bend&lt;br /&gt;
|-&lt;br /&gt;
|1213&lt;br /&gt;
|14&lt;br /&gt;
|E&#039;&lt;br /&gt;
|Very slight&lt;br /&gt;
|Bend&lt;br /&gt;
|-&lt;br /&gt;
|1213&lt;br /&gt;
|14&lt;br /&gt;
|E&#039;&lt;br /&gt;
|Very slight&lt;br /&gt;
|Bend&lt;br /&gt;
|-&lt;br /&gt;
|2582&lt;br /&gt;
|0&lt;br /&gt;
|A&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;&#039;&lt;br /&gt;
|No&lt;br /&gt;
|Symmetric stretch&lt;br /&gt;
|-&lt;br /&gt;
|2716&lt;br /&gt;
|126&lt;br /&gt;
|E&#039;&lt;br /&gt;
|Yes&lt;br /&gt;
|Asymmetric stretch&lt;br /&gt;
|-&lt;br /&gt;
|2716&lt;br /&gt;
|126&lt;br /&gt;
|E&#039;&lt;br /&gt;
|Yes&lt;br /&gt;
|Asymmetric stretch&lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;IR spectrum&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
[[file:Hyc116_ir_bh3.png|400*600]]&lt;br /&gt;
&lt;br /&gt;
There are only three peaks on the IR spectrum of BH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;, despite that there are 6 vibrational modes for the molecule. As shown in the table above, the symmetric stretching mode with A1 symmetry at 2582 cm&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt; is not IR active; naturally, that vibrational mode doesn’t give a peak on the IR spectrum. As shown from the table, two pairs of vibrational modes, the bond angle deformation/bend at 1213 cm&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt; and the asymmetric bond stretch at 2716 cm&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;, are degenerate with the symmetry label E. This means that they have the same energy, and hence give the same wavenumber on the IR spectrum. Each pair of degenerate vibrational modes give rise to one peak. This leaves three peaks, as confirmed by the IR spectrum above.&lt;br /&gt;
&lt;br /&gt;
===Molecular orbitals of BH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;===&lt;br /&gt;
&lt;br /&gt;
[[file:hyc116_bh3_MO_diagram.png]]&lt;br /&gt;
&lt;br /&gt;
The above molecular orbital diagram was taken from Dr Patricia Hunt&#039;s &amp;lt;i&amp;gt;Lecture 4 Tutorial Problem Model Answers&amp;lt;/i&amp;gt;. &amp;lt;ref&amp;gt;P. Hunt, &amp;quot;Lecture 4 Tutorial Problem Model Answers&amp;quot;, 2 (2018)&amp;lt;/ref&amp;gt;. Diagrams of the &amp;quot;real&amp;quot; MOs were obtained from Gaussian.&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
There is no significant difference between the LCAO MOs and the real ones. Features such as orbital phases are shown clearly on both the LCAO MOs and the real MOs, illustrating the bonding/anti-bonding characters of the molecular orbitals. This suggests that the the qualitative MO theory is highly accurate and useful when studying the molecular orbitals of molecules.&lt;br /&gt;
&lt;br /&gt;
==Associated energies: ammonium borane==&lt;br /&gt;
&lt;br /&gt;
===NH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;===&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;Calculation type&amp;lt;/b&amp;gt;: Optimisation&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;Calculation Method&amp;lt;/b&amp;gt;: B3LYP&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;Basis set&amp;lt;/b&amp;gt;: 6-31G(d,p) &lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Summary table&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
[[file:Hyc116_nh3_631g_summarytable.png]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Items table&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;pre&amp;gt;&lt;br /&gt;
Item               Value     Threshold  Converged?&lt;br /&gt;
 Maximum Force            0.000006     0.000450     YES&lt;br /&gt;
 RMS     Force            0.000004     0.000300     YES&lt;br /&gt;
 Maximum Displacement     0.000012     0.001800     YES&lt;br /&gt;
 RMS     Displacement     0.000008     0.001200     YES&lt;br /&gt;
&amp;lt;/pre&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Frequency log file&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
[[Media:HYC116_NH3_FREQ.LOG]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Frequencies&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;pre&amp;gt;&lt;br /&gt;
Low frequencies ---   -8.5646   -8.5588   -0.0047    0.0454    0.1784   26.4183&lt;br /&gt;
Low frequencies --- 1089.7603 1694.1865 1694.1865&lt;br /&gt;
&amp;lt;/pre&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;jmol of NH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;&#039;&#039;&#039;&lt;br /&gt;
&amp;lt;jmol&amp;gt;&amp;lt;jmolApplet&amp;gt;&lt;br /&gt;
  &amp;lt;title&amp;gt;optimised NH3&amp;lt;/title&amp;gt;&lt;br /&gt;
  &amp;lt;color&amp;gt;black&amp;lt;/color&amp;gt;&lt;br /&gt;
  &amp;lt;size&amp;gt;200&amp;lt;/size&amp;gt;&lt;br /&gt;
  &amp;lt;uploadedFileContents&amp;gt;HYC116_NH3_FREQ.LOG&amp;lt;/uploadedFileContents&amp;gt;&lt;br /&gt;
&amp;lt;/jmolApplet&amp;gt;&amp;lt;/jmol&amp;gt;&lt;br /&gt;
&lt;br /&gt;
===NH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;BH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;===&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;Calculation type&amp;lt;/b&amp;gt;: Optimisation&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;Calculation Method&amp;lt;/b&amp;gt;: B3LYP&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;Basis set&amp;lt;/b&amp;gt;: 6-31G(d,p) &lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Summary table&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
[[file:Hyc116_nh3bh3_631g_summarytable.png]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Items table&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;pre&amp;gt;&lt;br /&gt;
Item               Value     Threshold  Converged?&lt;br /&gt;
 Maximum Force            0.000123     0.000450     YES&lt;br /&gt;
 RMS     Force            0.000058     0.000300     YES&lt;br /&gt;
 Maximum Displacement     0.000515     0.001800     YES&lt;br /&gt;
 RMS     Displacement     0.000296     0.001200     YES&lt;br /&gt;
&amp;lt;/pre&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Frequency log file&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
[[Media:HYC116_NH3BH3_FREQ.LOG]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Frequencies&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;pre&amp;gt;&lt;br /&gt;
Low frequencies ---   -0.0014   -0.0011   -0.0006    6.9624   20.4518   43.5542&lt;br /&gt;
Low frequencies ---  266.4530  632.2458  639.0504&lt;br /&gt;
&amp;lt;/pre&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;jmol of NH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;BH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;&#039;&#039;&#039;&lt;br /&gt;
&amp;lt;jmol&amp;gt;&amp;lt;jmolApplet&amp;gt;&lt;br /&gt;
  &amp;lt;title&amp;gt;optimised NH3BH3&amp;lt;/title&amp;gt;&lt;br /&gt;
  &amp;lt;color&amp;gt;black&amp;lt;/color&amp;gt;&lt;br /&gt;
  &amp;lt;size&amp;gt;200&amp;lt;/size&amp;gt;&lt;br /&gt;
  &amp;lt;uploadedFileContents&amp;gt;HYC116_NH3BH3_FREQ.LOG&amp;lt;/uploadedFileContents&amp;gt;&lt;br /&gt;
&amp;lt;/jmolApplet&amp;gt;&amp;lt;/jmol&amp;gt;&lt;br /&gt;
&lt;br /&gt;
===Association energy===&lt;br /&gt;
&lt;br /&gt;
E(BH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;) (using the optimisation with the correct symmetry) = -26.61532363 a.u. = &amp;lt;b&amp;gt;-26.61532 a.u. (5 d.p.)&amp;lt;/b&amp;gt;&lt;br /&gt;
&lt;br /&gt;
E(NH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;) = -56.55776873 a.u. = &amp;lt;b&amp;gt;-56.55777 a.u. (5 d.p.)&amp;lt;/b&amp;gt;&lt;br /&gt;
&lt;br /&gt;
E(NH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;BH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;) = -83.22468893 a.u. = &amp;lt;b&amp;gt;-83.22469 a.u. (5 d.p.)&amp;lt;/b&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
Carrying out calculations using numbers which has already been rounded up can possibly result in errors in the last digit. Hence, here the calculations were carried out using the numbers provided from the optimisations (i.e. with more decimal places than necessary); the answer was then rounded up to the desired accuracy. &lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
ΔE = E(NH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;BH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;)-[E(NH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;)+E(BH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;)]&lt;br /&gt;
&lt;br /&gt;
ΔE = -83.22468893 - (-56.55776873 + -26.61532363) = -0.05159657 a.u. &lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;ΔE = -0.05160 a.u. (5 d.p.)&amp;lt;/b&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Converting energy from a.u. to kJ/mol&#039;&#039;&#039;&lt;br /&gt;
An atomic unit for energy is Hartree, which is equal to 2625.5 kJ/mol. &amp;lt;ref&amp;gt;https://cccbdb.nist.gov/hartree.asp (Accessed: 22.05.2018)&amp;lt;/ref&amp;gt;&lt;br /&gt;
&lt;br /&gt;
So ΔE in kJ/mol = -0.05159657 * 2625.5 = -135.466794535 kJ/mol&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;ΔE = -135 kJ/mol (nearest integer)&amp;lt;/b&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
The energy difference calculated above comes from the formation of the B-N dative bond. It is a relatively weak bond. According to a bond energy data sheet provided by the University of California, &amp;lt;ref&amp;gt;https://labs.chem.ucsb.edu/zakarian/armen/11---bonddissociationenergy.pdf (Accessed on 24.05.2018)&amp;lt;/ref&amp;gt; the bond energy of the C-C bond of an ethane molecule is 368 kJ/mol. This is a fair comparison to the NH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;BH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt; molecule as the two molecules have the same structure, only with the carbon atoms on ethane swapped for Boron and Nitrogen in NH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;BH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;&lt;br /&gt;
&lt;br /&gt;
==Using a mixture of basis-sets and pseudo-potentials==&lt;br /&gt;
&lt;br /&gt;
===BBr&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;===&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;Calculation type&amp;lt;/b&amp;gt;: Optimisation&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;Calculation Method&amp;lt;/b&amp;gt;: B3LYP&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;Basis set&amp;lt;/b&amp;gt;: Boron: 6-31G(d,p) ; Br: LANL2DZ&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
Larger calculations are often sent to a web-server to run on a high-performance computer instead of a desktop. In order to experience and learn to use a web-server, the optimisation and the frequency analysis for BBr&amp;lt;sub&amp;gt;3&amp;lt;/sub were both sent and done on a server instead of the desktop. The calculation results were downloaded from the web-server once they were finished.   &lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Summary table&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
[[file:Hyc116_bbr3_opt_summarytable.png]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Items table&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;pre&amp;gt;&lt;br /&gt;
Item               Value     Threshold  Converged?&lt;br /&gt;
 Maximum Force            0.000008     0.000450     YES&lt;br /&gt;
 RMS     Force            0.000005     0.000300     YES&lt;br /&gt;
 Maximum Displacement     0.000036     0.001800     YES&lt;br /&gt;
 RMS     Displacement     0.000023     0.001200     YES&lt;br /&gt;
&amp;lt;/pre&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Frequency log file&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
[[Media:Hyc116_bbr3_freq.log]]&lt;br /&gt;
&lt;br /&gt;
Attached above is the frequency file saved onto the computer from the SCAN server portal. The frequency file was also published on the chemistry database DSpace. {{DOI|10042/202442}}&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Frequencies&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;pre&amp;gt;&lt;br /&gt;
Low frequencies ---   -0.0137   -0.0064   -0.0046    2.4315    2.4315    4.8421&lt;br /&gt;
Low frequencies ---  155.9631  155.9651  267.7052&lt;br /&gt;
&amp;lt;/pre&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;jmol of BBr&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;&#039;&#039;&#039;&lt;br /&gt;
&amp;lt;jmol&amp;gt;&amp;lt;jmolApplet&amp;gt;&lt;br /&gt;
  &amp;lt;title&amp;gt;optimised BBr3&amp;lt;/title&amp;gt;&lt;br /&gt;
  &amp;lt;color&amp;gt;black&amp;lt;/color&amp;gt;&lt;br /&gt;
  &amp;lt;size&amp;gt;200&amp;lt;/size&amp;gt;&lt;br /&gt;
  &amp;lt;uploadedFileContents&amp;gt;Hyc116_bbr3_freq.log&amp;lt;/uploadedFileContents&amp;gt;&lt;br /&gt;
&amp;lt;/jmolApplet&amp;gt;&amp;lt;/jmol&amp;gt;&lt;br /&gt;
&lt;br /&gt;
==Aromaticity==&lt;br /&gt;
&lt;br /&gt;
===Benzene===&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;Calculation type&amp;lt;/b&amp;gt;: Optimisation&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;Calculation Method&amp;lt;/b&amp;gt;: B3LYP&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;Basis set&amp;lt;/b&amp;gt;: 6-31G(d,p) &lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Summary table&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
[[file:Hyc116_c6h6_summarytable.png]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Items table&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;pre&amp;gt;&lt;br /&gt;
Item               Value     Threshold  Converged?&lt;br /&gt;
 Maximum Force            0.000193     0.000450     YES&lt;br /&gt;
 RMS     Force            0.000079     0.000300     YES&lt;br /&gt;
 Maximum Displacement     0.000830     0.001800     YES&lt;br /&gt;
 RMS     Displacement     0.000294     0.001200     YES&lt;br /&gt;
&amp;lt;/pre&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Frequency log file&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
[[Media:HYC116_C6H6_FREQ.LOG]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Frequencies&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;pre&amp;gt;&lt;br /&gt;
Low frequencies ---   -3.5606   -3.5606   -0.0089   -0.0043   -0.0043   10.0905&lt;br /&gt;
Low frequencies ---  413.9582  413.9582  621.1416&lt;br /&gt;
&amp;lt;/pre&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;jmol of C&amp;lt;sub&amp;gt;6&amp;lt;/sub&amp;gt;H&amp;lt;sub&amp;gt;6&amp;lt;/sub&amp;gt;&#039;&#039;&#039;&lt;br /&gt;
&amp;lt;jmol&amp;gt;&amp;lt;jmolApplet&amp;gt;&lt;br /&gt;
  &amp;lt;title&amp;gt;optimised Benzene&amp;lt;/title&amp;gt;&lt;br /&gt;
  &amp;lt;color&amp;gt;black&amp;lt;/color&amp;gt;&lt;br /&gt;
  &amp;lt;size&amp;gt;200&amp;lt;/size&amp;gt;&lt;br /&gt;
  &amp;lt;uploadedFileContents&amp;gt;HYC116_C6H6_FREQ.LOG&amp;lt;/uploadedFileContents&amp;gt;&lt;br /&gt;
&amp;lt;/jmolApplet&amp;gt;&amp;lt;/jmol&amp;gt;&lt;br /&gt;
&lt;br /&gt;
===Borazine===&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;Calculation type&amp;lt;/b&amp;gt;: Optimisation&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;Calculation Method&amp;lt;/b&amp;gt;: B3LYP&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;Basis set&amp;lt;/b&amp;gt;: 6-31G(d,p) &lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Summary table&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
[[file:Hyc116_borazine_summarytable.png]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Items table&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;pre&amp;gt;&lt;br /&gt;
Item               Value     Threshold  Converged?&lt;br /&gt;
 Maximum Force            0.000085     0.000450     YES&lt;br /&gt;
 RMS     Force            0.000033     0.000300     YES&lt;br /&gt;
 Maximum Displacement     0.000250     0.001800     YES&lt;br /&gt;
 RMS     Displacement     0.000074     0.001200     YES&lt;br /&gt;
&amp;lt;/pre&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Frequency log file&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
[[Media:HYC116_BORAZINE_FREQ.LOG]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Frequencies&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;pre&amp;gt;&lt;br /&gt;
Low frequencies ---  -12.6626  -12.6626   -8.9272   -0.0211   -0.0104   -0.0104&lt;br /&gt;
Low frequencies ---  289.1112  289.1112  403.8613&lt;br /&gt;
&amp;lt;/pre&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;jmol of Borazine&#039;&#039;&#039;&lt;br /&gt;
&amp;lt;jmol&amp;gt;&amp;lt;jmolApplet&amp;gt;&lt;br /&gt;
  &amp;lt;title&amp;gt;optimised Borazine&amp;lt;/title&amp;gt;&lt;br /&gt;
  &amp;lt;color&amp;gt;black&amp;lt;/color&amp;gt;&lt;br /&gt;
  &amp;lt;size&amp;gt;200&amp;lt;/size&amp;gt;&lt;br /&gt;
  &amp;lt;uploadedFileContents&amp;gt;HYC116_BORAZINE_FREQ.LOG&amp;lt;/uploadedFileContents&amp;gt;&lt;br /&gt;
&amp;lt;/jmolApplet&amp;gt;&amp;lt;/jmol&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
===Charge distribution===&lt;br /&gt;
&lt;br /&gt;
An NBO charge analysis was carried out on both the optimised benzene and borazine. Visualisations of the charge distribution are shown in the table below, with the colour range going from -1.102 to 1.102 for both molecule. This large scale was chosen as it allows direct comparison of the charge on any atoms in these two molecules and shows the relative magnitude of charges on all these atoms. Negative charges are shown in red, and positive charges are shown in green. A neutral charge is displayed in black, so the smaller a charge is (positive or negative), the darker its colour representation is. Larger charges are shown in brighter colours. The charges are also displayed on the atoms as numbers with a neutral charge being zero. Negative charges are shown as negative number and positive charges are shown as positive numbers. &lt;br /&gt;
&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot;&lt;br /&gt;
!&lt;br /&gt;
!Benzene&lt;br /&gt;
!Borazine&lt;br /&gt;
|-&lt;br /&gt;
!Visualisation of charge distribution&lt;br /&gt;
|[[File:Hyc116_benzene_charge_distribution1.png|500x500px|thumb|centre|Charge distribution of Benzene visualisation]]&lt;br /&gt;
|[[File:Hyc116_borazine_charge_distribution1.png|500x500px|thumb|centre|Charge distribution of Borazine visualisation]]&lt;br /&gt;
|-&lt;br /&gt;
!Charge &lt;br /&gt;
|Carbon: -0.239&lt;br /&gt;
&lt;br /&gt;
Hydrogen: 0.239&lt;br /&gt;
|Nitrogen: -1.102 &lt;br /&gt;
&lt;br /&gt;
Boron: 0.747&lt;br /&gt;
&lt;br /&gt;
Hydrogen (bonded to N): 0.432&lt;br /&gt;
&lt;br /&gt;
Hydrogen (bonded to B): -0.077&lt;br /&gt;
|-&lt;br /&gt;
!Discussion&lt;br /&gt;
|From the visualisation, it is shown that there is a slightly negative charge on the carbon atoms, and a positive charge of the same magnitude on the hydrogen atoms. All the carbon atoms have the same charge as they are in identical environments. The same applies to all the hydrogen atoms. This is due to the highly symmetrical structure of benzene. Since the same colour scale was used for both benzene and borazine, and the charges are much smaller in magnitude on atoms in benzene than atoms on borazine, the colours on the charge distribution visualisation is much darker. &lt;br /&gt;
|From the colours displayed on the charge distribution visualisation as well as the charge values, it is shown that nitrogen has a relatively large negative charge, while boron has a positive charge. This is due to the difference in electrogenativity between these atoms: nitrogen atoms are more electronegative than boron and tends to attract electrons towards themselves. It is worth noting that the hydrogen atoms do not all have the same charge. The hydrogen atoms bonded to boron have a slightly negative charge, and the ones bonded to nitrogen have a small positive charge. &lt;br /&gt;
&lt;br /&gt;
The fact that the same colour scale was used for both molecules comes in helpful here. It allows the charges on atoms to be compared directly. For example, just from looking at the colours, one can tell that or example, even though both carbon and nitrogen are electronegative, nitrogen is much more electronegative, which is quantitatively shown by Pauling&#039;s electronegativity scale.&amp;lt;ref&amp;gt;http://www.tutor-homework.com/Chemistry_Help/electronegativity_table/electronegativity.html (Date accessed: 24.0502018&amp;lt;/ref&amp;gt;&lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
===Comparative MOs of Benzene and Borazine===&lt;br /&gt;
&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot;&lt;br /&gt;
!&lt;br /&gt;
!Benzene&lt;br /&gt;
!Borazine&lt;br /&gt;
!Comparison and Discussion&lt;br /&gt;
|-&lt;br /&gt;
!1st comparative pair&lt;br /&gt;
|[[File:Hyc116_benzene_1st_MO_pair_7.png|200x200px|centre]]&lt;br /&gt;
|[[File:Hyc116_borazine_1st_MO_pair_level9.png|200x200px|centre]]&lt;br /&gt;
|MO 9 of both benzene and borazine are comparable. They both show delocalised molecular orbital with an overall bonding character. There is a nodal plane across the molecular orbitals for both benzene and borazine. For benzene, there is contribution from all the carbon and hydrogen s orbitals. Moreover, the molecular orbitals are symmetric to their counterpart of opposite phase. That is not the case for borazine; they are less symmetric in borazine. Nitrogen atoms are more electronegative than boron atoms and pull electron density towards themselves, resulting in a larger MO. There is contribution from all the boron and nitrogen s orbitals, and three of the hydrogen s orbitals, though not all of them. &lt;br /&gt;
|-&lt;br /&gt;
!2nd comparative pair&lt;br /&gt;
|[[File:Hyc116_benzene_2nd_MO_pair_10.png|200x200px|centre]]&lt;br /&gt;
|[[File:Hyc116_borazine_2nd_MO_pair_level11.png|200x200px|centre]]&lt;br /&gt;
|&lt;br /&gt;
|-&lt;br /&gt;
!3rd comparative pair&lt;br /&gt;
|[[File:Hyc116_benzene_3rd_MO_pair_21.png|200x200px|centre]]&lt;br /&gt;
|[[File:Hyc116_borazine_3rd_MO_pair_level21.png|200x200px|centre]]&lt;br /&gt;
|&lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
===Aromaticity: some theories===&lt;br /&gt;
&lt;br /&gt;
==References==&lt;/div&gt;</summary>
		<author><name>Hyc116</name></author>
	</entry>
	<entry>
		<id>https://chemwiki.ch.ic.ac.uk/index.php?title=MO_hyc116&amp;diff=730159</id>
		<title>MO hyc116</title>
		<link rel="alternate" type="text/html" href="https://chemwiki.ch.ic.ac.uk/index.php?title=MO_hyc116&amp;diff=730159"/>
		<updated>2018-05-24T17:32:47Z</updated>

		<summary type="html">&lt;p&gt;Hyc116: &lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;==BH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;==&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;Calculation type&amp;lt;/b&amp;gt;: Optimisation&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;Calculation Method&amp;lt;/b&amp;gt;: B3LYP&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;Basis set&amp;lt;/b&amp;gt;: 6-31G(d,p) &lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Summary table&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
[[file:Hyc116_bh3_631g_opt_summarytable.png]]&lt;br /&gt;
&lt;br /&gt;
The above summary table was obtained after the 2nd optimisation of BH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt; (after the initial optimisation using the 3-21G basis set). Notice how the symmetry is incorrect and shown as Cs. This is because the symmetry was manually broken at the beginning by changing the bond length of B-H bonds. The point group was manually adjusted and the molecule was optimised again before the frequency analysis and the new summary table is attached below.&lt;br /&gt;
&lt;br /&gt;
[[file:Hyc116_bh3_correctsummarytable.png]]&lt;br /&gt;
&lt;br /&gt;
The above summary table was obtained from the optimisation after adjusting the symmetry. The point shown in this summary table is D&amp;lt;sub&amp;gt;3h&amp;lt;/sub&amp;gt;, which is the correct for BH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;. &lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Items table&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
Below is the items table taken from the optimisation with the correct point group.&lt;br /&gt;
&lt;br /&gt;
&amp;lt;pre&amp;gt;&lt;br /&gt;
Item               Value     Threshold  Converged?&lt;br /&gt;
 Maximum Force            0.000015     0.000450     YES&lt;br /&gt;
 RMS     Force            0.000010     0.000300     YES&lt;br /&gt;
 Maximum Displacement     0.000058     0.001800     YES&lt;br /&gt;
 RMS     Displacement     0.000038     0.001200     YES&lt;br /&gt;
&amp;lt;/pre&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Frequency log file&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
[[Media:HYC116 BH3 FREQ.LOG]] &lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Frequencies&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;pre&amp;gt;&lt;br /&gt;
Low frequencies ---  -10.3498   -3.4492   -1.2454   -0.0055    0.4779    3.2165&lt;br /&gt;
Low frequencies --- 1162.9519 1213.1527 1213.1554&lt;br /&gt;
&amp;lt;/pre&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;jmol of BH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;&#039;&#039;&#039;&lt;br /&gt;
&amp;lt;jmol&amp;gt;&amp;lt;jmolApplet&amp;gt;&lt;br /&gt;
  &amp;lt;title&amp;gt;optimised BH3&amp;lt;/title&amp;gt;&lt;br /&gt;
  &amp;lt;color&amp;gt;black&amp;lt;/color&amp;gt;&lt;br /&gt;
  &amp;lt;size&amp;gt;200&amp;lt;/size&amp;gt;&lt;br /&gt;
  &amp;lt;uploadedFileContents&amp;gt;HYC116_BH3_FREQ.LOG&amp;lt;/uploadedFileContents&amp;gt;&lt;br /&gt;
&amp;lt;/jmolApplet&amp;gt;&amp;lt;/jmol&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
===Vibrational spectrum===&lt;br /&gt;
&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot;&lt;br /&gt;
!wavenumber (cm&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;)&lt;br /&gt;
!Intensity (arbitrary units)&lt;br /&gt;
!symmetry&lt;br /&gt;
!IR active?&lt;br /&gt;
!type&lt;br /&gt;
|-&lt;br /&gt;
|1163&lt;br /&gt;
|93&lt;br /&gt;
|A&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;&#039; &#039;&lt;br /&gt;
|Yes&lt;br /&gt;
|Out of plane bend&lt;br /&gt;
|-&lt;br /&gt;
|1213&lt;br /&gt;
|14&lt;br /&gt;
|E&#039;&lt;br /&gt;
|Very slight&lt;br /&gt;
|Bend&lt;br /&gt;
|-&lt;br /&gt;
|1213&lt;br /&gt;
|14&lt;br /&gt;
|E&#039;&lt;br /&gt;
|Very slight&lt;br /&gt;
|Bend&lt;br /&gt;
|-&lt;br /&gt;
|2582&lt;br /&gt;
|0&lt;br /&gt;
|A&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;&#039;&lt;br /&gt;
|No&lt;br /&gt;
|Symmetric stretch&lt;br /&gt;
|-&lt;br /&gt;
|2716&lt;br /&gt;
|126&lt;br /&gt;
|E&#039;&lt;br /&gt;
|Yes&lt;br /&gt;
|Asymmetric stretch&lt;br /&gt;
|-&lt;br /&gt;
|2716&lt;br /&gt;
|126&lt;br /&gt;
|E&#039;&lt;br /&gt;
|Yes&lt;br /&gt;
|Asymmetric stretch&lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;IR spectrum&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
[[file:Hyc116_ir_bh3.png|400*600]]&lt;br /&gt;
&lt;br /&gt;
There are only three peaks on the IR spectrum of BH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;, despite that there are 6 vibrational modes for the molecule. As shown in the table above, the symmetric stretching mode with A1 symmetry at 2582 cm&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt; is not IR active; naturally, that vibrational mode doesn’t give a peak on the IR spectrum. As shown from the table, two pairs of vibrational modes, the bond angle deformation/bend at 1213 cm&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt; and the asymmetric bond stretch at 2716 cm&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;, are degenerate with the symmetry label E. This means that they have the same energy, and hence give the same wavenumber on the IR spectrum. Each pair of degenerate vibrational modes give rise to one peak. This leaves three peaks, as confirmed by the IR spectrum above.&lt;br /&gt;
&lt;br /&gt;
===Molecular orbitals of BH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;===&lt;br /&gt;
&lt;br /&gt;
[[file:hyc116_bh3_MO_diagram.png]]&lt;br /&gt;
&lt;br /&gt;
The above molecular orbital diagram was taken from Dr Patricia Hunt&#039;s &amp;lt;i&amp;gt;Lecture 4 Tutorial Problem Model Answers&amp;lt;/i&amp;gt;. &amp;lt;ref&amp;gt;P. Hunt, &amp;quot;Lecture 4 Tutorial Problem Model Answers&amp;quot;, 2 (2018)&amp;lt;/ref&amp;gt;. Diagrams of the &amp;quot;real&amp;quot; MOs were obtained from Gaussian.&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
There is no significant difference between the LCAO MOs and the real ones. Features such as orbital phases are shown clearly on both the LCAO MOs and the real MOs, illustrating the bonding/anti-bonding characters of the molecular orbitals. This suggests that the the qualitative MO theory is highly accurate and useful when studying the molecular orbitals of molecules.&lt;br /&gt;
&lt;br /&gt;
==Associated energies: ammonium borane==&lt;br /&gt;
&lt;br /&gt;
===NH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;===&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;Calculation type&amp;lt;/b&amp;gt;: Optimisation&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;Calculation Method&amp;lt;/b&amp;gt;: B3LYP&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;Basis set&amp;lt;/b&amp;gt;: 6-31G(d,p) &lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Summary table&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
[[file:Hyc116_nh3_631g_summarytable.png]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Items table&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;pre&amp;gt;&lt;br /&gt;
Item               Value     Threshold  Converged?&lt;br /&gt;
 Maximum Force            0.000006     0.000450     YES&lt;br /&gt;
 RMS     Force            0.000004     0.000300     YES&lt;br /&gt;
 Maximum Displacement     0.000012     0.001800     YES&lt;br /&gt;
 RMS     Displacement     0.000008     0.001200     YES&lt;br /&gt;
&amp;lt;/pre&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Frequency log file&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
[[Media:HYC116_NH3_FREQ.LOG]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Frequencies&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;pre&amp;gt;&lt;br /&gt;
Low frequencies ---   -8.5646   -8.5588   -0.0047    0.0454    0.1784   26.4183&lt;br /&gt;
Low frequencies --- 1089.7603 1694.1865 1694.1865&lt;br /&gt;
&amp;lt;/pre&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;jmol of NH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;&#039;&#039;&#039;&lt;br /&gt;
&amp;lt;jmol&amp;gt;&amp;lt;jmolApplet&amp;gt;&lt;br /&gt;
  &amp;lt;title&amp;gt;optimised NH3&amp;lt;/title&amp;gt;&lt;br /&gt;
  &amp;lt;color&amp;gt;black&amp;lt;/color&amp;gt;&lt;br /&gt;
  &amp;lt;size&amp;gt;200&amp;lt;/size&amp;gt;&lt;br /&gt;
  &amp;lt;uploadedFileContents&amp;gt;HYC116_NH3_FREQ.LOG&amp;lt;/uploadedFileContents&amp;gt;&lt;br /&gt;
&amp;lt;/jmolApplet&amp;gt;&amp;lt;/jmol&amp;gt;&lt;br /&gt;
&lt;br /&gt;
===NH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;BH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;===&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;Calculation type&amp;lt;/b&amp;gt;: Optimisation&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;Calculation Method&amp;lt;/b&amp;gt;: B3LYP&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;Basis set&amp;lt;/b&amp;gt;: 6-31G(d,p) &lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Summary table&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
[[file:Hyc116_nh3bh3_631g_summarytable.png]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Items table&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;pre&amp;gt;&lt;br /&gt;
Item               Value     Threshold  Converged?&lt;br /&gt;
 Maximum Force            0.000123     0.000450     YES&lt;br /&gt;
 RMS     Force            0.000058     0.000300     YES&lt;br /&gt;
 Maximum Displacement     0.000515     0.001800     YES&lt;br /&gt;
 RMS     Displacement     0.000296     0.001200     YES&lt;br /&gt;
&amp;lt;/pre&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Frequency log file&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
[[Media:HYC116_NH3BH3_FREQ.LOG]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Frequencies&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;pre&amp;gt;&lt;br /&gt;
Low frequencies ---   -0.0014   -0.0011   -0.0006    6.9624   20.4518   43.5542&lt;br /&gt;
Low frequencies ---  266.4530  632.2458  639.0504&lt;br /&gt;
&amp;lt;/pre&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;jmol of NH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;BH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;&#039;&#039;&#039;&lt;br /&gt;
&amp;lt;jmol&amp;gt;&amp;lt;jmolApplet&amp;gt;&lt;br /&gt;
  &amp;lt;title&amp;gt;optimised NH3BH3&amp;lt;/title&amp;gt;&lt;br /&gt;
  &amp;lt;color&amp;gt;black&amp;lt;/color&amp;gt;&lt;br /&gt;
  &amp;lt;size&amp;gt;200&amp;lt;/size&amp;gt;&lt;br /&gt;
  &amp;lt;uploadedFileContents&amp;gt;HYC116_NH3BH3_FREQ.LOG&amp;lt;/uploadedFileContents&amp;gt;&lt;br /&gt;
&amp;lt;/jmolApplet&amp;gt;&amp;lt;/jmol&amp;gt;&lt;br /&gt;
&lt;br /&gt;
===Association energy===&lt;br /&gt;
&lt;br /&gt;
E(BH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;) (using the optimisation with the correct symmetry) = -26.61532363 a.u. = &amp;lt;b&amp;gt;-26.61532 a.u. (5 d.p.)&amp;lt;/b&amp;gt;&lt;br /&gt;
&lt;br /&gt;
E(NH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;) = -56.55776873 a.u. = &amp;lt;b&amp;gt;-56.55777 a.u. (5 d.p.)&amp;lt;/b&amp;gt;&lt;br /&gt;
&lt;br /&gt;
E(NH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;BH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;) = -83.22468893 a.u. = &amp;lt;b&amp;gt;-83.22469 a.u. (5 d.p.)&amp;lt;/b&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
Carrying out calculations using numbers which has already been rounded up can possibly result in errors in the last digit. Hence, here the calculations were carried out using the numbers provided from the optimisations (i.e. with more decimal places than necessary); the answer was then rounded up to the desired accuracy. &lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
ΔE = E(NH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;BH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;)-[E(NH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;)+E(BH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;)]&lt;br /&gt;
&lt;br /&gt;
ΔE = -83.22468893 - (-56.55776873 + -26.61532363) = -0.05159657 a.u. &lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;ΔE = -0.05160 a.u. (5 d.p.)&amp;lt;/b&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Converting energy from a.u. to kJ/mol&#039;&#039;&#039;&lt;br /&gt;
An atomic unit for energy is Hartree, which is equal to 2625.5 kJ/mol. &amp;lt;ref&amp;gt;https://cccbdb.nist.gov/hartree.asp (Accessed: 22.05.2018)&amp;lt;/ref&amp;gt;&lt;br /&gt;
&lt;br /&gt;
So ΔE in kJ/mol = -0.05159657 * 2625.5 = -135.466794535 kJ/mol&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;ΔE = -135 kJ/mol (nearest integer)&amp;lt;/b&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
The energy difference calculated above comes from the formation of the B-N dative bond. It is a relatively weak bond. According to a bond energy data sheet provided by the University of California, &amp;lt;ref&amp;gt;https://labs.chem.ucsb.edu/zakarian/armen/11---bonddissociationenergy.pdf (Accessed on 24.05.2018)&amp;lt;/ref&amp;gt; the bond energy of the C-C bond of an ethane molecule is 368 kJ/mol. This is a fair comparison to the NH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;BH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt; molecule as the two molecules have the same structure, only with the carbon atoms on ethane swapped for Boron and Nitrogen in NH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;BH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;&lt;br /&gt;
&lt;br /&gt;
==Using a mixture of basis-sets and pseudo-potentials==&lt;br /&gt;
&lt;br /&gt;
===BBr&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;===&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;Calculation type&amp;lt;/b&amp;gt;: Optimisation&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;Calculation Method&amp;lt;/b&amp;gt;: B3LYP&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;Basis set&amp;lt;/b&amp;gt;: Boron: 6-31G(d,p) ; Br: LANL2DZ&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
Larger calculations are often sent to a web-server to run on a high-performance computer instead of a desktop. In order to experience and learn to use a web-server, the optimisation and the frequency analysis for BBr&amp;lt;sub&amp;gt;3&amp;lt;/sub were both sent and done on a server instead of the desktop. The calculation results were downloaded from the web-server once they were finished.   &lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Summary table&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
[[file:Hyc116_bbr3_opt_summarytable.png]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Items table&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;pre&amp;gt;&lt;br /&gt;
Item               Value     Threshold  Converged?&lt;br /&gt;
 Maximum Force            0.000008     0.000450     YES&lt;br /&gt;
 RMS     Force            0.000005     0.000300     YES&lt;br /&gt;
 Maximum Displacement     0.000036     0.001800     YES&lt;br /&gt;
 RMS     Displacement     0.000023     0.001200     YES&lt;br /&gt;
&amp;lt;/pre&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Frequency log file&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
[[Media:Hyc116_bbr3_freq.log]]&lt;br /&gt;
&lt;br /&gt;
Attached above is the frequency file saved onto the computer from the SCAN server portal. The frequency file was also published on the chemistry database DSpace. {{DOI|10042/202442}}&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Frequencies&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;pre&amp;gt;&lt;br /&gt;
Low frequencies ---   -0.0137   -0.0064   -0.0046    2.4315    2.4315    4.8421&lt;br /&gt;
Low frequencies ---  155.9631  155.9651  267.7052&lt;br /&gt;
&amp;lt;/pre&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;jmol of BBr&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;&#039;&#039;&#039;&lt;br /&gt;
&amp;lt;jmol&amp;gt;&amp;lt;jmolApplet&amp;gt;&lt;br /&gt;
  &amp;lt;title&amp;gt;optimised BBr3&amp;lt;/title&amp;gt;&lt;br /&gt;
  &amp;lt;color&amp;gt;black&amp;lt;/color&amp;gt;&lt;br /&gt;
  &amp;lt;size&amp;gt;200&amp;lt;/size&amp;gt;&lt;br /&gt;
  &amp;lt;uploadedFileContents&amp;gt;Hyc116_bbr3_freq.log&amp;lt;/uploadedFileContents&amp;gt;&lt;br /&gt;
&amp;lt;/jmolApplet&amp;gt;&amp;lt;/jmol&amp;gt;&lt;br /&gt;
&lt;br /&gt;
==Aromaticity==&lt;br /&gt;
&lt;br /&gt;
===Benzene===&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;Calculation type&amp;lt;/b&amp;gt;: Optimisation&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;Calculation Method&amp;lt;/b&amp;gt;: B3LYP&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;Basis set&amp;lt;/b&amp;gt;: 6-31G(d,p) &lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Summary table&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
[[file:Hyc116_c6h6_summarytable.png]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Items table&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;pre&amp;gt;&lt;br /&gt;
Item               Value     Threshold  Converged?&lt;br /&gt;
 Maximum Force            0.000193     0.000450     YES&lt;br /&gt;
 RMS     Force            0.000079     0.000300     YES&lt;br /&gt;
 Maximum Displacement     0.000830     0.001800     YES&lt;br /&gt;
 RMS     Displacement     0.000294     0.001200     YES&lt;br /&gt;
&amp;lt;/pre&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Frequency log file&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
[[Media:HYC116_C6H6_FREQ.LOG]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Frequencies&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;pre&amp;gt;&lt;br /&gt;
Low frequencies ---   -3.5606   -3.5606   -0.0089   -0.0043   -0.0043   10.0905&lt;br /&gt;
Low frequencies ---  413.9582  413.9582  621.1416&lt;br /&gt;
&amp;lt;/pre&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;jmol of C&amp;lt;sub&amp;gt;6&amp;lt;/sub&amp;gt;H&amp;lt;sub&amp;gt;6&amp;lt;/sub&amp;gt;&#039;&#039;&#039;&lt;br /&gt;
&amp;lt;jmol&amp;gt;&amp;lt;jmolApplet&amp;gt;&lt;br /&gt;
  &amp;lt;title&amp;gt;optimised Benzene&amp;lt;/title&amp;gt;&lt;br /&gt;
  &amp;lt;color&amp;gt;black&amp;lt;/color&amp;gt;&lt;br /&gt;
  &amp;lt;size&amp;gt;200&amp;lt;/size&amp;gt;&lt;br /&gt;
  &amp;lt;uploadedFileContents&amp;gt;HYC116_C6H6_FREQ.LOG&amp;lt;/uploadedFileContents&amp;gt;&lt;br /&gt;
&amp;lt;/jmolApplet&amp;gt;&amp;lt;/jmol&amp;gt;&lt;br /&gt;
&lt;br /&gt;
===Borazine===&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;Calculation type&amp;lt;/b&amp;gt;: Optimisation&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;Calculation Method&amp;lt;/b&amp;gt;: B3LYP&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;Basis set&amp;lt;/b&amp;gt;: 6-31G(d,p) &lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Summary table&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
[[file:Hyc116_borazine_summarytable.png]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Items table&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;pre&amp;gt;&lt;br /&gt;
Item               Value     Threshold  Converged?&lt;br /&gt;
 Maximum Force            0.000085     0.000450     YES&lt;br /&gt;
 RMS     Force            0.000033     0.000300     YES&lt;br /&gt;
 Maximum Displacement     0.000250     0.001800     YES&lt;br /&gt;
 RMS     Displacement     0.000074     0.001200     YES&lt;br /&gt;
&amp;lt;/pre&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Frequency log file&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
[[Media:HYC116_BORAZINE_FREQ.LOG]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Frequencies&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;pre&amp;gt;&lt;br /&gt;
Low frequencies ---  -12.6626  -12.6626   -8.9272   -0.0211   -0.0104   -0.0104&lt;br /&gt;
Low frequencies ---  289.1112  289.1112  403.8613&lt;br /&gt;
&amp;lt;/pre&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;jmol of Borazine&#039;&#039;&#039;&lt;br /&gt;
&amp;lt;jmol&amp;gt;&amp;lt;jmolApplet&amp;gt;&lt;br /&gt;
  &amp;lt;title&amp;gt;optimised Borazine&amp;lt;/title&amp;gt;&lt;br /&gt;
  &amp;lt;color&amp;gt;black&amp;lt;/color&amp;gt;&lt;br /&gt;
  &amp;lt;size&amp;gt;200&amp;lt;/size&amp;gt;&lt;br /&gt;
  &amp;lt;uploadedFileContents&amp;gt;HYC116_BORAZINE_FREQ.LOG&amp;lt;/uploadedFileContents&amp;gt;&lt;br /&gt;
&amp;lt;/jmolApplet&amp;gt;&amp;lt;/jmol&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
===Charge distribution===&lt;br /&gt;
&lt;br /&gt;
An NBO charge analysis was carried out on both the optimised benzene and borazine. Visualisations of the charge distribution are shown in the table below, with the colour range going from -1.102 to 1.102 for both molecule. This large scale was chosen as it allows direct comparison of the charge on any atoms in these two molecules and shows the relative magnitude of charges on all these atoms. Negative charges are shown in red, and positive charges are shown in green. A neutral charge is displayed in black, so the smaller a charge is (positive or negative), the darker its colour representation is. Larger charges are shown in brighter colours. The charges are also displayed on the atoms as numbers with a neutral charge being zero. Negative charges are shown as negative number and positive charges are shown as positive numbers. &lt;br /&gt;
&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot;&lt;br /&gt;
!&lt;br /&gt;
!Benzene&lt;br /&gt;
!Borazine&lt;br /&gt;
|-&lt;br /&gt;
!Visualisation of charge distribution&lt;br /&gt;
|[[File:Hyc116_benzene_charge_distribution1.png|500x500px|thumb|centre|Charge distribution of Benzene visualisation]]&lt;br /&gt;
|[[File:Hyc116_borazine_charge_distribution1.png|500x500px|thumb|centre|Charge distribution of Borazine visualisation]]&lt;br /&gt;
|-&lt;br /&gt;
!Charge &lt;br /&gt;
|Carbon: -0.239&lt;br /&gt;
&lt;br /&gt;
Hydrogen: 0.239&lt;br /&gt;
|Nitrogen: -1.102 &lt;br /&gt;
&lt;br /&gt;
Boron: 0.747&lt;br /&gt;
&lt;br /&gt;
Hydrogen (bonded to N): 0.432&lt;br /&gt;
&lt;br /&gt;
Hydrogen (bonded to B): -0.077&lt;br /&gt;
|-&lt;br /&gt;
!Discussion&lt;br /&gt;
|From the visualisation, it is shown that there is a slightly negative charge on the carbon atoms, and a positive charge of the same magnitude on the hydrogen atoms. All the carbon atoms have the same charge as they are in identical environments. The same applies to all the hydrogen atoms. This is due to the highly symmetrical structure of benzene. Since the same colour scale was used for both benzene and borazine, and the charges are much smaller in magnitude on atoms in benzene than atoms on borazine, the colours on the charge distribution visualisation is much darker. &lt;br /&gt;
|From the colours displayed on the charge distribution visualisation as well as the charge values, it is shown that nitrogen has a relatively large negative charge, while boron has a positive charge. This is due to the difference in electrogenativity between these atoms: nitrogen atoms are more electronegative than boron and tends to attract electrons towards themselves. It is worth noting that the hydrogen atoms do not all have the same charge. The hydrogen atoms bonded to boron have a slightly negative charge, and the ones bonded to nitrogen have a small positive charge. &lt;br /&gt;
&lt;br /&gt;
The fact that the same colour scale was used for both molecules comes in helpful here. It allows the charges on atoms to be compared directly. For example, just from looking at the colours, one can tell that or example, even though both carbon and nitrogen are electronegative, nitrogen is much more electronegative, which is quantitatively shown by Pauling&#039;s electronegativity scale.&amp;lt;ref&amp;gt;http://www.tutor-homework.com/Chemistry_Help/electronegativity_table/electronegativity.html (Date accessed: 24.0502018&amp;lt;/ref&amp;gt;&lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
===Comparative MOs of Benzene and Borazine===&lt;br /&gt;
&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot;&lt;br /&gt;
!&lt;br /&gt;
!Benzene&lt;br /&gt;
!Borazine&lt;br /&gt;
!Comparison and Discussion&lt;br /&gt;
|-&lt;br /&gt;
!1st comparative pair&lt;br /&gt;
|[[File:Hyc116_benzene_1st_MO_pair_7.png|200x200px|centre]]&lt;br /&gt;
|[[File:Hyc116_borazine_1st_MO_pair_level9.png|200x200px|centre]]&lt;br /&gt;
|MO 9 of both benzene and borazine are comparable. They both show delocalised molecular orbital with an overall bonding character. There is a nodal plane across the molecular orbitals for both benzene and borazine. For benzene, there is contribution from all the carbon and hydrogen s orbitals. Moreover, the molecular orbitals are symmetric to their counterpart of opposite phase. That is not the case for borazine; they are less symmetric in borazine. Nitrogen atoms are more electronegative than boron atoms and pull electron density towards themselves, resulting in a larger MO. There is contribution from all the boron and nitrogen s orbitals, and three of the hydrogen s orbitals, though not all of them. &lt;br /&gt;
|-&lt;br /&gt;
!2nd comparative pair&lt;br /&gt;
|[[File:Hyc116_benzene_2nd_MO_pair_10.png|200x200px|centre]]&lt;br /&gt;
|[[File:Hyc116_borazine_2nd_MO_pair_level11.png|200x200px|centre]]&lt;br /&gt;
|&lt;br /&gt;
|-&lt;br /&gt;
!3rd comparative pair&lt;br /&gt;
|[[File:Hyc116_benzene_3rd_MO_pair_21.png|200x200px|centre]]&lt;br /&gt;
|[[File:Hyc116_borazine_3rd_MO_pair_level21.png|200x200px|centre]]&lt;br /&gt;
|&lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
===Aromaticity: some theories===&lt;/div&gt;</summary>
		<author><name>Hyc116</name></author>
	</entry>
	<entry>
		<id>https://chemwiki.ch.ic.ac.uk/index.php?title=MO_hyc116&amp;diff=730157</id>
		<title>MO hyc116</title>
		<link rel="alternate" type="text/html" href="https://chemwiki.ch.ic.ac.uk/index.php?title=MO_hyc116&amp;diff=730157"/>
		<updated>2018-05-24T17:32:31Z</updated>

		<summary type="html">&lt;p&gt;Hyc116: &lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;==BH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;==&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;Calculation type&amp;lt;/b&amp;gt;: Optimisation&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;Calculation Method&amp;lt;/b&amp;gt;: B3LYP&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;Basis set&amp;lt;/b&amp;gt;: 6-31G(d,p) &lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Summary table&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
[[file:Hyc116_bh3_631g_opt_summarytable.png]]&lt;br /&gt;
&lt;br /&gt;
The above summary table was obtained after the 2nd optimisation of BH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt; (after the initial optimisation using the 3-21G basis set). Notice how the symmetry is incorrect and shown as Cs. This is because the symmetry was manually broken at the beginning by changing the bond length of B-H bonds. The point group was manually adjusted and the molecule was optimised again before the frequency analysis and the new summary table is attached below.&lt;br /&gt;
&lt;br /&gt;
[[file:Hyc116_bh3_correctsummarytable.png]]&lt;br /&gt;
&lt;br /&gt;
The above summary table was obtained from the optimisation after adjusting the symmetry. The point shown in this summary table is D&amp;lt;sub&amp;gt;3h&amp;lt;/sub&amp;gt;, which is the correct for BH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;. &lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Items table&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
Below is the items table taken from the optimisation with the correct point group.&lt;br /&gt;
&lt;br /&gt;
&amp;lt;pre&amp;gt;&lt;br /&gt;
Item               Value     Threshold  Converged?&lt;br /&gt;
 Maximum Force            0.000015     0.000450     YES&lt;br /&gt;
 RMS     Force            0.000010     0.000300     YES&lt;br /&gt;
 Maximum Displacement     0.000058     0.001800     YES&lt;br /&gt;
 RMS     Displacement     0.000038     0.001200     YES&lt;br /&gt;
&amp;lt;/pre&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Frequency log file&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
[[Media:HYC116 BH3 FREQ.LOG]] &lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Frequencies&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;pre&amp;gt;&lt;br /&gt;
Low frequencies ---  -10.3498   -3.4492   -1.2454   -0.0055    0.4779    3.2165&lt;br /&gt;
Low frequencies --- 1162.9519 1213.1527 1213.1554&lt;br /&gt;
&amp;lt;/pre&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;jmol of BH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;&#039;&#039;&#039;&lt;br /&gt;
&amp;lt;jmol&amp;gt;&amp;lt;jmolApplet&amp;gt;&lt;br /&gt;
  &amp;lt;title&amp;gt;optimised BH3&amp;lt;/title&amp;gt;&lt;br /&gt;
  &amp;lt;color&amp;gt;black&amp;lt;/color&amp;gt;&lt;br /&gt;
  &amp;lt;size&amp;gt;200&amp;lt;/size&amp;gt;&lt;br /&gt;
  &amp;lt;uploadedFileContents&amp;gt;HYC116_BH3_FREQ.LOG&amp;lt;/uploadedFileContents&amp;gt;&lt;br /&gt;
&amp;lt;/jmolApplet&amp;gt;&amp;lt;/jmol&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
===Vibrational spectrum===&lt;br /&gt;
&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot;&lt;br /&gt;
!wavenumber (cm&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;)&lt;br /&gt;
!Intensity (arbitrary units)&lt;br /&gt;
!symmetry&lt;br /&gt;
!IR active?&lt;br /&gt;
!type&lt;br /&gt;
|-&lt;br /&gt;
|1163&lt;br /&gt;
|93&lt;br /&gt;
|A&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;&#039; &#039;&lt;br /&gt;
|Yes&lt;br /&gt;
|Out of plane bend&lt;br /&gt;
|-&lt;br /&gt;
|1213&lt;br /&gt;
|14&lt;br /&gt;
|E&#039;&lt;br /&gt;
|Very slight&lt;br /&gt;
|Bend&lt;br /&gt;
|-&lt;br /&gt;
|1213&lt;br /&gt;
|14&lt;br /&gt;
|E&#039;&lt;br /&gt;
|Very slight&lt;br /&gt;
|Bend&lt;br /&gt;
|-&lt;br /&gt;
|2582&lt;br /&gt;
|0&lt;br /&gt;
|A&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;&#039;&lt;br /&gt;
|No&lt;br /&gt;
|Symmetric stretch&lt;br /&gt;
|-&lt;br /&gt;
|2716&lt;br /&gt;
|126&lt;br /&gt;
|E&#039;&lt;br /&gt;
|Yes&lt;br /&gt;
|Asymmetric stretch&lt;br /&gt;
|-&lt;br /&gt;
|2716&lt;br /&gt;
|126&lt;br /&gt;
|E&#039;&lt;br /&gt;
|Yes&lt;br /&gt;
|Asymmetric stretch&lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;IR spectrum&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
[[file:Hyc116_ir_bh3.png|400*600]]&lt;br /&gt;
&lt;br /&gt;
There are only three peaks on the IR spectrum of BH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;, despite that there are 6 vibrational modes for the molecule. As shown in the table above, the symmetric stretching mode with A1 symmetry at 2582 cm&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt; is not IR active; naturally, that vibrational mode doesn’t give a peak on the IR spectrum. As shown from the table, two pairs of vibrational modes, the bond angle deformation/bend at 1213 cm&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt; and the asymmetric bond stretch at 2716 cm&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;, are degenerate with the symmetry label E. This means that they have the same energy, and hence give the same wavenumber on the IR spectrum. Each pair of degenerate vibrational modes give rise to one peak. This leaves three peaks, as confirmed by the IR spectrum above.&lt;br /&gt;
&lt;br /&gt;
===Molecular orbitals of BH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;===&lt;br /&gt;
&lt;br /&gt;
[[file:hyc116_bh3_MO_diagram.png]]&lt;br /&gt;
&lt;br /&gt;
The above molecular orbital diagram was taken from Dr Patricia Hunt&#039;s &amp;lt;i&amp;gt;Lecture 4 Tutorial Problem Model Answers&amp;lt;/i&amp;gt;. &amp;lt;ref&amp;gt;P. Hunt, &amp;quot;Lecture 4 Tutorial Problem Model Answers&amp;quot;, 2 (2018)&amp;lt;/ref&amp;gt;. Diagrams of the &amp;quot;real&amp;quot; MOs were obtained from Gaussian.&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
There is no significant difference between the LCAO MOs and the real ones. Features such as orbital phases are shown clearly on both the LCAO MOs and the real MOs, illustrating the bonding/anti-bonding characters of the molecular orbitals. This suggests that the the qualitative MO theory is highly accurate and useful when studying the molecular orbitals of molecules.&lt;br /&gt;
&lt;br /&gt;
==Associated energies: ammonium borane==&lt;br /&gt;
&lt;br /&gt;
===NH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;===&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;Calculation type&amp;lt;/b&amp;gt;: Optimisation&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;Calculation Method&amp;lt;/b&amp;gt;: B3LYP&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;Basis set&amp;lt;/b&amp;gt;: 6-31G(d,p) &lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Summary table&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
[[file:Hyc116_nh3_631g_summarytable.png]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Items table&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;pre&amp;gt;&lt;br /&gt;
Item               Value     Threshold  Converged?&lt;br /&gt;
 Maximum Force            0.000006     0.000450     YES&lt;br /&gt;
 RMS     Force            0.000004     0.000300     YES&lt;br /&gt;
 Maximum Displacement     0.000012     0.001800     YES&lt;br /&gt;
 RMS     Displacement     0.000008     0.001200     YES&lt;br /&gt;
&amp;lt;/pre&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Frequency log file&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
[[Media:HYC116_NH3_FREQ.LOG]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Frequencies&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;pre&amp;gt;&lt;br /&gt;
Low frequencies ---   -8.5646   -8.5588   -0.0047    0.0454    0.1784   26.4183&lt;br /&gt;
Low frequencies --- 1089.7603 1694.1865 1694.1865&lt;br /&gt;
&amp;lt;/pre&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;jmol of NH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;&#039;&#039;&#039;&lt;br /&gt;
&amp;lt;jmol&amp;gt;&amp;lt;jmolApplet&amp;gt;&lt;br /&gt;
  &amp;lt;title&amp;gt;optimised NH3&amp;lt;/title&amp;gt;&lt;br /&gt;
  &amp;lt;color&amp;gt;black&amp;lt;/color&amp;gt;&lt;br /&gt;
  &amp;lt;size&amp;gt;200&amp;lt;/size&amp;gt;&lt;br /&gt;
  &amp;lt;uploadedFileContents&amp;gt;HYC116_NH3_FREQ.LOG&amp;lt;/uploadedFileContents&amp;gt;&lt;br /&gt;
&amp;lt;/jmolApplet&amp;gt;&amp;lt;/jmol&amp;gt;&lt;br /&gt;
&lt;br /&gt;
===NH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;BH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;===&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;Calculation type&amp;lt;/b&amp;gt;: Optimisation&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;Calculation Method&amp;lt;/b&amp;gt;: B3LYP&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;Basis set&amp;lt;/b&amp;gt;: 6-31G(d,p) &lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Summary table&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
[[file:Hyc116_nh3bh3_631g_summarytable.png]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Items table&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;pre&amp;gt;&lt;br /&gt;
Item               Value     Threshold  Converged?&lt;br /&gt;
 Maximum Force            0.000123     0.000450     YES&lt;br /&gt;
 RMS     Force            0.000058     0.000300     YES&lt;br /&gt;
 Maximum Displacement     0.000515     0.001800     YES&lt;br /&gt;
 RMS     Displacement     0.000296     0.001200     YES&lt;br /&gt;
&amp;lt;/pre&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Frequency log file&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
[[Media:HYC116_NH3BH3_FREQ.LOG]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Frequencies&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;pre&amp;gt;&lt;br /&gt;
Low frequencies ---   -0.0014   -0.0011   -0.0006    6.9624   20.4518   43.5542&lt;br /&gt;
Low frequencies ---  266.4530  632.2458  639.0504&lt;br /&gt;
&amp;lt;/pre&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;jmol of NH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;BH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;&#039;&#039;&#039;&lt;br /&gt;
&amp;lt;jmol&amp;gt;&amp;lt;jmolApplet&amp;gt;&lt;br /&gt;
  &amp;lt;title&amp;gt;optimised NH3BH3&amp;lt;/title&amp;gt;&lt;br /&gt;
  &amp;lt;color&amp;gt;black&amp;lt;/color&amp;gt;&lt;br /&gt;
  &amp;lt;size&amp;gt;200&amp;lt;/size&amp;gt;&lt;br /&gt;
  &amp;lt;uploadedFileContents&amp;gt;HYC116_NH3BH3_FREQ.LOG&amp;lt;/uploadedFileContents&amp;gt;&lt;br /&gt;
&amp;lt;/jmolApplet&amp;gt;&amp;lt;/jmol&amp;gt;&lt;br /&gt;
&lt;br /&gt;
===Association energy===&lt;br /&gt;
&lt;br /&gt;
E(BH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;) (using the optimisation with the correct symmetry) = -26.61532363 a.u. = &amp;lt;b&amp;gt;-26.61532 a.u. (5 d.p.)&amp;lt;/b&amp;gt;&lt;br /&gt;
&lt;br /&gt;
E(NH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;) = -56.55776873 a.u. = &amp;lt;b&amp;gt;-56.55777 a.u. (5 d.p.)&amp;lt;/b&amp;gt;&lt;br /&gt;
&lt;br /&gt;
E(NH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;BH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;) = -83.22468893 a.u. = &amp;lt;b&amp;gt;-83.22469 a.u. (5 d.p.)&amp;lt;/b&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
Carrying out calculations using numbers which has already been rounded up can possibly result in errors in the last digit. Hence, here the calculations were carried out using the numbers provided from the optimisations (i.e. with more decimal places than necessary); the answer was then rounded up to the desired accuracy. &lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
ΔE = E(NH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;BH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;)-[E(NH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;)+E(BH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;)]&lt;br /&gt;
&lt;br /&gt;
ΔE = -83.22468893 - (-56.55776873 + -26.61532363) = -0.05159657 a.u. &lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;ΔE = -0.05160 a.u. (5 d.p.)&amp;lt;/b&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Converting energy from a.u. to kJ/mol&#039;&#039;&#039;&lt;br /&gt;
An atomic unit for energy is Hartree, which is equal to 2625.5 kJ/mol. &amp;lt;ref&amp;gt;https://cccbdb.nist.gov/hartree.asp (Accessed: 22.05.2018)&amp;lt;/ref&amp;gt;&lt;br /&gt;
&lt;br /&gt;
So ΔE in kJ/mol = -0.05159657 * 2625.5 = -135.466794535 kJ/mol&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;ΔE = -135 kJ/mol (nearest integer)&amp;lt;/b&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
The energy difference calculated above comes from the formation of the B-N dative bond. It is a relatively weak bond. According to a bond energy data sheet provided by the University of California, &amp;lt;ref&amp;gt;https://labs.chem.ucsb.edu/zakarian/armen/11---bonddissociationenergy.pdf (Accessed on 24.05.2018)&amp;lt;/ref&amp;gt; the bond energy of the C-C bond of an ethane molecule is 368 kJ/mol. This is a fair comparison to the NH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;BH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt; molecule as the two molecules have the same structure, only with the carbon atoms on ethane swapped for Boron and Nitrogen in NH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;BH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;&lt;br /&gt;
&lt;br /&gt;
==Using a mixture of basis-sets and pseudo-potentials==&lt;br /&gt;
&lt;br /&gt;
===BBr&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;===&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;Calculation type&amp;lt;/b&amp;gt;: Optimisation&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;Calculation Method&amp;lt;/b&amp;gt;: B3LYP&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;Basis set&amp;lt;/b&amp;gt;: Boron: 6-31G(d,p) ; Br: LANL2DZ&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
Larger calculations are often sent to a web-server to run on a high-performance computer instead of a desktop. In order to experience and learn to use a web-server, the optimisation and the frequency analysis for BBr&amp;lt;sub&amp;gt;3&amp;lt;/sub were both sent and done on a server instead of the desktop. The calculation results were downloaded from the web-server once they were finished.   &lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Summary table&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
[[file:Hyc116_bbr3_opt_summarytable.png]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Items table&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;pre&amp;gt;&lt;br /&gt;
Item               Value     Threshold  Converged?&lt;br /&gt;
 Maximum Force            0.000008     0.000450     YES&lt;br /&gt;
 RMS     Force            0.000005     0.000300     YES&lt;br /&gt;
 Maximum Displacement     0.000036     0.001800     YES&lt;br /&gt;
 RMS     Displacement     0.000023     0.001200     YES&lt;br /&gt;
&amp;lt;/pre&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Frequency log file&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
[[Media:Hyc116_bbr3_freq.log]]&lt;br /&gt;
&lt;br /&gt;
Attached above is the frequency file saved onto the computer from the SCAN server portal. The frequency file was also published on the chemistry database DSpace. {{DOI|10042/202442}}&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Frequencies&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;pre&amp;gt;&lt;br /&gt;
Low frequencies ---   -0.0137   -0.0064   -0.0046    2.4315    2.4315    4.8421&lt;br /&gt;
Low frequencies ---  155.9631  155.9651  267.7052&lt;br /&gt;
&amp;lt;/pre&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;jmol of BBr&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;&#039;&#039;&#039;&lt;br /&gt;
&amp;lt;jmol&amp;gt;&amp;lt;jmolApplet&amp;gt;&lt;br /&gt;
  &amp;lt;title&amp;gt;optimised BBr3&amp;lt;/title&amp;gt;&lt;br /&gt;
  &amp;lt;color&amp;gt;black&amp;lt;/color&amp;gt;&lt;br /&gt;
  &amp;lt;size&amp;gt;200&amp;lt;/size&amp;gt;&lt;br /&gt;
  &amp;lt;uploadedFileContents&amp;gt;Hyc116_bbr3_freq.log&amp;lt;/uploadedFileContents&amp;gt;&lt;br /&gt;
&amp;lt;/jmolApplet&amp;gt;&amp;lt;/jmol&amp;gt;&lt;br /&gt;
&lt;br /&gt;
==Aromaticity==&lt;br /&gt;
&lt;br /&gt;
===Benzene===&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;Calculation type&amp;lt;/b&amp;gt;: Optimisation&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;Calculation Method&amp;lt;/b&amp;gt;: B3LYP&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;Basis set&amp;lt;/b&amp;gt;: 6-31G(d,p) &lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Summary table&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
[[file:Hyc116_c6h6_summarytable.png]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Items table&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;pre&amp;gt;&lt;br /&gt;
Item               Value     Threshold  Converged?&lt;br /&gt;
 Maximum Force            0.000193     0.000450     YES&lt;br /&gt;
 RMS     Force            0.000079     0.000300     YES&lt;br /&gt;
 Maximum Displacement     0.000830     0.001800     YES&lt;br /&gt;
 RMS     Displacement     0.000294     0.001200     YES&lt;br /&gt;
&amp;lt;/pre&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Frequency log file&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
[[Media:HYC116_C6H6_FREQ.LOG]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Frequencies&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;pre&amp;gt;&lt;br /&gt;
Low frequencies ---   -3.5606   -3.5606   -0.0089   -0.0043   -0.0043   10.0905&lt;br /&gt;
Low frequencies ---  413.9582  413.9582  621.1416&lt;br /&gt;
&amp;lt;/pre&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;jmol of C&amp;lt;sub&amp;gt;6&amp;lt;/sub&amp;gt;H&amp;lt;sub&amp;gt;6&amp;lt;/sub&amp;gt;&#039;&#039;&#039;&lt;br /&gt;
&amp;lt;jmol&amp;gt;&amp;lt;jmolApplet&amp;gt;&lt;br /&gt;
  &amp;lt;title&amp;gt;optimised Benzene&amp;lt;/title&amp;gt;&lt;br /&gt;
  &amp;lt;color&amp;gt;black&amp;lt;/color&amp;gt;&lt;br /&gt;
  &amp;lt;size&amp;gt;200&amp;lt;/size&amp;gt;&lt;br /&gt;
  &amp;lt;uploadedFileContents&amp;gt;HYC116_C6H6_FREQ.LOG&amp;lt;/uploadedFileContents&amp;gt;&lt;br /&gt;
&amp;lt;/jmolApplet&amp;gt;&amp;lt;/jmol&amp;gt;&lt;br /&gt;
&lt;br /&gt;
===Borazine===&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;Calculation type&amp;lt;/b&amp;gt;: Optimisation&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;Calculation Method&amp;lt;/b&amp;gt;: B3LYP&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;Basis set&amp;lt;/b&amp;gt;: 6-31G(d,p) &lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Summary table&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
[[file:Hyc116_borazine_summarytable.png]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Items table&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;pre&amp;gt;&lt;br /&gt;
Item               Value     Threshold  Converged?&lt;br /&gt;
 Maximum Force            0.000085     0.000450     YES&lt;br /&gt;
 RMS     Force            0.000033     0.000300     YES&lt;br /&gt;
 Maximum Displacement     0.000250     0.001800     YES&lt;br /&gt;
 RMS     Displacement     0.000074     0.001200     YES&lt;br /&gt;
&amp;lt;/pre&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Frequency log file&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
[[Media:HYC116_BORAZINE_FREQ.LOG]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Frequencies&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;pre&amp;gt;&lt;br /&gt;
Low frequencies ---  -12.6626  -12.6626   -8.9272   -0.0211   -0.0104   -0.0104&lt;br /&gt;
Low frequencies ---  289.1112  289.1112  403.8613&lt;br /&gt;
&amp;lt;/pre&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;jmol of Borazine&#039;&#039;&#039;&lt;br /&gt;
&amp;lt;jmol&amp;gt;&amp;lt;jmolApplet&amp;gt;&lt;br /&gt;
  &amp;lt;title&amp;gt;optimised Borazine&amp;lt;/title&amp;gt;&lt;br /&gt;
  &amp;lt;color&amp;gt;black&amp;lt;/color&amp;gt;&lt;br /&gt;
  &amp;lt;size&amp;gt;200&amp;lt;/size&amp;gt;&lt;br /&gt;
  &amp;lt;uploadedFileContents&amp;gt;HYC116_BORAZINE_FREQ.LOG&amp;lt;/uploadedFileContents&amp;gt;&lt;br /&gt;
&amp;lt;/jmolApplet&amp;gt;&amp;lt;/jmol&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
===Charge distribution===&lt;br /&gt;
&lt;br /&gt;
An NBO charge analysis was carried out on both the optimised benzene and borazine. Visualisations of the charge distribution are shown in the table below, with the colour range going from -1.102 to 1.102 for both molecule. This large scale was chosen as it allows direct comparison of the charge on any atoms in these two molecules and shows the relative magnitude of charges on all these atoms. Negative charges are shown in red, and positive charges are shown in green. A neutral charge is displayed in black, so the smaller a charge is (positive or negative), the darker its colour representation is. Larger charges are shown in brighter colours. The charges are also displayed on the atoms as numbers with a neutral charge being zero. Negative charges are shown as negative number and positive charges are shown as positive numbers. &lt;br /&gt;
&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot;&lt;br /&gt;
!&lt;br /&gt;
!Benzene&lt;br /&gt;
!Borazine&lt;br /&gt;
|-&lt;br /&gt;
!Visualisation of charge distribution&lt;br /&gt;
|[[File:Hyc116_benzene_charge_distribution1.png|500x500px|thumb|centre|Charge distribution of Benzene visualisation]]&lt;br /&gt;
|[[File:Hyc116_borazine_charge_distribution1.png|500x500px|thumb|centre|Charge distribution of Borazine visualisation]]&lt;br /&gt;
|-&lt;br /&gt;
!Charge &lt;br /&gt;
|Carbon: -0.239&lt;br /&gt;
&lt;br /&gt;
Hydrogen: 0.239&lt;br /&gt;
|Nitrogen: -1.102 &lt;br /&gt;
&lt;br /&gt;
Boron: 0.747&lt;br /&gt;
&lt;br /&gt;
Hydrogen (bonded to N): 0.432&lt;br /&gt;
&lt;br /&gt;
Hydrogen (bonded to B): -0.077&lt;br /&gt;
|-&lt;br /&gt;
!Discussion&lt;br /&gt;
|From the visualisation, it is shown that there is a slightly negative charge on the carbon atoms, and a positive charge of the same magnitude on the hydrogen atoms. All the carbon atoms have the same charge as they are in identical environments. The same applies to all the hydrogen atoms. This is due to the highly symmetrical structure of benzene. Since the same colour scale was used for both benzene and borazine, and the charges are much smaller in magnitude on atoms in benzene than atoms on borazine, the colours on the charge distribution visualisation is much darker. &lt;br /&gt;
|From the colours displayed on the charge distribution visualisation as well as the charge values, it is shown that nitrogen has a relatively large negative charge, while boron has a positive charge. This is due to the difference in electrogenativity between these atoms: nitrogen atoms are more electronegative than boron and tends to attract electrons towards themselves. It is worth noting that the hydrogen atoms do not all have the same charge. The hydrogen atoms bonded to boron have a slightly negative charge, and the ones bonded to nitrogen have a small positive charge. &lt;br /&gt;
&lt;br /&gt;
The fact that the same colour scale was used for both molecules comes in helpful here. It allows the charges on atoms to be compared directly. For example, just from looking at the colours, one can tell that or example, even though both carbon and nitrogen are electronegative, nitrogen is much more electronegative, which is quantitatively shown by Pauling&#039;s electronegativity scale.&amp;lt;ref&amp;gt;http://www.tutor-homework.com/Chemistry_Help/electronegativity_table/electronegativity.html (Date accessed: 24.0502018&amp;lt;/ref&amp;gt;&lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
===Comparative MOs of Benzene and Borazine===&lt;br /&gt;
&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot;&lt;br /&gt;
!&lt;br /&gt;
!Benzene&lt;br /&gt;
!Borazine&lt;br /&gt;
!Comparison and Discussion&lt;br /&gt;
|-&lt;br /&gt;
!1st comparative pair&lt;br /&gt;
|[[File:Hyc116_benzene_1st_MO_pair_7.png|200x200px|centre]]&lt;br /&gt;
|[[File:Hyc116_borazine_1st_MO_pair_level9.png|200x200px|centre]]&lt;br /&gt;
|MO 9 of both benzene and borazine are comparable. They both show delocalised molecular orbital with an overall bonding character. There is a nodal plane across the molecular orbitals for both benzene and borazine. For benzene, there is contribution from all the carbon and hydrogen s orbitals. Moreover, the molecular orbitals are symmetric to their counterpart of opposite phase. That is not the case for borazine; they are less symmetric in borazine. Nitrogen atoms are more electronegative than boron atoms and pull electron density towards themselves, resulting in a larger MO. There is contribution from all the boron and nitrogen s orbitals, and three of the hydrogen s orbitals, though not all of them. &lt;br /&gt;
|-&lt;br /&gt;
!2nd comparative pair&lt;br /&gt;
|[[File:Hyc116_benzene_2nd_MO_pair_10.png|200x200px|centre]]&lt;br /&gt;
|[[File:Hyc116_borazine_2nd_MO_pair_level11.png|200x200px|centre]]&lt;br /&gt;
|&lt;br /&gt;
|-&lt;br /&gt;
!3rd comparative pair&lt;br /&gt;
|[[File:Hyc116_benzene_3rd_MO_pair_21.png|200x200px|centre]]&lt;br /&gt;
|[[File:Hyc116_borazine_3rd_MO_pair_level21.png|200x200px|centre]]&lt;br /&gt;
|&lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
===Aromaticity: some theories===&lt;br /&gt;
&lt;br /&gt;
===References===&lt;/div&gt;</summary>
		<author><name>Hyc116</name></author>
	</entry>
	<entry>
		<id>https://chemwiki.ch.ic.ac.uk/index.php?title=MO_hyc116&amp;diff=730152</id>
		<title>MO hyc116</title>
		<link rel="alternate" type="text/html" href="https://chemwiki.ch.ic.ac.uk/index.php?title=MO_hyc116&amp;diff=730152"/>
		<updated>2018-05-24T17:30:42Z</updated>

		<summary type="html">&lt;p&gt;Hyc116: &lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;==BH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;==&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;Calculation type&amp;lt;/b&amp;gt;: Optimisation&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;Calculation Method&amp;lt;/b&amp;gt;: B3LYP&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;Basis set&amp;lt;/b&amp;gt;: 6-31G(d,p) &lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Summary table&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
[[file:Hyc116_bh3_631g_opt_summarytable.png]]&lt;br /&gt;
&lt;br /&gt;
The above summary table was obtained after the 2nd optimisation of BH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt; (after the initial optimisation using the 3-21G basis set). Notice how the symmetry is incorrect and shown as Cs. This is because the symmetry was manually broken at the beginning by changing the bond length of B-H bonds. The point group was manually adjusted and the molecule was optimised again before the frequency analysis and the new summary table is attached below.&lt;br /&gt;
&lt;br /&gt;
[[file:Hyc116_bh3_correctsummarytable.png]]&lt;br /&gt;
&lt;br /&gt;
The above summary table was obtained from the optimisation after adjusting the symmetry. The point shown in this summary table is D&amp;lt;sub&amp;gt;3h&amp;lt;/sub&amp;gt;, which is the correct for BH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;. &lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Items table&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
Below is the items table taken from the optimisation with the correct point group.&lt;br /&gt;
&lt;br /&gt;
&amp;lt;pre&amp;gt;&lt;br /&gt;
Item               Value     Threshold  Converged?&lt;br /&gt;
 Maximum Force            0.000015     0.000450     YES&lt;br /&gt;
 RMS     Force            0.000010     0.000300     YES&lt;br /&gt;
 Maximum Displacement     0.000058     0.001800     YES&lt;br /&gt;
 RMS     Displacement     0.000038     0.001200     YES&lt;br /&gt;
&amp;lt;/pre&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Frequency log file&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
[[Media:HYC116 BH3 FREQ.LOG]] &lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Frequencies&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;pre&amp;gt;&lt;br /&gt;
Low frequencies ---  -10.3498   -3.4492   -1.2454   -0.0055    0.4779    3.2165&lt;br /&gt;
Low frequencies --- 1162.9519 1213.1527 1213.1554&lt;br /&gt;
&amp;lt;/pre&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;jmol of BH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;&#039;&#039;&#039;&lt;br /&gt;
&amp;lt;jmol&amp;gt;&amp;lt;jmolApplet&amp;gt;&lt;br /&gt;
  &amp;lt;title&amp;gt;optimised BH3&amp;lt;/title&amp;gt;&lt;br /&gt;
  &amp;lt;color&amp;gt;black&amp;lt;/color&amp;gt;&lt;br /&gt;
  &amp;lt;size&amp;gt;200&amp;lt;/size&amp;gt;&lt;br /&gt;
  &amp;lt;uploadedFileContents&amp;gt;HYC116_BH3_FREQ.LOG&amp;lt;/uploadedFileContents&amp;gt;&lt;br /&gt;
&amp;lt;/jmolApplet&amp;gt;&amp;lt;/jmol&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
===Vibrational spectrum===&lt;br /&gt;
&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot;&lt;br /&gt;
!wavenumber (cm&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;)&lt;br /&gt;
!Intensity (arbitrary units)&lt;br /&gt;
!symmetry&lt;br /&gt;
!IR active?&lt;br /&gt;
!type&lt;br /&gt;
|-&lt;br /&gt;
|1163&lt;br /&gt;
|93&lt;br /&gt;
|A&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;&#039; &#039;&lt;br /&gt;
|Yes&lt;br /&gt;
|Out of plane bend&lt;br /&gt;
|-&lt;br /&gt;
|1213&lt;br /&gt;
|14&lt;br /&gt;
|E&#039;&lt;br /&gt;
|Very slight&lt;br /&gt;
|Bend&lt;br /&gt;
|-&lt;br /&gt;
|1213&lt;br /&gt;
|14&lt;br /&gt;
|E&#039;&lt;br /&gt;
|Very slight&lt;br /&gt;
|Bend&lt;br /&gt;
|-&lt;br /&gt;
|2582&lt;br /&gt;
|0&lt;br /&gt;
|A&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;&#039;&lt;br /&gt;
|No&lt;br /&gt;
|Symmetric stretch&lt;br /&gt;
|-&lt;br /&gt;
|2716&lt;br /&gt;
|126&lt;br /&gt;
|E&#039;&lt;br /&gt;
|Yes&lt;br /&gt;
|Asymmetric stretch&lt;br /&gt;
|-&lt;br /&gt;
|2716&lt;br /&gt;
|126&lt;br /&gt;
|E&#039;&lt;br /&gt;
|Yes&lt;br /&gt;
|Asymmetric stretch&lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;IR spectrum&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
[[file:Hyc116_ir_bh3.png|400*600]]&lt;br /&gt;
&lt;br /&gt;
There are only three peaks on the IR spectrum of BH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;, despite that there are 6 vibrational modes for the molecule. As shown in the table above, the symmetric stretching mode with A1 symmetry at 2582 cm&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt; is not IR active; naturally, that vibrational mode doesn’t give a peak on the IR spectrum. As shown from the table, two pairs of vibrational modes, the bond angle deformation/bend at 1213 cm&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt; and the asymmetric bond stretch at 2716 cm&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;, are degenerate with the symmetry label E. This means that they have the same energy, and hence give the same wavenumber on the IR spectrum. Each pair of degenerate vibrational modes give rise to one peak. This leaves three peaks, as confirmed by the IR spectrum above.&lt;br /&gt;
&lt;br /&gt;
===Molecular orbitals of BH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;===&lt;br /&gt;
&lt;br /&gt;
[[file:hyc116_bh3_MO_diagram.png]]&lt;br /&gt;
&lt;br /&gt;
The above molecular orbital diagram was taken from Dr Patricia Hunt&#039;s &amp;lt;i&amp;gt;Lecture 4 Tutorial Problem Model Answers&amp;lt;/i&amp;gt;. &amp;lt;ref&amp;gt;P. Hunt, &amp;quot;Lecture 4 Tutorial Problem Model Answers&amp;quot;, 2 (2018)&amp;lt;/ref&amp;gt;. Diagrams of the &amp;quot;real&amp;quot; MOs were obtained from Gaussian.&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
There is no significant difference between the LCAO MOs and the real ones. Features such as orbital phases are shown clearly on both the LCAO MOs and the real MOs, illustrating the bonding/anti-bonding characters of the molecular orbitals. This suggests that the the qualitative MO theory is highly accurate and useful when studying the molecular orbitals of molecules.&lt;br /&gt;
&lt;br /&gt;
==Associated energies: ammonium borane==&lt;br /&gt;
&lt;br /&gt;
===NH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;===&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;Calculation type&amp;lt;/b&amp;gt;: Optimisation&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;Calculation Method&amp;lt;/b&amp;gt;: B3LYP&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;Basis set&amp;lt;/b&amp;gt;: 6-31G(d,p) &lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Summary table&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
[[file:Hyc116_nh3_631g_summarytable.png]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Items table&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;pre&amp;gt;&lt;br /&gt;
Item               Value     Threshold  Converged?&lt;br /&gt;
 Maximum Force            0.000006     0.000450     YES&lt;br /&gt;
 RMS     Force            0.000004     0.000300     YES&lt;br /&gt;
 Maximum Displacement     0.000012     0.001800     YES&lt;br /&gt;
 RMS     Displacement     0.000008     0.001200     YES&lt;br /&gt;
&amp;lt;/pre&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Frequency log file&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
[[Media:HYC116_NH3_FREQ.LOG]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Frequencies&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;pre&amp;gt;&lt;br /&gt;
Low frequencies ---   -8.5646   -8.5588   -0.0047    0.0454    0.1784   26.4183&lt;br /&gt;
Low frequencies --- 1089.7603 1694.1865 1694.1865&lt;br /&gt;
&amp;lt;/pre&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;jmol of NH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;&#039;&#039;&#039;&lt;br /&gt;
&amp;lt;jmol&amp;gt;&amp;lt;jmolApplet&amp;gt;&lt;br /&gt;
  &amp;lt;title&amp;gt;optimised NH3&amp;lt;/title&amp;gt;&lt;br /&gt;
  &amp;lt;color&amp;gt;black&amp;lt;/color&amp;gt;&lt;br /&gt;
  &amp;lt;size&amp;gt;200&amp;lt;/size&amp;gt;&lt;br /&gt;
  &amp;lt;uploadedFileContents&amp;gt;HYC116_NH3_FREQ.LOG&amp;lt;/uploadedFileContents&amp;gt;&lt;br /&gt;
&amp;lt;/jmolApplet&amp;gt;&amp;lt;/jmol&amp;gt;&lt;br /&gt;
&lt;br /&gt;
===NH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;BH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;===&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;Calculation type&amp;lt;/b&amp;gt;: Optimisation&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;Calculation Method&amp;lt;/b&amp;gt;: B3LYP&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;Basis set&amp;lt;/b&amp;gt;: 6-31G(d,p) &lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Summary table&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
[[file:Hyc116_nh3bh3_631g_summarytable.png]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Items table&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;pre&amp;gt;&lt;br /&gt;
Item               Value     Threshold  Converged?&lt;br /&gt;
 Maximum Force            0.000123     0.000450     YES&lt;br /&gt;
 RMS     Force            0.000058     0.000300     YES&lt;br /&gt;
 Maximum Displacement     0.000515     0.001800     YES&lt;br /&gt;
 RMS     Displacement     0.000296     0.001200     YES&lt;br /&gt;
&amp;lt;/pre&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Frequency log file&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
[[Media:HYC116_NH3BH3_FREQ.LOG]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Frequencies&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;pre&amp;gt;&lt;br /&gt;
Low frequencies ---   -0.0014   -0.0011   -0.0006    6.9624   20.4518   43.5542&lt;br /&gt;
Low frequencies ---  266.4530  632.2458  639.0504&lt;br /&gt;
&amp;lt;/pre&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;jmol of NH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;BH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;&#039;&#039;&#039;&lt;br /&gt;
&amp;lt;jmol&amp;gt;&amp;lt;jmolApplet&amp;gt;&lt;br /&gt;
  &amp;lt;title&amp;gt;optimised NH3BH3&amp;lt;/title&amp;gt;&lt;br /&gt;
  &amp;lt;color&amp;gt;black&amp;lt;/color&amp;gt;&lt;br /&gt;
  &amp;lt;size&amp;gt;200&amp;lt;/size&amp;gt;&lt;br /&gt;
  &amp;lt;uploadedFileContents&amp;gt;HYC116_NH3BH3_FREQ.LOG&amp;lt;/uploadedFileContents&amp;gt;&lt;br /&gt;
&amp;lt;/jmolApplet&amp;gt;&amp;lt;/jmol&amp;gt;&lt;br /&gt;
&lt;br /&gt;
===Association energy===&lt;br /&gt;
&lt;br /&gt;
E(BH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;) (using the optimisation with the correct symmetry) = -26.61532363 a.u. = &amp;lt;b&amp;gt;-26.61532 a.u. (5 d.p.)&amp;lt;/b&amp;gt;&lt;br /&gt;
&lt;br /&gt;
E(NH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;) = -56.55776873 a.u. = &amp;lt;b&amp;gt;-56.55777 a.u. (5 d.p.)&amp;lt;/b&amp;gt;&lt;br /&gt;
&lt;br /&gt;
E(NH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;BH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;) = -83.22468893 a.u. = &amp;lt;b&amp;gt;-83.22469 a.u. (5 d.p.)&amp;lt;/b&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
Carrying out calculations using numbers which has already been rounded up can possibly result in errors in the last digit. Hence, here the calculations were carried out using the numbers provided from the optimisations (i.e. with more decimal places than necessary); the answer was then rounded up to the desired accuracy. &lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
ΔE = E(NH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;BH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;)-[E(NH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;)+E(BH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;)]&lt;br /&gt;
&lt;br /&gt;
ΔE = -83.22468893 - (-56.55776873 + -26.61532363) = -0.05159657 a.u. &lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;ΔE = -0.05160 a.u. (5 d.p.)&amp;lt;/b&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Converting energy from a.u. to kJ/mol&#039;&#039;&#039;&lt;br /&gt;
An atomic unit for energy is Hartree, which is equal to 2625.5 kJ/mol. &amp;lt;ref&amp;gt;https://cccbdb.nist.gov/hartree.asp (Accessed: 22.05.2018)&amp;lt;/ref&amp;gt;&lt;br /&gt;
&lt;br /&gt;
So ΔE in kJ/mol = -0.05159657 * 2625.5 = -135.466794535 kJ/mol&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;ΔE = -135 kJ/mol (nearest integer)&amp;lt;/b&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
The energy difference calculated above comes from the formation of the B-N dative bond. It is a relatively weak bond. According to a bond energy data sheet provided by the University of California, &amp;lt;ref&amp;gt;https://labs.chem.ucsb.edu/zakarian/armen/11---bonddissociationenergy.pdf (Accessed on 24.05.2018)&amp;lt;/ref&amp;gt; the bond energy of the C-C bond of an ethane molecule is 368 kJ/mol. This is a fair comparison to the NH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;BH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt; molecule as the two molecules have the same structure, only with the carbon atoms on ethane swapped for Boron and Nitrogen in NH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;BH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;&lt;br /&gt;
&lt;br /&gt;
==Using a mixture of basis-sets and pseudo-potentials==&lt;br /&gt;
&lt;br /&gt;
===BBr&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;===&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;Calculation type&amp;lt;/b&amp;gt;: Optimisation&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;Calculation Method&amp;lt;/b&amp;gt;: B3LYP&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;Basis set&amp;lt;/b&amp;gt;: Boron: 6-31G(d,p) ; Br: LANL2DZ&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
Larger calculations are often sent to a web-server to run on a high-performance computer instead of a desktop. In order to experience and learn to use a web-server, the optimisation and the frequency analysis for BBr&amp;lt;sub&amp;gt;3&amp;lt;/sub were both sent and done on a server instead of the desktop. The calculation results were downloaded from the web-server once they were finished.   &lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Summary table&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
[[file:Hyc116_bbr3_opt_summarytable.png]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Items table&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;pre&amp;gt;&lt;br /&gt;
Item               Value     Threshold  Converged?&lt;br /&gt;
 Maximum Force            0.000008     0.000450     YES&lt;br /&gt;
 RMS     Force            0.000005     0.000300     YES&lt;br /&gt;
 Maximum Displacement     0.000036     0.001800     YES&lt;br /&gt;
 RMS     Displacement     0.000023     0.001200     YES&lt;br /&gt;
&amp;lt;/pre&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Frequency log file&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
[[Media:Hyc116_bbr3_freq.log]]&lt;br /&gt;
&lt;br /&gt;
Attached above is the frequency file saved onto the computer from the SCAN server portal. The frequency file was also published on the chemistry database DSpace. {{DOI|10042/202442}}&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Frequencies&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;pre&amp;gt;&lt;br /&gt;
Low frequencies ---   -0.0137   -0.0064   -0.0046    2.4315    2.4315    4.8421&lt;br /&gt;
Low frequencies ---  155.9631  155.9651  267.7052&lt;br /&gt;
&amp;lt;/pre&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;jmol of BBr&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;&#039;&#039;&#039;&lt;br /&gt;
&amp;lt;jmol&amp;gt;&amp;lt;jmolApplet&amp;gt;&lt;br /&gt;
  &amp;lt;title&amp;gt;optimised BBr3&amp;lt;/title&amp;gt;&lt;br /&gt;
  &amp;lt;color&amp;gt;black&amp;lt;/color&amp;gt;&lt;br /&gt;
  &amp;lt;size&amp;gt;200&amp;lt;/size&amp;gt;&lt;br /&gt;
  &amp;lt;uploadedFileContents&amp;gt;Hyc116_bbr3_freq.log&amp;lt;/uploadedFileContents&amp;gt;&lt;br /&gt;
&amp;lt;/jmolApplet&amp;gt;&amp;lt;/jmol&amp;gt;&lt;br /&gt;
&lt;br /&gt;
==Aromaticity==&lt;br /&gt;
&lt;br /&gt;
===Benzene===&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;Calculation type&amp;lt;/b&amp;gt;: Optimisation&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;Calculation Method&amp;lt;/b&amp;gt;: B3LYP&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;Basis set&amp;lt;/b&amp;gt;: 6-31G(d,p) &lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Summary table&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
[[file:Hyc116_c6h6_summarytable.png]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Items table&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;pre&amp;gt;&lt;br /&gt;
Item               Value     Threshold  Converged?&lt;br /&gt;
 Maximum Force            0.000193     0.000450     YES&lt;br /&gt;
 RMS     Force            0.000079     0.000300     YES&lt;br /&gt;
 Maximum Displacement     0.000830     0.001800     YES&lt;br /&gt;
 RMS     Displacement     0.000294     0.001200     YES&lt;br /&gt;
&amp;lt;/pre&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Frequency log file&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
[[Media:HYC116_C6H6_FREQ.LOG]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Frequencies&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;pre&amp;gt;&lt;br /&gt;
Low frequencies ---   -3.5606   -3.5606   -0.0089   -0.0043   -0.0043   10.0905&lt;br /&gt;
Low frequencies ---  413.9582  413.9582  621.1416&lt;br /&gt;
&amp;lt;/pre&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;jmol of C&amp;lt;sub&amp;gt;6&amp;lt;/sub&amp;gt;H&amp;lt;sub&amp;gt;6&amp;lt;/sub&amp;gt;&#039;&#039;&#039;&lt;br /&gt;
&amp;lt;jmol&amp;gt;&amp;lt;jmolApplet&amp;gt;&lt;br /&gt;
  &amp;lt;title&amp;gt;optimised Benzene&amp;lt;/title&amp;gt;&lt;br /&gt;
  &amp;lt;color&amp;gt;black&amp;lt;/color&amp;gt;&lt;br /&gt;
  &amp;lt;size&amp;gt;200&amp;lt;/size&amp;gt;&lt;br /&gt;
  &amp;lt;uploadedFileContents&amp;gt;HYC116_C6H6_FREQ.LOG&amp;lt;/uploadedFileContents&amp;gt;&lt;br /&gt;
&amp;lt;/jmolApplet&amp;gt;&amp;lt;/jmol&amp;gt;&lt;br /&gt;
&lt;br /&gt;
===Borazine===&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;Calculation type&amp;lt;/b&amp;gt;: Optimisation&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;Calculation Method&amp;lt;/b&amp;gt;: B3LYP&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;Basis set&amp;lt;/b&amp;gt;: 6-31G(d,p) &lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Summary table&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
[[file:Hyc116_borazine_summarytable.png]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Items table&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;pre&amp;gt;&lt;br /&gt;
Item               Value     Threshold  Converged?&lt;br /&gt;
 Maximum Force            0.000085     0.000450     YES&lt;br /&gt;
 RMS     Force            0.000033     0.000300     YES&lt;br /&gt;
 Maximum Displacement     0.000250     0.001800     YES&lt;br /&gt;
 RMS     Displacement     0.000074     0.001200     YES&lt;br /&gt;
&amp;lt;/pre&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Frequency log file&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
[[Media:HYC116_BORAZINE_FREQ.LOG]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Frequencies&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;pre&amp;gt;&lt;br /&gt;
Low frequencies ---  -12.6626  -12.6626   -8.9272   -0.0211   -0.0104   -0.0104&lt;br /&gt;
Low frequencies ---  289.1112  289.1112  403.8613&lt;br /&gt;
&amp;lt;/pre&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;jmol of Borazine&#039;&#039;&#039;&lt;br /&gt;
&amp;lt;jmol&amp;gt;&amp;lt;jmolApplet&amp;gt;&lt;br /&gt;
  &amp;lt;title&amp;gt;optimised Borazine&amp;lt;/title&amp;gt;&lt;br /&gt;
  &amp;lt;color&amp;gt;black&amp;lt;/color&amp;gt;&lt;br /&gt;
  &amp;lt;size&amp;gt;200&amp;lt;/size&amp;gt;&lt;br /&gt;
  &amp;lt;uploadedFileContents&amp;gt;HYC116_BORAZINE_FREQ.LOG&amp;lt;/uploadedFileContents&amp;gt;&lt;br /&gt;
&amp;lt;/jmolApplet&amp;gt;&amp;lt;/jmol&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
===Charge distribution===&lt;br /&gt;
&lt;br /&gt;
An NBO charge analysis was carried out on both the optimised benzene and borazine. Visualisations of the charge distribution are shown in the table below, with the colour range going from -1.102 to 1.102 for both molecule. This large scale was chosen as it allows direct comparison of the charge on any atoms in these two molecules and shows the relative magnitude of charges on all these atoms. Negative charges are shown in red, and positive charges are shown in green. A neutral charge is displayed in black, so the smaller a charge is (positive or negative), the darker its colour representation is. Larger charges are shown in brighter colours. The charges are also displayed on the atoms as numbers with a neutral charge being zero. Negative charges are shown as negative number and positive charges are shown as positive numbers. &lt;br /&gt;
&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot;&lt;br /&gt;
!&lt;br /&gt;
!Benzene&lt;br /&gt;
!Borazine&lt;br /&gt;
|-&lt;br /&gt;
!Visualisation of charge distribution&lt;br /&gt;
|[[File:Hyc116_benzene_charge_distribution1.png|500x500px|thumb|centre|Charge distribution of Benzene visualisation]]&lt;br /&gt;
|[[File:Hyc116_borazine_charge_distribution1.png|500x500px|thumb|centre|Charge distribution of Borazine visualisation]]&lt;br /&gt;
|-&lt;br /&gt;
!Charge &lt;br /&gt;
|Carbon: -0.239&lt;br /&gt;
&lt;br /&gt;
Hydrogen: 0.239&lt;br /&gt;
|Nitrogen: -1.102 &lt;br /&gt;
&lt;br /&gt;
Boron: 0.747&lt;br /&gt;
&lt;br /&gt;
Hydrogen (bonded to N): 0.432&lt;br /&gt;
&lt;br /&gt;
Hydrogen (bonded to B): -0.077&lt;br /&gt;
|-&lt;br /&gt;
!Discussion&lt;br /&gt;
|From the visualisation, it is shown that there is a slightly negative charge on the carbon atoms, and a positive charge of the same magnitude on the hydrogen atoms. All the carbon atoms have the same charge as they are in identical environments. The same applies to all the hydrogen atoms. This is due to the highly symmetrical structure of benzene. Since the same colour scale was used for both benzene and borazine, and the charges are much smaller in magnitude on atoms in benzene than atoms on borazine, the colours on the charge distribution visualisation is much darker. &lt;br /&gt;
|From the colours displayed on the charge distribution visualisation as well as the charge values, it is shown that nitrogen has a relatively large negative charge, while boron has a positive charge. This is due to the difference in electrogenativity between these atoms: nitrogen atoms are more electronegative than boron and tends to attract electrons towards themselves. It is worth noting that the hydrogen atoms do not all have the same charge. The hydrogen atoms bonded to boron have a slightly negative charge, and the ones bonded to nitrogen have a small positive charge. &lt;br /&gt;
&lt;br /&gt;
The fact that the same colour scale was used for both molecules comes in helpful here. It allows the charges on atoms to be compared directly. For example, just from looking at the colours, one can tell that or example, even though both carbon and nitrogen are electronegative, nitrogen is much more electronegative, which is quantitatively shown by Pauling&#039;s electronegativity scale.&amp;lt;ref&amp;gt;http://www.tutor-homework.com/Chemistry_Help/electronegativity_table/electronegativity.html (Date accessed: 24.0502018&amp;lt;/ref&amp;gt;&lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
===Comparative MOs of Benzene and Borazine===&lt;br /&gt;
&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot;&lt;br /&gt;
!&lt;br /&gt;
!Benzene&lt;br /&gt;
!Borazine&lt;br /&gt;
!Comparison and Discussion&lt;br /&gt;
|-&lt;br /&gt;
!1st comparative pair&lt;br /&gt;
|[[File:Hyc116_benzene_1st_MO_pair_7.png|200x200px|centre]]&lt;br /&gt;
|[[File:Hyc116_borazine_1st_MO_pair_level9.png|200x200px|centre]]&lt;br /&gt;
|MO 9 of both benzene and borazine are comparable. They both show delocalised molecular orbital with an overall bonding character. There is a nodal plane across the molecular orbitals for both benzene and borazine. For benzene, there is contribution from all the carbon and hydrogen s orbitals. Moreover, the molecular orbitals are symmetric to their counterpart of opposite phase. That is not the case for borazine; they are less symmetric in borazine. Nitrogen atoms are more electronegative than boron atoms and pull electron density towards themselves, resulting in a larger MO. There is contribution from all the boron and nitrogen s orbitals, and three of the hydrogen s orbitals, though not all of them. &lt;br /&gt;
|-&lt;br /&gt;
!2nd comparative pair&lt;br /&gt;
|[[File:Hyc116_benzene_2nd_MO_pair_10.png|200x200px|centre]]&lt;br /&gt;
|[[File:Hyc116_borazine_2nd_MO_pair_level11.png|200x200px|centre]]&lt;br /&gt;
|&lt;br /&gt;
|-&lt;br /&gt;
!3rd comparative pair&lt;br /&gt;
|[[File:Hyc116_benzene_3rd_MO_pair_21.png|200x200px|centre]]&lt;br /&gt;
|[[File:Hyc116_borazine_3rd_MO_pair_level21.png|200x200px|centre]]&lt;br /&gt;
|&lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
===Aromaticity: some theories===&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
==Reference==&lt;/div&gt;</summary>
		<author><name>Hyc116</name></author>
	</entry>
	<entry>
		<id>https://chemwiki.ch.ic.ac.uk/index.php?title=MO_hyc116&amp;diff=730151</id>
		<title>MO hyc116</title>
		<link rel="alternate" type="text/html" href="https://chemwiki.ch.ic.ac.uk/index.php?title=MO_hyc116&amp;diff=730151"/>
		<updated>2018-05-24T17:30:26Z</updated>

		<summary type="html">&lt;p&gt;Hyc116: &lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;==BH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;==&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;Calculation type&amp;lt;/b&amp;gt;: Optimisation&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;Calculation Method&amp;lt;/b&amp;gt;: B3LYP&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;Basis set&amp;lt;/b&amp;gt;: 6-31G(d,p) &lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Summary table&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
[[file:Hyc116_bh3_631g_opt_summarytable.png]]&lt;br /&gt;
&lt;br /&gt;
The above summary table was obtained after the 2nd optimisation of BH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt; (after the initial optimisation using the 3-21G basis set). Notice how the symmetry is incorrect and shown as Cs. This is because the symmetry was manually broken at the beginning by changing the bond length of B-H bonds. The point group was manually adjusted and the molecule was optimised again before the frequency analysis and the new summary table is attached below.&lt;br /&gt;
&lt;br /&gt;
[[file:Hyc116_bh3_correctsummarytable.png]]&lt;br /&gt;
&lt;br /&gt;
The above summary table was obtained from the optimisation after adjusting the symmetry. The point shown in this summary table is D&amp;lt;sub&amp;gt;3h&amp;lt;/sub&amp;gt;, which is the correct for BH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;. &lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Items table&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
Below is the items table taken from the optimisation with the correct point group.&lt;br /&gt;
&lt;br /&gt;
&amp;lt;pre&amp;gt;&lt;br /&gt;
Item               Value     Threshold  Converged?&lt;br /&gt;
 Maximum Force            0.000015     0.000450     YES&lt;br /&gt;
 RMS     Force            0.000010     0.000300     YES&lt;br /&gt;
 Maximum Displacement     0.000058     0.001800     YES&lt;br /&gt;
 RMS     Displacement     0.000038     0.001200     YES&lt;br /&gt;
&amp;lt;/pre&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Frequency log file&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
[[Media:HYC116 BH3 FREQ.LOG]] &lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Frequencies&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;pre&amp;gt;&lt;br /&gt;
Low frequencies ---  -10.3498   -3.4492   -1.2454   -0.0055    0.4779    3.2165&lt;br /&gt;
Low frequencies --- 1162.9519 1213.1527 1213.1554&lt;br /&gt;
&amp;lt;/pre&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;jmol of BH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;&#039;&#039;&#039;&lt;br /&gt;
&amp;lt;jmol&amp;gt;&amp;lt;jmolApplet&amp;gt;&lt;br /&gt;
  &amp;lt;title&amp;gt;optimised BH3&amp;lt;/title&amp;gt;&lt;br /&gt;
  &amp;lt;color&amp;gt;black&amp;lt;/color&amp;gt;&lt;br /&gt;
  &amp;lt;size&amp;gt;200&amp;lt;/size&amp;gt;&lt;br /&gt;
  &amp;lt;uploadedFileContents&amp;gt;HYC116_BH3_FREQ.LOG&amp;lt;/uploadedFileContents&amp;gt;&lt;br /&gt;
&amp;lt;/jmolApplet&amp;gt;&amp;lt;/jmol&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
===Vibrational spectrum===&lt;br /&gt;
&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot;&lt;br /&gt;
!wavenumber (cm&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;)&lt;br /&gt;
!Intensity (arbitrary units)&lt;br /&gt;
!symmetry&lt;br /&gt;
!IR active?&lt;br /&gt;
!type&lt;br /&gt;
|-&lt;br /&gt;
|1163&lt;br /&gt;
|93&lt;br /&gt;
|A&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;&#039; &#039;&lt;br /&gt;
|Yes&lt;br /&gt;
|Out of plane bend&lt;br /&gt;
|-&lt;br /&gt;
|1213&lt;br /&gt;
|14&lt;br /&gt;
|E&#039;&lt;br /&gt;
|Very slight&lt;br /&gt;
|Bend&lt;br /&gt;
|-&lt;br /&gt;
|1213&lt;br /&gt;
|14&lt;br /&gt;
|E&#039;&lt;br /&gt;
|Very slight&lt;br /&gt;
|Bend&lt;br /&gt;
|-&lt;br /&gt;
|2582&lt;br /&gt;
|0&lt;br /&gt;
|A&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;&#039;&lt;br /&gt;
|No&lt;br /&gt;
|Symmetric stretch&lt;br /&gt;
|-&lt;br /&gt;
|2716&lt;br /&gt;
|126&lt;br /&gt;
|E&#039;&lt;br /&gt;
|Yes&lt;br /&gt;
|Asymmetric stretch&lt;br /&gt;
|-&lt;br /&gt;
|2716&lt;br /&gt;
|126&lt;br /&gt;
|E&#039;&lt;br /&gt;
|Yes&lt;br /&gt;
|Asymmetric stretch&lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;IR spectrum&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
[[file:Hyc116_ir_bh3.png|400*600]]&lt;br /&gt;
&lt;br /&gt;
There are only three peaks on the IR spectrum of BH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;, despite that there are 6 vibrational modes for the molecule. As shown in the table above, the symmetric stretching mode with A1 symmetry at 2582 cm&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt; is not IR active; naturally, that vibrational mode doesn’t give a peak on the IR spectrum. As shown from the table, two pairs of vibrational modes, the bond angle deformation/bend at 1213 cm&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt; and the asymmetric bond stretch at 2716 cm&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;, are degenerate with the symmetry label E. This means that they have the same energy, and hence give the same wavenumber on the IR spectrum. Each pair of degenerate vibrational modes give rise to one peak. This leaves three peaks, as confirmed by the IR spectrum above.&lt;br /&gt;
&lt;br /&gt;
===Molecular orbitals of BH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;===&lt;br /&gt;
&lt;br /&gt;
[[file:hyc116_bh3_MO_diagram.png]]&lt;br /&gt;
&lt;br /&gt;
The above molecular orbital diagram was taken from Dr Patricia Hunt&#039;s &amp;lt;i&amp;gt;Lecture 4 Tutorial Problem Model Answers&amp;lt;/i&amp;gt;. &amp;lt;ref&amp;gt;P. Hunt, &amp;quot;Lecture 4 Tutorial Problem Model Answers&amp;quot;, 2 (2018)&amp;lt;/ref&amp;gt;. Diagrams of the &amp;quot;real&amp;quot; MOs were obtained from Gaussian.&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
There is no significant difference between the LCAO MOs and the real ones. Features such as orbital phases are shown clearly on both the LCAO MOs and the real MOs, illustrating the bonding/anti-bonding characters of the molecular orbitals. This suggests that the the qualitative MO theory is highly accurate and useful when studying the molecular orbitals of molecules.&lt;br /&gt;
&lt;br /&gt;
==Associated energies: ammonium borane==&lt;br /&gt;
&lt;br /&gt;
===NH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;===&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;Calculation type&amp;lt;/b&amp;gt;: Optimisation&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;Calculation Method&amp;lt;/b&amp;gt;: B3LYP&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;Basis set&amp;lt;/b&amp;gt;: 6-31G(d,p) &lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Summary table&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
[[file:Hyc116_nh3_631g_summarytable.png]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Items table&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;pre&amp;gt;&lt;br /&gt;
Item               Value     Threshold  Converged?&lt;br /&gt;
 Maximum Force            0.000006     0.000450     YES&lt;br /&gt;
 RMS     Force            0.000004     0.000300     YES&lt;br /&gt;
 Maximum Displacement     0.000012     0.001800     YES&lt;br /&gt;
 RMS     Displacement     0.000008     0.001200     YES&lt;br /&gt;
&amp;lt;/pre&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Frequency log file&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
[[Media:HYC116_NH3_FREQ.LOG]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Frequencies&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;pre&amp;gt;&lt;br /&gt;
Low frequencies ---   -8.5646   -8.5588   -0.0047    0.0454    0.1784   26.4183&lt;br /&gt;
Low frequencies --- 1089.7603 1694.1865 1694.1865&lt;br /&gt;
&amp;lt;/pre&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;jmol of NH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;&#039;&#039;&#039;&lt;br /&gt;
&amp;lt;jmol&amp;gt;&amp;lt;jmolApplet&amp;gt;&lt;br /&gt;
  &amp;lt;title&amp;gt;optimised NH3&amp;lt;/title&amp;gt;&lt;br /&gt;
  &amp;lt;color&amp;gt;black&amp;lt;/color&amp;gt;&lt;br /&gt;
  &amp;lt;size&amp;gt;200&amp;lt;/size&amp;gt;&lt;br /&gt;
  &amp;lt;uploadedFileContents&amp;gt;HYC116_NH3_FREQ.LOG&amp;lt;/uploadedFileContents&amp;gt;&lt;br /&gt;
&amp;lt;/jmolApplet&amp;gt;&amp;lt;/jmol&amp;gt;&lt;br /&gt;
&lt;br /&gt;
===NH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;BH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;===&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;Calculation type&amp;lt;/b&amp;gt;: Optimisation&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;Calculation Method&amp;lt;/b&amp;gt;: B3LYP&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;Basis set&amp;lt;/b&amp;gt;: 6-31G(d,p) &lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Summary table&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
[[file:Hyc116_nh3bh3_631g_summarytable.png]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Items table&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;pre&amp;gt;&lt;br /&gt;
Item               Value     Threshold  Converged?&lt;br /&gt;
 Maximum Force            0.000123     0.000450     YES&lt;br /&gt;
 RMS     Force            0.000058     0.000300     YES&lt;br /&gt;
 Maximum Displacement     0.000515     0.001800     YES&lt;br /&gt;
 RMS     Displacement     0.000296     0.001200     YES&lt;br /&gt;
&amp;lt;/pre&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Frequency log file&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
[[Media:HYC116_NH3BH3_FREQ.LOG]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Frequencies&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;pre&amp;gt;&lt;br /&gt;
Low frequencies ---   -0.0014   -0.0011   -0.0006    6.9624   20.4518   43.5542&lt;br /&gt;
Low frequencies ---  266.4530  632.2458  639.0504&lt;br /&gt;
&amp;lt;/pre&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;jmol of NH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;BH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;&#039;&#039;&#039;&lt;br /&gt;
&amp;lt;jmol&amp;gt;&amp;lt;jmolApplet&amp;gt;&lt;br /&gt;
  &amp;lt;title&amp;gt;optimised NH3BH3&amp;lt;/title&amp;gt;&lt;br /&gt;
  &amp;lt;color&amp;gt;black&amp;lt;/color&amp;gt;&lt;br /&gt;
  &amp;lt;size&amp;gt;200&amp;lt;/size&amp;gt;&lt;br /&gt;
  &amp;lt;uploadedFileContents&amp;gt;HYC116_NH3BH3_FREQ.LOG&amp;lt;/uploadedFileContents&amp;gt;&lt;br /&gt;
&amp;lt;/jmolApplet&amp;gt;&amp;lt;/jmol&amp;gt;&lt;br /&gt;
&lt;br /&gt;
===Association energy===&lt;br /&gt;
&lt;br /&gt;
E(BH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;) (using the optimisation with the correct symmetry) = -26.61532363 a.u. = &amp;lt;b&amp;gt;-26.61532 a.u. (5 d.p.)&amp;lt;/b&amp;gt;&lt;br /&gt;
&lt;br /&gt;
E(NH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;) = -56.55776873 a.u. = &amp;lt;b&amp;gt;-56.55777 a.u. (5 d.p.)&amp;lt;/b&amp;gt;&lt;br /&gt;
&lt;br /&gt;
E(NH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;BH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;) = -83.22468893 a.u. = &amp;lt;b&amp;gt;-83.22469 a.u. (5 d.p.)&amp;lt;/b&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
Carrying out calculations using numbers which has already been rounded up can possibly result in errors in the last digit. Hence, here the calculations were carried out using the numbers provided from the optimisations (i.e. with more decimal places than necessary); the answer was then rounded up to the desired accuracy. &lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
ΔE = E(NH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;BH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;)-[E(NH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;)+E(BH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;)]&lt;br /&gt;
&lt;br /&gt;
ΔE = -83.22468893 - (-56.55776873 + -26.61532363) = -0.05159657 a.u. &lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;ΔE = -0.05160 a.u. (5 d.p.)&amp;lt;/b&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Converting energy from a.u. to kJ/mol&#039;&#039;&#039;&lt;br /&gt;
An atomic unit for energy is Hartree, which is equal to 2625.5 kJ/mol. &amp;lt;ref&amp;gt;https://cccbdb.nist.gov/hartree.asp (Accessed: 22.05.2018)&amp;lt;/ref&amp;gt;&lt;br /&gt;
&lt;br /&gt;
So ΔE in kJ/mol = -0.05159657 * 2625.5 = -135.466794535 kJ/mol&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;ΔE = -135 kJ/mol (nearest integer)&amp;lt;/b&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
The energy difference calculated above comes from the formation of the B-N dative bond. It is a relatively weak bond. According to a bond energy data sheet provided by the University of California, &amp;lt;ref&amp;gt;https://labs.chem.ucsb.edu/zakarian/armen/11---bonddissociationenergy.pdf (Accessed on 24.05.2018)&amp;lt;/ref&amp;gt; the bond energy of the C-C bond of an ethane molecule is 368 kJ/mol. This is a fair comparison to the NH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;BH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt; molecule as the two molecules have the same structure, only with the carbon atoms on ethane swapped for Boron and Nitrogen in NH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;BH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;&lt;br /&gt;
&lt;br /&gt;
==Using a mixture of basis-sets and pseudo-potentials==&lt;br /&gt;
&lt;br /&gt;
===BBr&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;===&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;Calculation type&amp;lt;/b&amp;gt;: Optimisation&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;Calculation Method&amp;lt;/b&amp;gt;: B3LYP&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;Basis set&amp;lt;/b&amp;gt;: Boron: 6-31G(d,p) ; Br: LANL2DZ&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
Larger calculations are often sent to a web-server to run on a high-performance computer instead of a desktop. In order to experience and learn to use a web-server, the optimisation and the frequency analysis for BBr&amp;lt;sub&amp;gt;3&amp;lt;/sub were both sent and done on a server instead of the desktop. The calculation results were downloaded from the web-server once they were finished.   &lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Summary table&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
[[file:Hyc116_bbr3_opt_summarytable.png]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Items table&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;pre&amp;gt;&lt;br /&gt;
Item               Value     Threshold  Converged?&lt;br /&gt;
 Maximum Force            0.000008     0.000450     YES&lt;br /&gt;
 RMS     Force            0.000005     0.000300     YES&lt;br /&gt;
 Maximum Displacement     0.000036     0.001800     YES&lt;br /&gt;
 RMS     Displacement     0.000023     0.001200     YES&lt;br /&gt;
&amp;lt;/pre&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Frequency log file&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
[[Media:Hyc116_bbr3_freq.log]]&lt;br /&gt;
&lt;br /&gt;
Attached above is the frequency file saved onto the computer from the SCAN server portal. The frequency file was also published on the chemistry database DSpace. {{DOI|10042/202442}}&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Frequencies&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;pre&amp;gt;&lt;br /&gt;
Low frequencies ---   -0.0137   -0.0064   -0.0046    2.4315    2.4315    4.8421&lt;br /&gt;
Low frequencies ---  155.9631  155.9651  267.7052&lt;br /&gt;
&amp;lt;/pre&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;jmol of BBr&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;&#039;&#039;&#039;&lt;br /&gt;
&amp;lt;jmol&amp;gt;&amp;lt;jmolApplet&amp;gt;&lt;br /&gt;
  &amp;lt;title&amp;gt;optimised BBr3&amp;lt;/title&amp;gt;&lt;br /&gt;
  &amp;lt;color&amp;gt;black&amp;lt;/color&amp;gt;&lt;br /&gt;
  &amp;lt;size&amp;gt;200&amp;lt;/size&amp;gt;&lt;br /&gt;
  &amp;lt;uploadedFileContents&amp;gt;Hyc116_bbr3_freq.log&amp;lt;/uploadedFileContents&amp;gt;&lt;br /&gt;
&amp;lt;/jmolApplet&amp;gt;&amp;lt;/jmol&amp;gt;&lt;br /&gt;
&lt;br /&gt;
==Aromaticity==&lt;br /&gt;
&lt;br /&gt;
===Benzene===&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;Calculation type&amp;lt;/b&amp;gt;: Optimisation&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;Calculation Method&amp;lt;/b&amp;gt;: B3LYP&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;Basis set&amp;lt;/b&amp;gt;: 6-31G(d,p) &lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Summary table&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
[[file:Hyc116_c6h6_summarytable.png]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Items table&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;pre&amp;gt;&lt;br /&gt;
Item               Value     Threshold  Converged?&lt;br /&gt;
 Maximum Force            0.000193     0.000450     YES&lt;br /&gt;
 RMS     Force            0.000079     0.000300     YES&lt;br /&gt;
 Maximum Displacement     0.000830     0.001800     YES&lt;br /&gt;
 RMS     Displacement     0.000294     0.001200     YES&lt;br /&gt;
&amp;lt;/pre&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Frequency log file&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
[[Media:HYC116_C6H6_FREQ.LOG]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Frequencies&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;pre&amp;gt;&lt;br /&gt;
Low frequencies ---   -3.5606   -3.5606   -0.0089   -0.0043   -0.0043   10.0905&lt;br /&gt;
Low frequencies ---  413.9582  413.9582  621.1416&lt;br /&gt;
&amp;lt;/pre&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;jmol of C&amp;lt;sub&amp;gt;6&amp;lt;/sub&amp;gt;H&amp;lt;sub&amp;gt;6&amp;lt;/sub&amp;gt;&#039;&#039;&#039;&lt;br /&gt;
&amp;lt;jmol&amp;gt;&amp;lt;jmolApplet&amp;gt;&lt;br /&gt;
  &amp;lt;title&amp;gt;optimised Benzene&amp;lt;/title&amp;gt;&lt;br /&gt;
  &amp;lt;color&amp;gt;black&amp;lt;/color&amp;gt;&lt;br /&gt;
  &amp;lt;size&amp;gt;200&amp;lt;/size&amp;gt;&lt;br /&gt;
  &amp;lt;uploadedFileContents&amp;gt;HYC116_C6H6_FREQ.LOG&amp;lt;/uploadedFileContents&amp;gt;&lt;br /&gt;
&amp;lt;/jmolApplet&amp;gt;&amp;lt;/jmol&amp;gt;&lt;br /&gt;
&lt;br /&gt;
===Borazine===&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;Calculation type&amp;lt;/b&amp;gt;: Optimisation&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;Calculation Method&amp;lt;/b&amp;gt;: B3LYP&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;Basis set&amp;lt;/b&amp;gt;: 6-31G(d,p) &lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Summary table&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
[[file:Hyc116_borazine_summarytable.png]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Items table&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;pre&amp;gt;&lt;br /&gt;
Item               Value     Threshold  Converged?&lt;br /&gt;
 Maximum Force            0.000085     0.000450     YES&lt;br /&gt;
 RMS     Force            0.000033     0.000300     YES&lt;br /&gt;
 Maximum Displacement     0.000250     0.001800     YES&lt;br /&gt;
 RMS     Displacement     0.000074     0.001200     YES&lt;br /&gt;
&amp;lt;/pre&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Frequency log file&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
[[Media:HYC116_BORAZINE_FREQ.LOG]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Frequencies&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;pre&amp;gt;&lt;br /&gt;
Low frequencies ---  -12.6626  -12.6626   -8.9272   -0.0211   -0.0104   -0.0104&lt;br /&gt;
Low frequencies ---  289.1112  289.1112  403.8613&lt;br /&gt;
&amp;lt;/pre&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;jmol of Borazine&#039;&#039;&#039;&lt;br /&gt;
&amp;lt;jmol&amp;gt;&amp;lt;jmolApplet&amp;gt;&lt;br /&gt;
  &amp;lt;title&amp;gt;optimised Borazine&amp;lt;/title&amp;gt;&lt;br /&gt;
  &amp;lt;color&amp;gt;black&amp;lt;/color&amp;gt;&lt;br /&gt;
  &amp;lt;size&amp;gt;200&amp;lt;/size&amp;gt;&lt;br /&gt;
  &amp;lt;uploadedFileContents&amp;gt;HYC116_BORAZINE_FREQ.LOG&amp;lt;/uploadedFileContents&amp;gt;&lt;br /&gt;
&amp;lt;/jmolApplet&amp;gt;&amp;lt;/jmol&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
===Charge distribution===&lt;br /&gt;
&lt;br /&gt;
An NBO charge analysis was carried out on both the optimised benzene and borazine. Visualisations of the charge distribution are shown in the table below, with the colour range going from -1.102 to 1.102 for both molecule. This large scale was chosen as it allows direct comparison of the charge on any atoms in these two molecules and shows the relative magnitude of charges on all these atoms. Negative charges are shown in red, and positive charges are shown in green. A neutral charge is displayed in black, so the smaller a charge is (positive or negative), the darker its colour representation is. Larger charges are shown in brighter colours. The charges are also displayed on the atoms as numbers with a neutral charge being zero. Negative charges are shown as negative number and positive charges are shown as positive numbers. &lt;br /&gt;
&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot;&lt;br /&gt;
!&lt;br /&gt;
!Benzene&lt;br /&gt;
!Borazine&lt;br /&gt;
|-&lt;br /&gt;
!Visualisation of charge distribution&lt;br /&gt;
|[[File:Hyc116_benzene_charge_distribution1.png|500x500px|thumb|centre|Charge distribution of Benzene visualisation]]&lt;br /&gt;
|[[File:Hyc116_borazine_charge_distribution1.png|500x500px|thumb|centre|Charge distribution of Borazine visualisation]]&lt;br /&gt;
|-&lt;br /&gt;
!Charge &lt;br /&gt;
|Carbon: -0.239&lt;br /&gt;
&lt;br /&gt;
Hydrogen: 0.239&lt;br /&gt;
|Nitrogen: -1.102 &lt;br /&gt;
&lt;br /&gt;
Boron: 0.747&lt;br /&gt;
&lt;br /&gt;
Hydrogen (bonded to N): 0.432&lt;br /&gt;
&lt;br /&gt;
Hydrogen (bonded to B): -0.077&lt;br /&gt;
|-&lt;br /&gt;
!Discussion&lt;br /&gt;
|From the visualisation, it is shown that there is a slightly negative charge on the carbon atoms, and a positive charge of the same magnitude on the hydrogen atoms. All the carbon atoms have the same charge as they are in identical environments. The same applies to all the hydrogen atoms. This is due to the highly symmetrical structure of benzene. Since the same colour scale was used for both benzene and borazine, and the charges are much smaller in magnitude on atoms in benzene than atoms on borazine, the colours on the charge distribution visualisation is much darker. &lt;br /&gt;
|From the colours displayed on the charge distribution visualisation as well as the charge values, it is shown that nitrogen has a relatively large negative charge, while boron has a positive charge. This is due to the difference in electrogenativity between these atoms: nitrogen atoms are more electronegative than boron and tends to attract electrons towards themselves. It is worth noting that the hydrogen atoms do not all have the same charge. The hydrogen atoms bonded to boron have a slightly negative charge, and the ones bonded to nitrogen have a small positive charge. &lt;br /&gt;
&lt;br /&gt;
The fact that the same colour scale was used for both molecules comes in helpful here. It allows the charges on atoms to be compared directly. For example, just from looking at the colours, one can tell that or example, even though both carbon and nitrogen are electronegative, nitrogen is much more electronegative, which is quantitatively shown by Pauling&#039;s electronegativity scale.&amp;lt;ref&amp;gt;http://www.tutor-homework.com/Chemistry_Help/electronegativity_table/electronegativity.html (Date accessed: 24.0502018&amp;lt;/ref&amp;gt;&lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
===Comparative MOs of Benzene and Borazine===&lt;br /&gt;
&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot;&lt;br /&gt;
!&lt;br /&gt;
!Benzene&lt;br /&gt;
!Borazine&lt;br /&gt;
!Comparison and Discussion&lt;br /&gt;
|-&lt;br /&gt;
!1st comparative pair&lt;br /&gt;
|[[File:Hyc116_benzene_1st_MO_pair_7.png|200x200px|centre]]&lt;br /&gt;
|[[File:Hyc116_borazine_1st_MO_pair_level9.png|200x200px|centre]]&lt;br /&gt;
|MO 9 of both benzene and borazine are comparable. They both show delocalised molecular orbital with an overall bonding character. There is a nodal plane across the molecular orbitals for both benzene and borazine. For benzene, there is contribution from all the carbon and hydrogen s orbitals. Moreover, the molecular orbitals are symmetric to their counterpart of opposite phase. That is not the case for borazine; they are less symmetric in borazine. Nitrogen atoms are more electronegative than boron atoms and pull electron density towards themselves, resulting in a larger MO. There is contribution from all the boron and nitrogen s orbitals, and three of the hydrogen s orbitals, though not all of them. &lt;br /&gt;
|-&lt;br /&gt;
!2nd comparative pair&lt;br /&gt;
|[[File:Hyc116_benzene_2nd_MO_pair_10.png|200x200px|centre]]&lt;br /&gt;
|[[File:Hyc116_borazine_2nd_MO_pair_level11.png|200x200px|centre]]&lt;br /&gt;
|&lt;br /&gt;
|-&lt;br /&gt;
!3rd comparative pair&lt;br /&gt;
|[[File:Hyc116_benzene_3rd_MO_pair_21.png|200x200px|centre]]&lt;br /&gt;
|[[File:Hyc116_borazine_3rd_MO_pair_level21.png|200x200px|centre]]&lt;br /&gt;
|&lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
===Aromaticity: some theories===&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
=Reference=&lt;/div&gt;</summary>
		<author><name>Hyc116</name></author>
	</entry>
	<entry>
		<id>https://chemwiki.ch.ic.ac.uk/index.php?title=MO_hyc116&amp;diff=730150</id>
		<title>MO hyc116</title>
		<link rel="alternate" type="text/html" href="https://chemwiki.ch.ic.ac.uk/index.php?title=MO_hyc116&amp;diff=730150"/>
		<updated>2018-05-24T17:30:05Z</updated>

		<summary type="html">&lt;p&gt;Hyc116: &lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;==BH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;==&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;Calculation type&amp;lt;/b&amp;gt;: Optimisation&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;Calculation Method&amp;lt;/b&amp;gt;: B3LYP&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;Basis set&amp;lt;/b&amp;gt;: 6-31G(d,p) &lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Summary table&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
[[file:Hyc116_bh3_631g_opt_summarytable.png]]&lt;br /&gt;
&lt;br /&gt;
The above summary table was obtained after the 2nd optimisation of BH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt; (after the initial optimisation using the 3-21G basis set). Notice how the symmetry is incorrect and shown as Cs. This is because the symmetry was manually broken at the beginning by changing the bond length of B-H bonds. The point group was manually adjusted and the molecule was optimised again before the frequency analysis and the new summary table is attached below.&lt;br /&gt;
&lt;br /&gt;
[[file:Hyc116_bh3_correctsummarytable.png]]&lt;br /&gt;
&lt;br /&gt;
The above summary table was obtained from the optimisation after adjusting the symmetry. The point shown in this summary table is D&amp;lt;sub&amp;gt;3h&amp;lt;/sub&amp;gt;, which is the correct for BH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;. &lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Items table&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
Below is the items table taken from the optimisation with the correct point group.&lt;br /&gt;
&lt;br /&gt;
&amp;lt;pre&amp;gt;&lt;br /&gt;
Item               Value     Threshold  Converged?&lt;br /&gt;
 Maximum Force            0.000015     0.000450     YES&lt;br /&gt;
 RMS     Force            0.000010     0.000300     YES&lt;br /&gt;
 Maximum Displacement     0.000058     0.001800     YES&lt;br /&gt;
 RMS     Displacement     0.000038     0.001200     YES&lt;br /&gt;
&amp;lt;/pre&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Frequency log file&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
[[Media:HYC116 BH3 FREQ.LOG]] &lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Frequencies&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;pre&amp;gt;&lt;br /&gt;
Low frequencies ---  -10.3498   -3.4492   -1.2454   -0.0055    0.4779    3.2165&lt;br /&gt;
Low frequencies --- 1162.9519 1213.1527 1213.1554&lt;br /&gt;
&amp;lt;/pre&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;jmol of BH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;&#039;&#039;&#039;&lt;br /&gt;
&amp;lt;jmol&amp;gt;&amp;lt;jmolApplet&amp;gt;&lt;br /&gt;
  &amp;lt;title&amp;gt;optimised BH3&amp;lt;/title&amp;gt;&lt;br /&gt;
  &amp;lt;color&amp;gt;black&amp;lt;/color&amp;gt;&lt;br /&gt;
  &amp;lt;size&amp;gt;200&amp;lt;/size&amp;gt;&lt;br /&gt;
  &amp;lt;uploadedFileContents&amp;gt;HYC116_BH3_FREQ.LOG&amp;lt;/uploadedFileContents&amp;gt;&lt;br /&gt;
&amp;lt;/jmolApplet&amp;gt;&amp;lt;/jmol&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
===Vibrational spectrum===&lt;br /&gt;
&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot;&lt;br /&gt;
!wavenumber (cm&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;)&lt;br /&gt;
!Intensity (arbitrary units)&lt;br /&gt;
!symmetry&lt;br /&gt;
!IR active?&lt;br /&gt;
!type&lt;br /&gt;
|-&lt;br /&gt;
|1163&lt;br /&gt;
|93&lt;br /&gt;
|A&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;&#039; &#039;&lt;br /&gt;
|Yes&lt;br /&gt;
|Out of plane bend&lt;br /&gt;
|-&lt;br /&gt;
|1213&lt;br /&gt;
|14&lt;br /&gt;
|E&#039;&lt;br /&gt;
|Very slight&lt;br /&gt;
|Bend&lt;br /&gt;
|-&lt;br /&gt;
|1213&lt;br /&gt;
|14&lt;br /&gt;
|E&#039;&lt;br /&gt;
|Very slight&lt;br /&gt;
|Bend&lt;br /&gt;
|-&lt;br /&gt;
|2582&lt;br /&gt;
|0&lt;br /&gt;
|A&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;&#039;&lt;br /&gt;
|No&lt;br /&gt;
|Symmetric stretch&lt;br /&gt;
|-&lt;br /&gt;
|2716&lt;br /&gt;
|126&lt;br /&gt;
|E&#039;&lt;br /&gt;
|Yes&lt;br /&gt;
|Asymmetric stretch&lt;br /&gt;
|-&lt;br /&gt;
|2716&lt;br /&gt;
|126&lt;br /&gt;
|E&#039;&lt;br /&gt;
|Yes&lt;br /&gt;
|Asymmetric stretch&lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;IR spectrum&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
[[file:Hyc116_ir_bh3.png|400*600]]&lt;br /&gt;
&lt;br /&gt;
There are only three peaks on the IR spectrum of BH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;, despite that there are 6 vibrational modes for the molecule. As shown in the table above, the symmetric stretching mode with A1 symmetry at 2582 cm&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt; is not IR active; naturally, that vibrational mode doesn’t give a peak on the IR spectrum. As shown from the table, two pairs of vibrational modes, the bond angle deformation/bend at 1213 cm&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt; and the asymmetric bond stretch at 2716 cm&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;, are degenerate with the symmetry label E. This means that they have the same energy, and hence give the same wavenumber on the IR spectrum. Each pair of degenerate vibrational modes give rise to one peak. This leaves three peaks, as confirmed by the IR spectrum above.&lt;br /&gt;
&lt;br /&gt;
===Molecular orbitals of BH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;===&lt;br /&gt;
&lt;br /&gt;
[[file:hyc116_bh3_MO_diagram.png]]&lt;br /&gt;
&lt;br /&gt;
The above molecular orbital diagram was taken from Dr Patricia Hunt&#039;s &amp;lt;i&amp;gt;Lecture 4 Tutorial Problem Model Answers&amp;lt;/i&amp;gt;. &amp;lt;ref&amp;gt;P. Hunt, &amp;quot;Lecture 4 Tutorial Problem Model Answers&amp;quot;, 2 (2018)&amp;lt;/ref&amp;gt;. Diagrams of the &amp;quot;real&amp;quot; MOs were obtained from Gaussian.&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
There is no significant difference between the LCAO MOs and the real ones. Features such as orbital phases are shown clearly on both the LCAO MOs and the real MOs, illustrating the bonding/anti-bonding characters of the molecular orbitals. This suggests that the the qualitative MO theory is highly accurate and useful when studying the molecular orbitals of molecules.&lt;br /&gt;
&lt;br /&gt;
==Associated energies: ammonium borane==&lt;br /&gt;
&lt;br /&gt;
===NH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;===&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;Calculation type&amp;lt;/b&amp;gt;: Optimisation&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;Calculation Method&amp;lt;/b&amp;gt;: B3LYP&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;Basis set&amp;lt;/b&amp;gt;: 6-31G(d,p) &lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Summary table&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
[[file:Hyc116_nh3_631g_summarytable.png]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Items table&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;pre&amp;gt;&lt;br /&gt;
Item               Value     Threshold  Converged?&lt;br /&gt;
 Maximum Force            0.000006     0.000450     YES&lt;br /&gt;
 RMS     Force            0.000004     0.000300     YES&lt;br /&gt;
 Maximum Displacement     0.000012     0.001800     YES&lt;br /&gt;
 RMS     Displacement     0.000008     0.001200     YES&lt;br /&gt;
&amp;lt;/pre&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Frequency log file&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
[[Media:HYC116_NH3_FREQ.LOG]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Frequencies&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;pre&amp;gt;&lt;br /&gt;
Low frequencies ---   -8.5646   -8.5588   -0.0047    0.0454    0.1784   26.4183&lt;br /&gt;
Low frequencies --- 1089.7603 1694.1865 1694.1865&lt;br /&gt;
&amp;lt;/pre&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;jmol of NH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;&#039;&#039;&#039;&lt;br /&gt;
&amp;lt;jmol&amp;gt;&amp;lt;jmolApplet&amp;gt;&lt;br /&gt;
  &amp;lt;title&amp;gt;optimised NH3&amp;lt;/title&amp;gt;&lt;br /&gt;
  &amp;lt;color&amp;gt;black&amp;lt;/color&amp;gt;&lt;br /&gt;
  &amp;lt;size&amp;gt;200&amp;lt;/size&amp;gt;&lt;br /&gt;
  &amp;lt;uploadedFileContents&amp;gt;HYC116_NH3_FREQ.LOG&amp;lt;/uploadedFileContents&amp;gt;&lt;br /&gt;
&amp;lt;/jmolApplet&amp;gt;&amp;lt;/jmol&amp;gt;&lt;br /&gt;
&lt;br /&gt;
===NH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;BH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;===&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;Calculation type&amp;lt;/b&amp;gt;: Optimisation&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;Calculation Method&amp;lt;/b&amp;gt;: B3LYP&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;Basis set&amp;lt;/b&amp;gt;: 6-31G(d,p) &lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Summary table&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
[[file:Hyc116_nh3bh3_631g_summarytable.png]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Items table&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;pre&amp;gt;&lt;br /&gt;
Item               Value     Threshold  Converged?&lt;br /&gt;
 Maximum Force            0.000123     0.000450     YES&lt;br /&gt;
 RMS     Force            0.000058     0.000300     YES&lt;br /&gt;
 Maximum Displacement     0.000515     0.001800     YES&lt;br /&gt;
 RMS     Displacement     0.000296     0.001200     YES&lt;br /&gt;
&amp;lt;/pre&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Frequency log file&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
[[Media:HYC116_NH3BH3_FREQ.LOG]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Frequencies&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;pre&amp;gt;&lt;br /&gt;
Low frequencies ---   -0.0014   -0.0011   -0.0006    6.9624   20.4518   43.5542&lt;br /&gt;
Low frequencies ---  266.4530  632.2458  639.0504&lt;br /&gt;
&amp;lt;/pre&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;jmol of NH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;BH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;&#039;&#039;&#039;&lt;br /&gt;
&amp;lt;jmol&amp;gt;&amp;lt;jmolApplet&amp;gt;&lt;br /&gt;
  &amp;lt;title&amp;gt;optimised NH3BH3&amp;lt;/title&amp;gt;&lt;br /&gt;
  &amp;lt;color&amp;gt;black&amp;lt;/color&amp;gt;&lt;br /&gt;
  &amp;lt;size&amp;gt;200&amp;lt;/size&amp;gt;&lt;br /&gt;
  &amp;lt;uploadedFileContents&amp;gt;HYC116_NH3BH3_FREQ.LOG&amp;lt;/uploadedFileContents&amp;gt;&lt;br /&gt;
&amp;lt;/jmolApplet&amp;gt;&amp;lt;/jmol&amp;gt;&lt;br /&gt;
&lt;br /&gt;
===Association energy===&lt;br /&gt;
&lt;br /&gt;
E(BH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;) (using the optimisation with the correct symmetry) = -26.61532363 a.u. = &amp;lt;b&amp;gt;-26.61532 a.u. (5 d.p.)&amp;lt;/b&amp;gt;&lt;br /&gt;
&lt;br /&gt;
E(NH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;) = -56.55776873 a.u. = &amp;lt;b&amp;gt;-56.55777 a.u. (5 d.p.)&amp;lt;/b&amp;gt;&lt;br /&gt;
&lt;br /&gt;
E(NH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;BH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;) = -83.22468893 a.u. = &amp;lt;b&amp;gt;-83.22469 a.u. (5 d.p.)&amp;lt;/b&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
Carrying out calculations using numbers which has already been rounded up can possibly result in errors in the last digit. Hence, here the calculations were carried out using the numbers provided from the optimisations (i.e. with more decimal places than necessary); the answer was then rounded up to the desired accuracy. &lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
ΔE = E(NH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;BH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;)-[E(NH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;)+E(BH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;)]&lt;br /&gt;
&lt;br /&gt;
ΔE = -83.22468893 - (-56.55776873 + -26.61532363) = -0.05159657 a.u. &lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;ΔE = -0.05160 a.u. (5 d.p.)&amp;lt;/b&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Converting energy from a.u. to kJ/mol&#039;&#039;&#039;&lt;br /&gt;
An atomic unit for energy is Hartree, which is equal to 2625.5 kJ/mol. &amp;lt;ref&amp;gt;https://cccbdb.nist.gov/hartree.asp (Accessed: 22.05.2018)&amp;lt;/ref&amp;gt;&lt;br /&gt;
&lt;br /&gt;
So ΔE in kJ/mol = -0.05159657 * 2625.5 = -135.466794535 kJ/mol&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;ΔE = -135 kJ/mol (nearest integer)&amp;lt;/b&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
The energy difference calculated above comes from the formation of the B-N dative bond. It is a relatively weak bond. According to a bond energy data sheet provided by the University of California, &amp;lt;ref&amp;gt;https://labs.chem.ucsb.edu/zakarian/armen/11---bonddissociationenergy.pdf (Accessed on 24.05.2018)&amp;lt;/ref&amp;gt; the bond energy of the C-C bond of an ethane molecule is 368 kJ/mol. This is a fair comparison to the NH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;BH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt; molecule as the two molecules have the same structure, only with the carbon atoms on ethane swapped for Boron and Nitrogen in NH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;BH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;&lt;br /&gt;
&lt;br /&gt;
==Using a mixture of basis-sets and pseudo-potentials==&lt;br /&gt;
&lt;br /&gt;
===BBr&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;===&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;Calculation type&amp;lt;/b&amp;gt;: Optimisation&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;Calculation Method&amp;lt;/b&amp;gt;: B3LYP&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;Basis set&amp;lt;/b&amp;gt;: Boron: 6-31G(d,p) ; Br: LANL2DZ&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
Larger calculations are often sent to a web-server to run on a high-performance computer instead of a desktop. In order to experience and learn to use a web-server, the optimisation and the frequency analysis for BBr&amp;lt;sub&amp;gt;3&amp;lt;/sub were both sent and done on a server instead of the desktop. The calculation results were downloaded from the web-server once they were finished.   &lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Summary table&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
[[file:Hyc116_bbr3_opt_summarytable.png]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Items table&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;pre&amp;gt;&lt;br /&gt;
Item               Value     Threshold  Converged?&lt;br /&gt;
 Maximum Force            0.000008     0.000450     YES&lt;br /&gt;
 RMS     Force            0.000005     0.000300     YES&lt;br /&gt;
 Maximum Displacement     0.000036     0.001800     YES&lt;br /&gt;
 RMS     Displacement     0.000023     0.001200     YES&lt;br /&gt;
&amp;lt;/pre&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Frequency log file&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
[[Media:Hyc116_bbr3_freq.log]]&lt;br /&gt;
&lt;br /&gt;
Attached above is the frequency file saved onto the computer from the SCAN server portal. The frequency file was also published on the chemistry database DSpace. {{DOI|10042/202442}}&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Frequencies&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;pre&amp;gt;&lt;br /&gt;
Low frequencies ---   -0.0137   -0.0064   -0.0046    2.4315    2.4315    4.8421&lt;br /&gt;
Low frequencies ---  155.9631  155.9651  267.7052&lt;br /&gt;
&amp;lt;/pre&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;jmol of BBr&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;&#039;&#039;&#039;&lt;br /&gt;
&amp;lt;jmol&amp;gt;&amp;lt;jmolApplet&amp;gt;&lt;br /&gt;
  &amp;lt;title&amp;gt;optimised BBr3&amp;lt;/title&amp;gt;&lt;br /&gt;
  &amp;lt;color&amp;gt;black&amp;lt;/color&amp;gt;&lt;br /&gt;
  &amp;lt;size&amp;gt;200&amp;lt;/size&amp;gt;&lt;br /&gt;
  &amp;lt;uploadedFileContents&amp;gt;Hyc116_bbr3_freq.log&amp;lt;/uploadedFileContents&amp;gt;&lt;br /&gt;
&amp;lt;/jmolApplet&amp;gt;&amp;lt;/jmol&amp;gt;&lt;br /&gt;
&lt;br /&gt;
==Aromaticity==&lt;br /&gt;
&lt;br /&gt;
===Benzene===&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;Calculation type&amp;lt;/b&amp;gt;: Optimisation&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;Calculation Method&amp;lt;/b&amp;gt;: B3LYP&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;Basis set&amp;lt;/b&amp;gt;: 6-31G(d,p) &lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Summary table&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
[[file:Hyc116_c6h6_summarytable.png]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Items table&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;pre&amp;gt;&lt;br /&gt;
Item               Value     Threshold  Converged?&lt;br /&gt;
 Maximum Force            0.000193     0.000450     YES&lt;br /&gt;
 RMS     Force            0.000079     0.000300     YES&lt;br /&gt;
 Maximum Displacement     0.000830     0.001800     YES&lt;br /&gt;
 RMS     Displacement     0.000294     0.001200     YES&lt;br /&gt;
&amp;lt;/pre&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Frequency log file&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
[[Media:HYC116_C6H6_FREQ.LOG]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Frequencies&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;pre&amp;gt;&lt;br /&gt;
Low frequencies ---   -3.5606   -3.5606   -0.0089   -0.0043   -0.0043   10.0905&lt;br /&gt;
Low frequencies ---  413.9582  413.9582  621.1416&lt;br /&gt;
&amp;lt;/pre&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;jmol of C&amp;lt;sub&amp;gt;6&amp;lt;/sub&amp;gt;H&amp;lt;sub&amp;gt;6&amp;lt;/sub&amp;gt;&#039;&#039;&#039;&lt;br /&gt;
&amp;lt;jmol&amp;gt;&amp;lt;jmolApplet&amp;gt;&lt;br /&gt;
  &amp;lt;title&amp;gt;optimised Benzene&amp;lt;/title&amp;gt;&lt;br /&gt;
  &amp;lt;color&amp;gt;black&amp;lt;/color&amp;gt;&lt;br /&gt;
  &amp;lt;size&amp;gt;200&amp;lt;/size&amp;gt;&lt;br /&gt;
  &amp;lt;uploadedFileContents&amp;gt;HYC116_C6H6_FREQ.LOG&amp;lt;/uploadedFileContents&amp;gt;&lt;br /&gt;
&amp;lt;/jmolApplet&amp;gt;&amp;lt;/jmol&amp;gt;&lt;br /&gt;
&lt;br /&gt;
===Borazine===&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;Calculation type&amp;lt;/b&amp;gt;: Optimisation&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;Calculation Method&amp;lt;/b&amp;gt;: B3LYP&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;Basis set&amp;lt;/b&amp;gt;: 6-31G(d,p) &lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Summary table&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
[[file:Hyc116_borazine_summarytable.png]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Items table&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;pre&amp;gt;&lt;br /&gt;
Item               Value     Threshold  Converged?&lt;br /&gt;
 Maximum Force            0.000085     0.000450     YES&lt;br /&gt;
 RMS     Force            0.000033     0.000300     YES&lt;br /&gt;
 Maximum Displacement     0.000250     0.001800     YES&lt;br /&gt;
 RMS     Displacement     0.000074     0.001200     YES&lt;br /&gt;
&amp;lt;/pre&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Frequency log file&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
[[Media:HYC116_BORAZINE_FREQ.LOG]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Frequencies&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;pre&amp;gt;&lt;br /&gt;
Low frequencies ---  -12.6626  -12.6626   -8.9272   -0.0211   -0.0104   -0.0104&lt;br /&gt;
Low frequencies ---  289.1112  289.1112  403.8613&lt;br /&gt;
&amp;lt;/pre&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;jmol of Borazine&#039;&#039;&#039;&lt;br /&gt;
&amp;lt;jmol&amp;gt;&amp;lt;jmolApplet&amp;gt;&lt;br /&gt;
  &amp;lt;title&amp;gt;optimised Borazine&amp;lt;/title&amp;gt;&lt;br /&gt;
  &amp;lt;color&amp;gt;black&amp;lt;/color&amp;gt;&lt;br /&gt;
  &amp;lt;size&amp;gt;200&amp;lt;/size&amp;gt;&lt;br /&gt;
  &amp;lt;uploadedFileContents&amp;gt;HYC116_BORAZINE_FREQ.LOG&amp;lt;/uploadedFileContents&amp;gt;&lt;br /&gt;
&amp;lt;/jmolApplet&amp;gt;&amp;lt;/jmol&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
===Charge distribution===&lt;br /&gt;
&lt;br /&gt;
An NBO charge analysis was carried out on both the optimised benzene and borazine. Visualisations of the charge distribution are shown in the table below, with the colour range going from -1.102 to 1.102 for both molecule. This large scale was chosen as it allows direct comparison of the charge on any atoms in these two molecules and shows the relative magnitude of charges on all these atoms. Negative charges are shown in red, and positive charges are shown in green. A neutral charge is displayed in black, so the smaller a charge is (positive or negative), the darker its colour representation is. Larger charges are shown in brighter colours. The charges are also displayed on the atoms as numbers with a neutral charge being zero. Negative charges are shown as negative number and positive charges are shown as positive numbers. &lt;br /&gt;
&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot;&lt;br /&gt;
!&lt;br /&gt;
!Benzene&lt;br /&gt;
!Borazine&lt;br /&gt;
|-&lt;br /&gt;
!Visualisation of charge distribution&lt;br /&gt;
|[[File:Hyc116_benzene_charge_distribution1.png|500x500px|thumb|centre|Charge distribution of Benzene visualisation]]&lt;br /&gt;
|[[File:Hyc116_borazine_charge_distribution1.png|500x500px|thumb|centre|Charge distribution of Borazine visualisation]]&lt;br /&gt;
|-&lt;br /&gt;
!Charge &lt;br /&gt;
|Carbon: -0.239&lt;br /&gt;
&lt;br /&gt;
Hydrogen: 0.239&lt;br /&gt;
|Nitrogen: -1.102 &lt;br /&gt;
&lt;br /&gt;
Boron: 0.747&lt;br /&gt;
&lt;br /&gt;
Hydrogen (bonded to N): 0.432&lt;br /&gt;
&lt;br /&gt;
Hydrogen (bonded to B): -0.077&lt;br /&gt;
|-&lt;br /&gt;
!Discussion&lt;br /&gt;
|From the visualisation, it is shown that there is a slightly negative charge on the carbon atoms, and a positive charge of the same magnitude on the hydrogen atoms. All the carbon atoms have the same charge as they are in identical environments. The same applies to all the hydrogen atoms. This is due to the highly symmetrical structure of benzene. Since the same colour scale was used for both benzene and borazine, and the charges are much smaller in magnitude on atoms in benzene than atoms on borazine, the colours on the charge distribution visualisation is much darker. &lt;br /&gt;
|From the colours displayed on the charge distribution visualisation as well as the charge values, it is shown that nitrogen has a relatively large negative charge, while boron has a positive charge. This is due to the difference in electrogenativity between these atoms: nitrogen atoms are more electronegative than boron and tends to attract electrons towards themselves. It is worth noting that the hydrogen atoms do not all have the same charge. The hydrogen atoms bonded to boron have a slightly negative charge, and the ones bonded to nitrogen have a small positive charge. &lt;br /&gt;
&lt;br /&gt;
The fact that the same colour scale was used for both molecules comes in helpful here. It allows the charges on atoms to be compared directly. For example, just from looking at the colours, one can tell that or example, even though both carbon and nitrogen are electronegative, nitrogen is much more electronegative, which is quantitatively shown by Pauling&#039;s electronegativity scale.&amp;lt;ref&amp;gt;http://www.tutor-homework.com/Chemistry_Help/electronegativity_table/electronegativity.html (Date accessed: 24.0502018&amp;lt;/ref&amp;gt;&lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
===Comparative MOs of Benzene and Borazine===&lt;br /&gt;
&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot;&lt;br /&gt;
!&lt;br /&gt;
!Benzene&lt;br /&gt;
!Borazine&lt;br /&gt;
!Comparison and Discussion&lt;br /&gt;
|-&lt;br /&gt;
!1st comparative pair&lt;br /&gt;
|[[File:Hyc116_benzene_1st_MO_pair_7.png|200x200px|centre]]&lt;br /&gt;
|[[File:Hyc116_borazine_1st_MO_pair_level9.png|200x200px|centre]]&lt;br /&gt;
|MO 9 of both benzene and borazine are comparable. They both show delocalised molecular orbital with an overall bonding character. There is a nodal plane across the molecular orbitals for both benzene and borazine. For benzene, there is contribution from all the carbon and hydrogen s orbitals. Moreover, the molecular orbitals are symmetric to their counterpart of opposite phase. That is not the case for borazine; they are less symmetric in borazine. Nitrogen atoms are more electronegative than boron atoms and pull electron density towards themselves, resulting in a larger MO. There is contribution from all the boron and nitrogen s orbitals, and three of the hydrogen s orbitals, though not all of them. &lt;br /&gt;
|-&lt;br /&gt;
!2nd comparative pair&lt;br /&gt;
|[[File:Hyc116_benzene_2nd_MO_pair_10.png|200x200px|centre]]&lt;br /&gt;
|[[File:Hyc116_borazine_2nd_MO_pair_level11.png|200x200px|centre]]&lt;br /&gt;
|&lt;br /&gt;
|-&lt;br /&gt;
!3rd comparative pair&lt;br /&gt;
|[[File:Hyc116_benzene_3rd_MO_pair_21.png|200x200px|centre]]&lt;br /&gt;
|[[File:Hyc116_borazine_3rd_MO_pair_level21.png|200x200px|centre]]&lt;br /&gt;
|&lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
===Aromaticity: some theories===&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
==Reference==&lt;/div&gt;</summary>
		<author><name>Hyc116</name></author>
	</entry>
	<entry>
		<id>https://chemwiki.ch.ic.ac.uk/index.php?title=MO_hyc116&amp;diff=730149</id>
		<title>MO hyc116</title>
		<link rel="alternate" type="text/html" href="https://chemwiki.ch.ic.ac.uk/index.php?title=MO_hyc116&amp;diff=730149"/>
		<updated>2018-05-24T17:29:39Z</updated>

		<summary type="html">&lt;p&gt;Hyc116: &lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;==BH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;==&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;Calculation type&amp;lt;/b&amp;gt;: Optimisation&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;Calculation Method&amp;lt;/b&amp;gt;: B3LYP&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;Basis set&amp;lt;/b&amp;gt;: 6-31G(d,p) &lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Summary table&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
[[file:Hyc116_bh3_631g_opt_summarytable.png]]&lt;br /&gt;
&lt;br /&gt;
The above summary table was obtained after the 2nd optimisation of BH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt; (after the initial optimisation using the 3-21G basis set). Notice how the symmetry is incorrect and shown as Cs. This is because the symmetry was manually broken at the beginning by changing the bond length of B-H bonds. The point group was manually adjusted and the molecule was optimised again before the frequency analysis and the new summary table is attached below.&lt;br /&gt;
&lt;br /&gt;
[[file:Hyc116_bh3_correctsummarytable.png]]&lt;br /&gt;
&lt;br /&gt;
The above summary table was obtained from the optimisation after adjusting the symmetry. The point shown in this summary table is D&amp;lt;sub&amp;gt;3h&amp;lt;/sub&amp;gt;, which is the correct for BH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;. &lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Items table&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
Below is the items table taken from the optimisation with the correct point group.&lt;br /&gt;
&lt;br /&gt;
&amp;lt;pre&amp;gt;&lt;br /&gt;
Item               Value     Threshold  Converged?&lt;br /&gt;
 Maximum Force            0.000015     0.000450     YES&lt;br /&gt;
 RMS     Force            0.000010     0.000300     YES&lt;br /&gt;
 Maximum Displacement     0.000058     0.001800     YES&lt;br /&gt;
 RMS     Displacement     0.000038     0.001200     YES&lt;br /&gt;
&amp;lt;/pre&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Frequency log file&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
[[Media:HYC116 BH3 FREQ.LOG]] &lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Frequencies&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;pre&amp;gt;&lt;br /&gt;
Low frequencies ---  -10.3498   -3.4492   -1.2454   -0.0055    0.4779    3.2165&lt;br /&gt;
Low frequencies --- 1162.9519 1213.1527 1213.1554&lt;br /&gt;
&amp;lt;/pre&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;jmol of BH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;&#039;&#039;&#039;&lt;br /&gt;
&amp;lt;jmol&amp;gt;&amp;lt;jmolApplet&amp;gt;&lt;br /&gt;
  &amp;lt;title&amp;gt;optimised BH3&amp;lt;/title&amp;gt;&lt;br /&gt;
  &amp;lt;color&amp;gt;black&amp;lt;/color&amp;gt;&lt;br /&gt;
  &amp;lt;size&amp;gt;200&amp;lt;/size&amp;gt;&lt;br /&gt;
  &amp;lt;uploadedFileContents&amp;gt;HYC116_BH3_FREQ.LOG&amp;lt;/uploadedFileContents&amp;gt;&lt;br /&gt;
&amp;lt;/jmolApplet&amp;gt;&amp;lt;/jmol&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
===Vibrational spectrum===&lt;br /&gt;
&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot;&lt;br /&gt;
!wavenumber (cm&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;)&lt;br /&gt;
!Intensity (arbitrary units)&lt;br /&gt;
!symmetry&lt;br /&gt;
!IR active?&lt;br /&gt;
!type&lt;br /&gt;
|-&lt;br /&gt;
|1163&lt;br /&gt;
|93&lt;br /&gt;
|A&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;&#039; &#039;&lt;br /&gt;
|Yes&lt;br /&gt;
|Out of plane bend&lt;br /&gt;
|-&lt;br /&gt;
|1213&lt;br /&gt;
|14&lt;br /&gt;
|E&#039;&lt;br /&gt;
|Very slight&lt;br /&gt;
|Bend&lt;br /&gt;
|-&lt;br /&gt;
|1213&lt;br /&gt;
|14&lt;br /&gt;
|E&#039;&lt;br /&gt;
|Very slight&lt;br /&gt;
|Bend&lt;br /&gt;
|-&lt;br /&gt;
|2582&lt;br /&gt;
|0&lt;br /&gt;
|A&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;&#039;&lt;br /&gt;
|No&lt;br /&gt;
|Symmetric stretch&lt;br /&gt;
|-&lt;br /&gt;
|2716&lt;br /&gt;
|126&lt;br /&gt;
|E&#039;&lt;br /&gt;
|Yes&lt;br /&gt;
|Asymmetric stretch&lt;br /&gt;
|-&lt;br /&gt;
|2716&lt;br /&gt;
|126&lt;br /&gt;
|E&#039;&lt;br /&gt;
|Yes&lt;br /&gt;
|Asymmetric stretch&lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;IR spectrum&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
[[file:Hyc116_ir_bh3.png|400*600]]&lt;br /&gt;
&lt;br /&gt;
There are only three peaks on the IR spectrum of BH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;, despite that there are 6 vibrational modes for the molecule. As shown in the table above, the symmetric stretching mode with A1 symmetry at 2582 cm&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt; is not IR active; naturally, that vibrational mode doesn’t give a peak on the IR spectrum. As shown from the table, two pairs of vibrational modes, the bond angle deformation/bend at 1213 cm&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt; and the asymmetric bond stretch at 2716 cm&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;, are degenerate with the symmetry label E. This means that they have the same energy, and hence give the same wavenumber on the IR spectrum. Each pair of degenerate vibrational modes give rise to one peak. This leaves three peaks, as confirmed by the IR spectrum above.&lt;br /&gt;
&lt;br /&gt;
===Molecular orbitals of BH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;===&lt;br /&gt;
&lt;br /&gt;
[[file:hyc116_bh3_MO_diagram.png]]&lt;br /&gt;
&lt;br /&gt;
The above molecular orbital diagram was taken from Dr Patricia Hunt&#039;s &amp;lt;i&amp;gt;Lecture 4 Tutorial Problem Model Answers&amp;lt;/i&amp;gt;. &amp;lt;ref&amp;gt;P. Hunt, &amp;quot;Lecture 4 Tutorial Problem Model Answers&amp;quot;, 2 (2018)&amp;lt;/ref&amp;gt;. Diagrams of the &amp;quot;real&amp;quot; MOs were obtained from Gaussian.&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
There is no significant difference between the LCAO MOs and the real ones. Features such as orbital phases are shown clearly on both the LCAO MOs and the real MOs, illustrating the bonding/anti-bonding characters of the molecular orbitals. This suggests that the the qualitative MO theory is highly accurate and useful when studying the molecular orbitals of molecules.&lt;br /&gt;
&lt;br /&gt;
==Associated energies: ammonium borane==&lt;br /&gt;
&lt;br /&gt;
===NH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;===&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;Calculation type&amp;lt;/b&amp;gt;: Optimisation&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;Calculation Method&amp;lt;/b&amp;gt;: B3LYP&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;Basis set&amp;lt;/b&amp;gt;: 6-31G(d,p) &lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Summary table&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
[[file:Hyc116_nh3_631g_summarytable.png]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Items table&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;pre&amp;gt;&lt;br /&gt;
Item               Value     Threshold  Converged?&lt;br /&gt;
 Maximum Force            0.000006     0.000450     YES&lt;br /&gt;
 RMS     Force            0.000004     0.000300     YES&lt;br /&gt;
 Maximum Displacement     0.000012     0.001800     YES&lt;br /&gt;
 RMS     Displacement     0.000008     0.001200     YES&lt;br /&gt;
&amp;lt;/pre&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Frequency log file&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
[[Media:HYC116_NH3_FREQ.LOG]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Frequencies&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;pre&amp;gt;&lt;br /&gt;
Low frequencies ---   -8.5646   -8.5588   -0.0047    0.0454    0.1784   26.4183&lt;br /&gt;
Low frequencies --- 1089.7603 1694.1865 1694.1865&lt;br /&gt;
&amp;lt;/pre&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;jmol of NH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;&#039;&#039;&#039;&lt;br /&gt;
&amp;lt;jmol&amp;gt;&amp;lt;jmolApplet&amp;gt;&lt;br /&gt;
  &amp;lt;title&amp;gt;optimised NH3&amp;lt;/title&amp;gt;&lt;br /&gt;
  &amp;lt;color&amp;gt;black&amp;lt;/color&amp;gt;&lt;br /&gt;
  &amp;lt;size&amp;gt;200&amp;lt;/size&amp;gt;&lt;br /&gt;
  &amp;lt;uploadedFileContents&amp;gt;HYC116_NH3_FREQ.LOG&amp;lt;/uploadedFileContents&amp;gt;&lt;br /&gt;
&amp;lt;/jmolApplet&amp;gt;&amp;lt;/jmol&amp;gt;&lt;br /&gt;
&lt;br /&gt;
===NH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;BH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;===&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;Calculation type&amp;lt;/b&amp;gt;: Optimisation&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;Calculation Method&amp;lt;/b&amp;gt;: B3LYP&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;Basis set&amp;lt;/b&amp;gt;: 6-31G(d,p) &lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Summary table&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
[[file:Hyc116_nh3bh3_631g_summarytable.png]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Items table&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;pre&amp;gt;&lt;br /&gt;
Item               Value     Threshold  Converged?&lt;br /&gt;
 Maximum Force            0.000123     0.000450     YES&lt;br /&gt;
 RMS     Force            0.000058     0.000300     YES&lt;br /&gt;
 Maximum Displacement     0.000515     0.001800     YES&lt;br /&gt;
 RMS     Displacement     0.000296     0.001200     YES&lt;br /&gt;
&amp;lt;/pre&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Frequency log file&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
[[Media:HYC116_NH3BH3_FREQ.LOG]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Frequencies&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;pre&amp;gt;&lt;br /&gt;
Low frequencies ---   -0.0014   -0.0011   -0.0006    6.9624   20.4518   43.5542&lt;br /&gt;
Low frequencies ---  266.4530  632.2458  639.0504&lt;br /&gt;
&amp;lt;/pre&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;jmol of NH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;BH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;&#039;&#039;&#039;&lt;br /&gt;
&amp;lt;jmol&amp;gt;&amp;lt;jmolApplet&amp;gt;&lt;br /&gt;
  &amp;lt;title&amp;gt;optimised NH3BH3&amp;lt;/title&amp;gt;&lt;br /&gt;
  &amp;lt;color&amp;gt;black&amp;lt;/color&amp;gt;&lt;br /&gt;
  &amp;lt;size&amp;gt;200&amp;lt;/size&amp;gt;&lt;br /&gt;
  &amp;lt;uploadedFileContents&amp;gt;HYC116_NH3BH3_FREQ.LOG&amp;lt;/uploadedFileContents&amp;gt;&lt;br /&gt;
&amp;lt;/jmolApplet&amp;gt;&amp;lt;/jmol&amp;gt;&lt;br /&gt;
&lt;br /&gt;
===Association energy===&lt;br /&gt;
&lt;br /&gt;
E(BH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;) (using the optimisation with the correct symmetry) = -26.61532363 a.u. = &amp;lt;b&amp;gt;-26.61532 a.u. (5 d.p.)&amp;lt;/b&amp;gt;&lt;br /&gt;
&lt;br /&gt;
E(NH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;) = -56.55776873 a.u. = &amp;lt;b&amp;gt;-56.55777 a.u. (5 d.p.)&amp;lt;/b&amp;gt;&lt;br /&gt;
&lt;br /&gt;
E(NH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;BH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;) = -83.22468893 a.u. = &amp;lt;b&amp;gt;-83.22469 a.u. (5 d.p.)&amp;lt;/b&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
Carrying out calculations using numbers which has already been rounded up can possibly result in errors in the last digit. Hence, here the calculations were carried out using the numbers provided from the optimisations (i.e. with more decimal places than necessary); the answer was then rounded up to the desired accuracy. &lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
ΔE = E(NH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;BH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;)-[E(NH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;)+E(BH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;)]&lt;br /&gt;
&lt;br /&gt;
ΔE = -83.22468893 - (-56.55776873 + -26.61532363) = -0.05159657 a.u. &lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;ΔE = -0.05160 a.u. (5 d.p.)&amp;lt;/b&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Converting energy from a.u. to kJ/mol&#039;&#039;&#039;&lt;br /&gt;
An atomic unit for energy is Hartree, which is equal to 2625.5 kJ/mol. &amp;lt;ref&amp;gt;https://cccbdb.nist.gov/hartree.asp (Accessed: 22.05.2018)&amp;lt;/ref&amp;gt;&lt;br /&gt;
&lt;br /&gt;
So ΔE in kJ/mol = -0.05159657 * 2625.5 = -135.466794535 kJ/mol&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;ΔE = -135 kJ/mol (nearest integer)&amp;lt;/b&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
The energy difference calculated above comes from the formation of the B-N dative bond. It is a relatively weak bond. According to a bond energy data sheet provided by the University of California, &amp;lt;ref&amp;gt;https://labs.chem.ucsb.edu/zakarian/armen/11---bonddissociationenergy.pdf (Accessed on 24.05.2018)&amp;lt;/ref&amp;gt; the bond energy of the C-C bond of an ethane molecule is 368 kJ/mol. This is a fair comparison to the NH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;BH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt; molecule as the two molecules have the same structure, only with the carbon atoms on ethane swapped for Boron and Nitrogen in NH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;BH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;&lt;br /&gt;
&lt;br /&gt;
==Using a mixture of basis-sets and pseudo-potentials==&lt;br /&gt;
&lt;br /&gt;
===BBr&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;===&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;Calculation type&amp;lt;/b&amp;gt;: Optimisation&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;Calculation Method&amp;lt;/b&amp;gt;: B3LYP&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;Basis set&amp;lt;/b&amp;gt;: Boron: 6-31G(d,p) ; Br: LANL2DZ&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
Larger calculations are often sent to a web-server to run on a high-performance computer instead of a desktop. In order to experience and learn to use a web-server, the optimisation and the frequency analysis for BBr&amp;lt;sub&amp;gt;3&amp;lt;/sub were both sent and done on a server instead of the desktop. The calculation results were downloaded from the web-server once they were finished.   &lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Summary table&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
[[file:Hyc116_bbr3_opt_summarytable.png]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Items table&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;pre&amp;gt;&lt;br /&gt;
Item               Value     Threshold  Converged?&lt;br /&gt;
 Maximum Force            0.000008     0.000450     YES&lt;br /&gt;
 RMS     Force            0.000005     0.000300     YES&lt;br /&gt;
 Maximum Displacement     0.000036     0.001800     YES&lt;br /&gt;
 RMS     Displacement     0.000023     0.001200     YES&lt;br /&gt;
&amp;lt;/pre&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Frequency log file&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
[[Media:Hyc116_bbr3_freq.log]]&lt;br /&gt;
&lt;br /&gt;
Attached above is the frequency file saved onto the computer from the SCAN server portal. The frequency file was also published on the chemistry database DSpace. {{DOI|10042/202442}}&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Frequencies&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;pre&amp;gt;&lt;br /&gt;
Low frequencies ---   -0.0137   -0.0064   -0.0046    2.4315    2.4315    4.8421&lt;br /&gt;
Low frequencies ---  155.9631  155.9651  267.7052&lt;br /&gt;
&amp;lt;/pre&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;jmol of BBr&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;&#039;&#039;&#039;&lt;br /&gt;
&amp;lt;jmol&amp;gt;&amp;lt;jmolApplet&amp;gt;&lt;br /&gt;
  &amp;lt;title&amp;gt;optimised BBr3&amp;lt;/title&amp;gt;&lt;br /&gt;
  &amp;lt;color&amp;gt;black&amp;lt;/color&amp;gt;&lt;br /&gt;
  &amp;lt;size&amp;gt;200&amp;lt;/size&amp;gt;&lt;br /&gt;
  &amp;lt;uploadedFileContents&amp;gt;Hyc116_bbr3_freq.log&amp;lt;/uploadedFileContents&amp;gt;&lt;br /&gt;
&amp;lt;/jmolApplet&amp;gt;&amp;lt;/jmol&amp;gt;&lt;br /&gt;
&lt;br /&gt;
==Aromaticity==&lt;br /&gt;
&lt;br /&gt;
===Benzene===&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;Calculation type&amp;lt;/b&amp;gt;: Optimisation&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;Calculation Method&amp;lt;/b&amp;gt;: B3LYP&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;Basis set&amp;lt;/b&amp;gt;: 6-31G(d,p) &lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Summary table&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
[[file:Hyc116_c6h6_summarytable.png]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Items table&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;pre&amp;gt;&lt;br /&gt;
Item               Value     Threshold  Converged?&lt;br /&gt;
 Maximum Force            0.000193     0.000450     YES&lt;br /&gt;
 RMS     Force            0.000079     0.000300     YES&lt;br /&gt;
 Maximum Displacement     0.000830     0.001800     YES&lt;br /&gt;
 RMS     Displacement     0.000294     0.001200     YES&lt;br /&gt;
&amp;lt;/pre&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Frequency log file&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
[[Media:HYC116_C6H6_FREQ.LOG]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Frequencies&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;pre&amp;gt;&lt;br /&gt;
Low frequencies ---   -3.5606   -3.5606   -0.0089   -0.0043   -0.0043   10.0905&lt;br /&gt;
Low frequencies ---  413.9582  413.9582  621.1416&lt;br /&gt;
&amp;lt;/pre&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;jmol of C&amp;lt;sub&amp;gt;6&amp;lt;/sub&amp;gt;H&amp;lt;sub&amp;gt;6&amp;lt;/sub&amp;gt;&#039;&#039;&#039;&lt;br /&gt;
&amp;lt;jmol&amp;gt;&amp;lt;jmolApplet&amp;gt;&lt;br /&gt;
  &amp;lt;title&amp;gt;optimised Benzene&amp;lt;/title&amp;gt;&lt;br /&gt;
  &amp;lt;color&amp;gt;black&amp;lt;/color&amp;gt;&lt;br /&gt;
  &amp;lt;size&amp;gt;200&amp;lt;/size&amp;gt;&lt;br /&gt;
  &amp;lt;uploadedFileContents&amp;gt;HYC116_C6H6_FREQ.LOG&amp;lt;/uploadedFileContents&amp;gt;&lt;br /&gt;
&amp;lt;/jmolApplet&amp;gt;&amp;lt;/jmol&amp;gt;&lt;br /&gt;
&lt;br /&gt;
===Borazine===&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;Calculation type&amp;lt;/b&amp;gt;: Optimisation&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;Calculation Method&amp;lt;/b&amp;gt;: B3LYP&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;Basis set&amp;lt;/b&amp;gt;: 6-31G(d,p) &lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Summary table&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
[[file:Hyc116_borazine_summarytable.png]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Items table&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;pre&amp;gt;&lt;br /&gt;
Item               Value     Threshold  Converged?&lt;br /&gt;
 Maximum Force            0.000085     0.000450     YES&lt;br /&gt;
 RMS     Force            0.000033     0.000300     YES&lt;br /&gt;
 Maximum Displacement     0.000250     0.001800     YES&lt;br /&gt;
 RMS     Displacement     0.000074     0.001200     YES&lt;br /&gt;
&amp;lt;/pre&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Frequency log file&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
[[Media:HYC116_BORAZINE_FREQ.LOG]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Frequencies&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;pre&amp;gt;&lt;br /&gt;
Low frequencies ---  -12.6626  -12.6626   -8.9272   -0.0211   -0.0104   -0.0104&lt;br /&gt;
Low frequencies ---  289.1112  289.1112  403.8613&lt;br /&gt;
&amp;lt;/pre&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;jmol of Borazine&#039;&#039;&#039;&lt;br /&gt;
&amp;lt;jmol&amp;gt;&amp;lt;jmolApplet&amp;gt;&lt;br /&gt;
  &amp;lt;title&amp;gt;optimised Borazine&amp;lt;/title&amp;gt;&lt;br /&gt;
  &amp;lt;color&amp;gt;black&amp;lt;/color&amp;gt;&lt;br /&gt;
  &amp;lt;size&amp;gt;200&amp;lt;/size&amp;gt;&lt;br /&gt;
  &amp;lt;uploadedFileContents&amp;gt;HYC116_BORAZINE_FREQ.LOG&amp;lt;/uploadedFileContents&amp;gt;&lt;br /&gt;
&amp;lt;/jmolApplet&amp;gt;&amp;lt;/jmol&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
===Charge distribution===&lt;br /&gt;
&lt;br /&gt;
An NBO charge analysis was carried out on both the optimised benzene and borazine. Visualisations of the charge distribution are shown in the table below, with the colour range going from -1.102 to 1.102 for both molecule. This large scale was chosen as it allows direct comparison of the charge on any atoms in these two molecules and shows the relative magnitude of charges on all these atoms. Negative charges are shown in red, and positive charges are shown in green. A neutral charge is displayed in black, so the smaller a charge is (positive or negative), the darker its colour representation is. Larger charges are shown in brighter colours. The charges are also displayed on the atoms as numbers with a neutral charge being zero. Negative charges are shown as negative number and positive charges are shown as positive numbers. &lt;br /&gt;
&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot;&lt;br /&gt;
!&lt;br /&gt;
!Benzene&lt;br /&gt;
!Borazine&lt;br /&gt;
|-&lt;br /&gt;
!Visualisation of charge distribution&lt;br /&gt;
|[[File:Hyc116_benzene_charge_distribution1.png|500x500px|thumb|centre|Charge distribution of Benzene visualisation]]&lt;br /&gt;
|[[File:Hyc116_borazine_charge_distribution1.png|500x500px|thumb|centre|Charge distribution of Borazine visualisation]]&lt;br /&gt;
|-&lt;br /&gt;
!Charge &lt;br /&gt;
|Carbon: -0.239&lt;br /&gt;
&lt;br /&gt;
Hydrogen: 0.239&lt;br /&gt;
|Nitrogen: -1.102 &lt;br /&gt;
&lt;br /&gt;
Boron: 0.747&lt;br /&gt;
&lt;br /&gt;
Hydrogen (bonded to N): 0.432&lt;br /&gt;
&lt;br /&gt;
Hydrogen (bonded to B): -0.077&lt;br /&gt;
|-&lt;br /&gt;
!Discussion&lt;br /&gt;
|From the visualisation, it is shown that there is a slightly negative charge on the carbon atoms, and a positive charge of the same magnitude on the hydrogen atoms. All the carbon atoms have the same charge as they are in identical environments. The same applies to all the hydrogen atoms. This is due to the highly symmetrical structure of benzene. Since the same colour scale was used for both benzene and borazine, and the charges are much smaller in magnitude on atoms in benzene than atoms on borazine, the colours on the charge distribution visualisation is much darker. &lt;br /&gt;
|From the colours displayed on the charge distribution visualisation as well as the charge values, it is shown that nitrogen has a relatively large negative charge, while boron has a positive charge. This is due to the difference in electrogenativity between these atoms: nitrogen atoms are more electronegative than boron and tends to attract electrons towards themselves. It is worth noting that the hydrogen atoms do not all have the same charge. The hydrogen atoms bonded to boron have a slightly negative charge, and the ones bonded to nitrogen have a small positive charge. &lt;br /&gt;
&lt;br /&gt;
The fact that the same colour scale was used for both molecules comes in helpful here. It allows the charges on atoms to be compared directly. For example, just from looking at the colours, one can tell that or example, even though both carbon and nitrogen are electronegative, nitrogen is much more electronegative, which is quantitatively shown by Pauling&#039;s electronegativity scale.&amp;lt;ref&amp;gt;http://www.tutor-homework.com/Chemistry_Help/electronegativity_table/electronegativity.html (Date accessed: 24.0502018&amp;lt;/ref&amp;gt;&lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
===Comparative MOs of Benzene and Borazine===&lt;br /&gt;
&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot;&lt;br /&gt;
!&lt;br /&gt;
!Benzene&lt;br /&gt;
!Borazine&lt;br /&gt;
!Comparison and Discussion&lt;br /&gt;
|-&lt;br /&gt;
!1st comparative pair&lt;br /&gt;
|[[File:Hyc116_benzene_1st_MO_pair_7.png|200x200px|centre]]&lt;br /&gt;
|[[File:Hyc116_borazine_1st_MO_pair_level9.png|200x200px|centre]]&lt;br /&gt;
|MO 9 of both benzene and borazine are comparable. They both show delocalised molecular orbital with an overall bonding character. There is a nodal plane across the molecular orbitals for both benzene and borazine. For benzene, there is contribution from all the carbon and hydrogen s orbitals. Moreover, the molecular orbitals are symmetric to their counterpart of opposite phase. That is not the case for borazine; they are less symmetric in borazine. Nitrogen atoms are more electronegative than boron atoms and pull electron density towards themselves, resulting in a larger MO. There is contribution from all the boron and nitrogen s orbitals, and three of the hydrogen s orbitals, though not all of them. &lt;br /&gt;
|-&lt;br /&gt;
!2nd comparative pair&lt;br /&gt;
|[[File:Hyc116_benzene_2nd_MO_pair_10.png|200x200px|centre]]&lt;br /&gt;
|[[File:Hyc116_borazine_2nd_MO_pair_level11.png|200x200px|centre]]&lt;br /&gt;
|&lt;br /&gt;
|-&lt;br /&gt;
!3rd comparative pair&lt;br /&gt;
|[[File:Hyc116_benzene_3rd_MO_pair_21.png|200x200px|centre]]&lt;br /&gt;
|[[File:Hyc116_borazine_3rd_MO_pair_level21.png|200x200px|centre]]&lt;br /&gt;
|&lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
===Aromaticity: some theories===&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
==Reference==&lt;/div&gt;</summary>
		<author><name>Hyc116</name></author>
	</entry>
	<entry>
		<id>https://chemwiki.ch.ic.ac.uk/index.php?title=MO_hyc116&amp;diff=730148</id>
		<title>MO hyc116</title>
		<link rel="alternate" type="text/html" href="https://chemwiki.ch.ic.ac.uk/index.php?title=MO_hyc116&amp;diff=730148"/>
		<updated>2018-05-24T17:29:01Z</updated>

		<summary type="html">&lt;p&gt;Hyc116: /* Using a mixture of basis-sets and pseudo-potentials */&lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;==BH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;==&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;Calculation type&amp;lt;/b&amp;gt;: Optimisation&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;Calculation Method&amp;lt;/b&amp;gt;: B3LYP&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;Basis set&amp;lt;/b&amp;gt;: 6-31G(d,p) &lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Summary table&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
[[file:Hyc116_bh3_631g_opt_summarytable.png]]&lt;br /&gt;
&lt;br /&gt;
The above summary table was obtained after the 2nd optimisation of BH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt; (after the initial optimisation using the 3-21G basis set). Notice how the symmetry is incorrect and shown as Cs. This is because the symmetry was manually broken at the beginning by changing the bond length of B-H bonds. The point group was manually adjusted and the molecule was optimised again before the frequency analysis and the new summary table is attached below.&lt;br /&gt;
&lt;br /&gt;
[[file:Hyc116_bh3_correctsummarytable.png]]&lt;br /&gt;
&lt;br /&gt;
The above summary table was obtained from the optimisation after adjusting the symmetry. The point shown in this summary table is D&amp;lt;sub&amp;gt;3h&amp;lt;/sub&amp;gt;, which is the correct for BH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;. &lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Items table&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
Below is the items table taken from the optimisation with the correct point group.&lt;br /&gt;
&lt;br /&gt;
&amp;lt;pre&amp;gt;&lt;br /&gt;
Item               Value     Threshold  Converged?&lt;br /&gt;
 Maximum Force            0.000015     0.000450     YES&lt;br /&gt;
 RMS     Force            0.000010     0.000300     YES&lt;br /&gt;
 Maximum Displacement     0.000058     0.001800     YES&lt;br /&gt;
 RMS     Displacement     0.000038     0.001200     YES&lt;br /&gt;
&amp;lt;/pre&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Frequency log file&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
[[Media:HYC116 BH3 FREQ.LOG]] &lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Frequencies&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;pre&amp;gt;&lt;br /&gt;
Low frequencies ---  -10.3498   -3.4492   -1.2454   -0.0055    0.4779    3.2165&lt;br /&gt;
Low frequencies --- 1162.9519 1213.1527 1213.1554&lt;br /&gt;
&amp;lt;/pre&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;jmol of BH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;&#039;&#039;&#039;&lt;br /&gt;
&amp;lt;jmol&amp;gt;&amp;lt;jmolApplet&amp;gt;&lt;br /&gt;
  &amp;lt;title&amp;gt;optimised BH3&amp;lt;/title&amp;gt;&lt;br /&gt;
  &amp;lt;color&amp;gt;black&amp;lt;/color&amp;gt;&lt;br /&gt;
  &amp;lt;size&amp;gt;200&amp;lt;/size&amp;gt;&lt;br /&gt;
  &amp;lt;uploadedFileContents&amp;gt;HYC116_BH3_FREQ.LOG&amp;lt;/uploadedFileContents&amp;gt;&lt;br /&gt;
&amp;lt;/jmolApplet&amp;gt;&amp;lt;/jmol&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
===Vibrational spectrum===&lt;br /&gt;
&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot;&lt;br /&gt;
!wavenumber (cm&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;)&lt;br /&gt;
!Intensity (arbitrary units)&lt;br /&gt;
!symmetry&lt;br /&gt;
!IR active?&lt;br /&gt;
!type&lt;br /&gt;
|-&lt;br /&gt;
|1163&lt;br /&gt;
|93&lt;br /&gt;
|A&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;&#039; &#039;&lt;br /&gt;
|Yes&lt;br /&gt;
|Out of plane bend&lt;br /&gt;
|-&lt;br /&gt;
|1213&lt;br /&gt;
|14&lt;br /&gt;
|E&#039;&lt;br /&gt;
|Very slight&lt;br /&gt;
|Bend&lt;br /&gt;
|-&lt;br /&gt;
|1213&lt;br /&gt;
|14&lt;br /&gt;
|E&#039;&lt;br /&gt;
|Very slight&lt;br /&gt;
|Bend&lt;br /&gt;
|-&lt;br /&gt;
|2582&lt;br /&gt;
|0&lt;br /&gt;
|A&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;&#039;&lt;br /&gt;
|No&lt;br /&gt;
|Symmetric stretch&lt;br /&gt;
|-&lt;br /&gt;
|2716&lt;br /&gt;
|126&lt;br /&gt;
|E&#039;&lt;br /&gt;
|Yes&lt;br /&gt;
|Asymmetric stretch&lt;br /&gt;
|-&lt;br /&gt;
|2716&lt;br /&gt;
|126&lt;br /&gt;
|E&#039;&lt;br /&gt;
|Yes&lt;br /&gt;
|Asymmetric stretch&lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;IR spectrum&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
[[file:Hyc116_ir_bh3.png|400*600]]&lt;br /&gt;
&lt;br /&gt;
There are only three peaks on the IR spectrum of BH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;, despite that there are 6 vibrational modes for the molecule. As shown in the table above, the symmetric stretching mode with A1 symmetry at 2582 cm&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt; is not IR active; naturally, that vibrational mode doesn’t give a peak on the IR spectrum. As shown from the table, two pairs of vibrational modes, the bond angle deformation/bend at 1213 cm&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt; and the asymmetric bond stretch at 2716 cm&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;, are degenerate with the symmetry label E. This means that they have the same energy, and hence give the same wavenumber on the IR spectrum. Each pair of degenerate vibrational modes give rise to one peak. This leaves three peaks, as confirmed by the IR spectrum above.&lt;br /&gt;
&lt;br /&gt;
===Molecular orbitals of BH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;===&lt;br /&gt;
&lt;br /&gt;
[[file:hyc116_bh3_MO_diagram.png]]&lt;br /&gt;
&lt;br /&gt;
The above molecular orbital diagram was taken from Dr Patricia Hunt&#039;s &amp;lt;i&amp;gt;Lecture 4 Tutorial Problem Model Answers&amp;lt;/i&amp;gt;. &amp;lt;ref&amp;gt;P. Hunt, &amp;quot;Lecture 4 Tutorial Problem Model Answers&amp;quot;, 2 (2018)&amp;lt;/ref&amp;gt;. Diagrams of the &amp;quot;real&amp;quot; MOs were obtained from Gaussian.&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
There is no significant difference between the LCAO MOs and the real ones. Features such as orbital phases are shown clearly on both the LCAO MOs and the real MOs, illustrating the bonding/anti-bonding characters of the molecular orbitals. This suggests that the the qualitative MO theory is highly accurate and useful when studying the molecular orbitals of molecules.&lt;br /&gt;
&lt;br /&gt;
==Associated energies: ammonium borane==&lt;br /&gt;
&lt;br /&gt;
===NH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;===&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;Calculation type&amp;lt;/b&amp;gt;: Optimisation&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;Calculation Method&amp;lt;/b&amp;gt;: B3LYP&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;Basis set&amp;lt;/b&amp;gt;: 6-31G(d,p) &lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Summary table&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
[[file:Hyc116_nh3_631g_summarytable.png]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Items table&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;pre&amp;gt;&lt;br /&gt;
Item               Value     Threshold  Converged?&lt;br /&gt;
 Maximum Force            0.000006     0.000450     YES&lt;br /&gt;
 RMS     Force            0.000004     0.000300     YES&lt;br /&gt;
 Maximum Displacement     0.000012     0.001800     YES&lt;br /&gt;
 RMS     Displacement     0.000008     0.001200     YES&lt;br /&gt;
&amp;lt;/pre&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Frequency log file&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
[[Media:HYC116_NH3_FREQ.LOG]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Frequencies&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;pre&amp;gt;&lt;br /&gt;
Low frequencies ---   -8.5646   -8.5588   -0.0047    0.0454    0.1784   26.4183&lt;br /&gt;
Low frequencies --- 1089.7603 1694.1865 1694.1865&lt;br /&gt;
&amp;lt;/pre&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;jmol of NH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;&#039;&#039;&#039;&lt;br /&gt;
&amp;lt;jmol&amp;gt;&amp;lt;jmolApplet&amp;gt;&lt;br /&gt;
  &amp;lt;title&amp;gt;optimised NH3&amp;lt;/title&amp;gt;&lt;br /&gt;
  &amp;lt;color&amp;gt;black&amp;lt;/color&amp;gt;&lt;br /&gt;
  &amp;lt;size&amp;gt;200&amp;lt;/size&amp;gt;&lt;br /&gt;
  &amp;lt;uploadedFileContents&amp;gt;HYC116_NH3_FREQ.LOG&amp;lt;/uploadedFileContents&amp;gt;&lt;br /&gt;
&amp;lt;/jmolApplet&amp;gt;&amp;lt;/jmol&amp;gt;&lt;br /&gt;
&lt;br /&gt;
===NH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;BH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;===&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;Calculation type&amp;lt;/b&amp;gt;: Optimisation&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;Calculation Method&amp;lt;/b&amp;gt;: B3LYP&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;Basis set&amp;lt;/b&amp;gt;: 6-31G(d,p) &lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Summary table&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
[[file:Hyc116_nh3bh3_631g_summarytable.png]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Items table&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;pre&amp;gt;&lt;br /&gt;
Item               Value     Threshold  Converged?&lt;br /&gt;
 Maximum Force            0.000123     0.000450     YES&lt;br /&gt;
 RMS     Force            0.000058     0.000300     YES&lt;br /&gt;
 Maximum Displacement     0.000515     0.001800     YES&lt;br /&gt;
 RMS     Displacement     0.000296     0.001200     YES&lt;br /&gt;
&amp;lt;/pre&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Frequency log file&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
[[Media:HYC116_NH3BH3_FREQ.LOG]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Frequencies&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;pre&amp;gt;&lt;br /&gt;
Low frequencies ---   -0.0014   -0.0011   -0.0006    6.9624   20.4518   43.5542&lt;br /&gt;
Low frequencies ---  266.4530  632.2458  639.0504&lt;br /&gt;
&amp;lt;/pre&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;jmol of NH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;BH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;&#039;&#039;&#039;&lt;br /&gt;
&amp;lt;jmol&amp;gt;&amp;lt;jmolApplet&amp;gt;&lt;br /&gt;
  &amp;lt;title&amp;gt;optimised NH3BH3&amp;lt;/title&amp;gt;&lt;br /&gt;
  &amp;lt;color&amp;gt;black&amp;lt;/color&amp;gt;&lt;br /&gt;
  &amp;lt;size&amp;gt;200&amp;lt;/size&amp;gt;&lt;br /&gt;
  &amp;lt;uploadedFileContents&amp;gt;HYC116_NH3BH3_FREQ.LOG&amp;lt;/uploadedFileContents&amp;gt;&lt;br /&gt;
&amp;lt;/jmolApplet&amp;gt;&amp;lt;/jmol&amp;gt;&lt;br /&gt;
&lt;br /&gt;
===Association energy===&lt;br /&gt;
&lt;br /&gt;
E(BH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;) (using the optimisation with the correct symmetry) = -26.61532363 a.u. = &amp;lt;b&amp;gt;-26.61532 a.u. (5 d.p.)&amp;lt;/b&amp;gt;&lt;br /&gt;
&lt;br /&gt;
E(NH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;) = -56.55776873 a.u. = &amp;lt;b&amp;gt;-56.55777 a.u. (5 d.p.)&amp;lt;/b&amp;gt;&lt;br /&gt;
&lt;br /&gt;
E(NH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;BH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;) = -83.22468893 a.u. = &amp;lt;b&amp;gt;-83.22469 a.u. (5 d.p.)&amp;lt;/b&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
Carrying out calculations using numbers which has already been rounded up can possibly result in errors in the last digit. Hence, here the calculations were carried out using the numbers provided from the optimisations (i.e. with more decimal places than necessary); the answer was then rounded up to the desired accuracy. &lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
ΔE = E(NH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;BH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;)-[E(NH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;)+E(BH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;)]&lt;br /&gt;
&lt;br /&gt;
ΔE = -83.22468893 - (-56.55776873 + -26.61532363) = -0.05159657 a.u. &lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;ΔE = -0.05160 a.u. (5 d.p.)&amp;lt;/b&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Converting energy from a.u. to kJ/mol&#039;&#039;&#039;&lt;br /&gt;
An atomic unit for energy is Hartree, which is equal to 2625.5 kJ/mol. &amp;lt;ref&amp;gt;https://cccbdb.nist.gov/hartree.asp (Accessed: 22.05.2018)&amp;lt;/ref&amp;gt;&lt;br /&gt;
&lt;br /&gt;
So ΔE in kJ/mol = -0.05159657 * 2625.5 = -135.466794535 kJ/mol&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;ΔE = -135 kJ/mol (nearest integer)&amp;lt;/b&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
The energy difference calculated above comes from the formation of the B-N dative bond. It is a relatively weak bond. According to a bond energy data sheet provided by the University of California, &amp;lt;ref&amp;gt;https://labs.chem.ucsb.edu/zakarian/armen/11---bonddissociationenergy.pdf (Accessed on 24.05.2018)&amp;lt;/ref&amp;gt; the bond energy of the C-C bond of an ethane molecule is 368 kJ/mol. This is a fair comparison to the NH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;BH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt; molecule as the two molecules have the same structure, only with the carbon atoms on ethane swapped for Boron and Nitrogen in NH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;BH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;&lt;br /&gt;
&lt;br /&gt;
==Using a mixture of basis-sets and pseudo-potentials==&lt;br /&gt;
&lt;br /&gt;
===BBr&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;===&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;Calculation type&amp;lt;/b&amp;gt;: Optimisation&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;Calculation Method&amp;lt;/b&amp;gt;: B3LYP&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;Basis set&amp;lt;/b&amp;gt;: Boron: 6-31G(d,p) ; Br: LANL2DZ&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
Larger calculations are often sent to a web-server to run on a high-performance computer instead of a desktop. In order to experience and learn to use a web-server, the optimisation and the frequency analysis for BBr&amp;lt;sub&amp;gt;3&amp;lt;/sub were both sent and done on a server instead of the desktop. The calculation results were downloaded from the web-server once they were finished.   &lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Summary table&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
[[file:Hyc116_bbr3_opt_summarytable.png]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Items table&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;pre&amp;gt;&lt;br /&gt;
Item               Value     Threshold  Converged?&lt;br /&gt;
 Maximum Force            0.000008     0.000450     YES&lt;br /&gt;
 RMS     Force            0.000005     0.000300     YES&lt;br /&gt;
 Maximum Displacement     0.000036     0.001800     YES&lt;br /&gt;
 RMS     Displacement     0.000023     0.001200     YES&lt;br /&gt;
&amp;lt;/pre&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Frequency log file&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
[[Media:Hyc116_bbr3_freq.log]]&lt;br /&gt;
&lt;br /&gt;
Attached above is the frequency file saved onto the computer from the SCAN server portal. The frequency file was also published on the chemistry database DSpace. {{DOI|10042/202442}}&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Frequencies&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;pre&amp;gt;&lt;br /&gt;
Low frequencies ---   -0.0137   -0.0064   -0.0046    2.4315    2.4315    4.8421&lt;br /&gt;
Low frequencies ---  155.9631  155.9651  267.7052&lt;br /&gt;
&amp;lt;/pre&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;jmol of BBr&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;&#039;&#039;&#039;&lt;br /&gt;
&amp;lt;jmol&amp;gt;&amp;lt;jmolApplet&amp;gt;&lt;br /&gt;
  &amp;lt;title&amp;gt;optimised BBr3&amp;lt;/title&amp;gt;&lt;br /&gt;
  &amp;lt;color&amp;gt;black&amp;lt;/color&amp;gt;&lt;br /&gt;
  &amp;lt;size&amp;gt;200&amp;lt;/size&amp;gt;&lt;br /&gt;
  &amp;lt;uploadedFileContents&amp;gt;Hyc116_bbr3_freq.log&amp;lt;/uploadedFileContents&amp;gt;&lt;br /&gt;
&amp;lt;/jmolApplet&amp;gt;&amp;lt;/jmol&amp;gt;&lt;br /&gt;
&lt;br /&gt;
==Aromaticity==&lt;br /&gt;
&lt;br /&gt;
===Benzene===&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;Calculation type&amp;lt;/b&amp;gt;: Optimisation&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;Calculation Method&amp;lt;/b&amp;gt;: B3LYP&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;Basis set&amp;lt;/b&amp;gt;: 6-31G(d,p) &lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Summary table&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
[[file:Hyc116_c6h6_summarytable.png]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Items table&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;pre&amp;gt;&lt;br /&gt;
Item               Value     Threshold  Converged?&lt;br /&gt;
 Maximum Force            0.000193     0.000450     YES&lt;br /&gt;
 RMS     Force            0.000079     0.000300     YES&lt;br /&gt;
 Maximum Displacement     0.000830     0.001800     YES&lt;br /&gt;
 RMS     Displacement     0.000294     0.001200     YES&lt;br /&gt;
&amp;lt;/pre&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Frequency log file&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
[[Media:HYC116_C6H6_FREQ.LOG]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Frequencies&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;pre&amp;gt;&lt;br /&gt;
Low frequencies ---   -3.5606   -3.5606   -0.0089   -0.0043   -0.0043   10.0905&lt;br /&gt;
Low frequencies ---  413.9582  413.9582  621.1416&lt;br /&gt;
&amp;lt;/pre&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;jmol of C&amp;lt;sub&amp;gt;6&amp;lt;/sub&amp;gt;H&amp;lt;sub&amp;gt;6&amp;lt;/sub&amp;gt;&#039;&#039;&#039;&lt;br /&gt;
&amp;lt;jmol&amp;gt;&amp;lt;jmolApplet&amp;gt;&lt;br /&gt;
  &amp;lt;title&amp;gt;optimised Benzene&amp;lt;/title&amp;gt;&lt;br /&gt;
  &amp;lt;color&amp;gt;black&amp;lt;/color&amp;gt;&lt;br /&gt;
  &amp;lt;size&amp;gt;200&amp;lt;/size&amp;gt;&lt;br /&gt;
  &amp;lt;uploadedFileContents&amp;gt;HYC116_C6H6_FREQ.LOG&amp;lt;/uploadedFileContents&amp;gt;&lt;br /&gt;
&amp;lt;/jmolApplet&amp;gt;&amp;lt;/jmol&amp;gt;&lt;br /&gt;
&lt;br /&gt;
===Borazine===&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;Calculation type&amp;lt;/b&amp;gt;: Optimisation&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;Calculation Method&amp;lt;/b&amp;gt;: B3LYP&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;Basis set&amp;lt;/b&amp;gt;: 6-31G(d,p) &lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Summary table&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
[[file:Hyc116_borazine_summarytable.png]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Items table&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;pre&amp;gt;&lt;br /&gt;
Item               Value     Threshold  Converged?&lt;br /&gt;
 Maximum Force            0.000085     0.000450     YES&lt;br /&gt;
 RMS     Force            0.000033     0.000300     YES&lt;br /&gt;
 Maximum Displacement     0.000250     0.001800     YES&lt;br /&gt;
 RMS     Displacement     0.000074     0.001200     YES&lt;br /&gt;
&amp;lt;/pre&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Frequency log file&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
[[Media:HYC116_BORAZINE_FREQ.LOG]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Frequencies&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;pre&amp;gt;&lt;br /&gt;
Low frequencies ---  -12.6626  -12.6626   -8.9272   -0.0211   -0.0104   -0.0104&lt;br /&gt;
Low frequencies ---  289.1112  289.1112  403.8613&lt;br /&gt;
&amp;lt;/pre&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;jmol of Borazine&#039;&#039;&#039;&lt;br /&gt;
&amp;lt;jmol&amp;gt;&amp;lt;jmolApplet&amp;gt;&lt;br /&gt;
  &amp;lt;title&amp;gt;optimised Borazine&amp;lt;/title&amp;gt;&lt;br /&gt;
  &amp;lt;color&amp;gt;black&amp;lt;/color&amp;gt;&lt;br /&gt;
  &amp;lt;size&amp;gt;200&amp;lt;/size&amp;gt;&lt;br /&gt;
  &amp;lt;uploadedFileContents&amp;gt;HYC116_BORAZINE_FREQ.LOG&amp;lt;/uploadedFileContents&amp;gt;&lt;br /&gt;
&amp;lt;/jmolApplet&amp;gt;&amp;lt;/jmol&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
===Charge distribution===&lt;br /&gt;
&lt;br /&gt;
An NBO charge analysis was carried out on both the optimised benzene and borazine. Visualisations of the charge distribution are shown in the table below, with the colour range going from -1.102 to 1.102 for both molecule. This large scale was chosen as it allows direct comparison of the charge on any atoms in these two molecules and shows the relative magnitude of charges on all these atoms. Negative charges are shown in red, and positive charges are shown in green. A neutral charge is displayed in black, so the smaller a charge is (positive or negative), the darker its colour representation is. Larger charges are shown in brighter colours. The charges are also displayed on the atoms as numbers with a neutral charge being zero. Negative charges are shown as negative number and positive charges are shown as positive numbers. &lt;br /&gt;
&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot;&lt;br /&gt;
!&lt;br /&gt;
!Benzene&lt;br /&gt;
!Borazine&lt;br /&gt;
|-&lt;br /&gt;
!Visualisation of charge distribution&lt;br /&gt;
|[[File:Hyc116_benzene_charge_distribution1.png|500x500px|thumb|centre|Charge distribution of Benzene visualisation]]&lt;br /&gt;
|[[File:Hyc116_borazine_charge_distribution1.png|500x500px|thumb|centre|Charge distribution of Borazine visualisation]]&lt;br /&gt;
|-&lt;br /&gt;
!Charge &lt;br /&gt;
|Carbon: -0.239&lt;br /&gt;
&lt;br /&gt;
Hydrogen: 0.239&lt;br /&gt;
|Nitrogen: -1.102 &lt;br /&gt;
&lt;br /&gt;
Boron: 0.747&lt;br /&gt;
&lt;br /&gt;
Hydrogen (bonded to N): 0.432&lt;br /&gt;
&lt;br /&gt;
Hydrogen (bonded to B): -0.077&lt;br /&gt;
|-&lt;br /&gt;
!Discussion&lt;br /&gt;
|From the visualisation, it is shown that there is a slightly negative charge on the carbon atoms, and a positive charge of the same magnitude on the hydrogen atoms. All the carbon atoms have the same charge as they are in identical environments. The same applies to all the hydrogen atoms. This is due to the highly symmetrical structure of benzene. Since the same colour scale was used for both benzene and borazine, and the charges are much smaller in magnitude on atoms in benzene than atoms on borazine, the colours on the charge distribution visualisation is much darker. &lt;br /&gt;
|From the colours displayed on the charge distribution visualisation as well as the charge values, it is shown that nitrogen has a relatively large negative charge, while boron has a positive charge. This is due to the difference in electrogenativity between these atoms: nitrogen atoms are more electronegative than boron and tends to attract electrons towards themselves. It is worth noting that the hydrogen atoms do not all have the same charge. The hydrogen atoms bonded to boron have a slightly negative charge, and the ones bonded to nitrogen have a small positive charge. &lt;br /&gt;
&lt;br /&gt;
The fact that the same colour scale was used for both molecules comes in helpful here. It allows the charges on atoms to be compared directly. For example, just from looking at the colours, one can tell that or example, even though both carbon and nitrogen are electronegative, nitrogen is much more electronegative, which is quantitatively shown by Pauling&#039;s electronegativity scale.&amp;lt;ref&amp;gt;http://www.tutor-homework.com/Chemistry_Help/electronegativity_table/electronegativity.html (Date accessed: 24.0502018&amp;lt;/ref&amp;gt;&lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
===Comparative MOs of Benzene and Borazine===&lt;br /&gt;
&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot;&lt;br /&gt;
!&lt;br /&gt;
!Benzene&lt;br /&gt;
!Borazine&lt;br /&gt;
!Comparison and Discussion&lt;br /&gt;
|-&lt;br /&gt;
!1st comparative pair&lt;br /&gt;
|[[File:Hyc116_benzene_1st_MO_pair_7.png|200x200px|centre]]&lt;br /&gt;
|[[File:Hyc116_borazine_1st_MO_pair_level9.png|200x200px|centre]]&lt;br /&gt;
|MO 9 of both benzene and borazine are comparable. They both show delocalised molecular orbital with an overall bonding character. There is a nodal plane across the molecular orbitals for both benzene and borazine. For benzene, there is contribution from all the carbon and hydrogen s orbitals. Moreover, the molecular orbitals are symmetric to their counterpart of opposite phase. That is not the case for borazine; they are less symmetric in borazine. Nitrogen atoms are more electronegative than boron atoms and pull electron density towards themselves, resulting in a larger MO. There is contribution from all the boron and nitrogen s orbitals, and three of the hydrogen s orbitals, though not all of them. &lt;br /&gt;
|-&lt;br /&gt;
!2nd comparative pair&lt;br /&gt;
|[[File:Hyc116_benzene_2nd_MO_pair_10.png|200x200px|centre]]&lt;br /&gt;
|[[File:Hyc116_borazine_2nd_MO_pair_level11.png|200x200px|centre]]&lt;br /&gt;
|&lt;br /&gt;
|-&lt;br /&gt;
!3rd comparative pair&lt;br /&gt;
|[[File:Hyc116_benzene_3rd_MO_pair_21.png|200x200px|centre]]&lt;br /&gt;
|[[File:Hyc116_borazine_3rd_MO_pair_level21.png|200x200px|centre]]&lt;br /&gt;
|&lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
===Aromaticity: some theories===&lt;br /&gt;
&lt;br /&gt;
==Reference==&lt;/div&gt;</summary>
		<author><name>Hyc116</name></author>
	</entry>
	<entry>
		<id>https://chemwiki.ch.ic.ac.uk/index.php?title=MO_hyc116&amp;diff=730125</id>
		<title>MO hyc116</title>
		<link rel="alternate" type="text/html" href="https://chemwiki.ch.ic.ac.uk/index.php?title=MO_hyc116&amp;diff=730125"/>
		<updated>2018-05-24T17:22:50Z</updated>

		<summary type="html">&lt;p&gt;Hyc116: /* Charge distribution */&lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;==BH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;==&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;Calculation type&amp;lt;/b&amp;gt;: Optimisation&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;Calculation Method&amp;lt;/b&amp;gt;: B3LYP&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;Basis set&amp;lt;/b&amp;gt;: 6-31G(d,p) &lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Summary table&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
[[file:Hyc116_bh3_631g_opt_summarytable.png]]&lt;br /&gt;
&lt;br /&gt;
The above summary table was obtained after the 2nd optimisation of BH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt; (after the initial optimisation using the 3-21G basis set). Notice how the symmetry is incorrect and shown as Cs. This is because the symmetry was manually broken at the beginning by changing the bond length of B-H bonds. The point group was manually adjusted and the molecule was optimised again before the frequency analysis and the new summary table is attached below.&lt;br /&gt;
&lt;br /&gt;
[[file:Hyc116_bh3_correctsummarytable.png]]&lt;br /&gt;
&lt;br /&gt;
The above summary table was obtained from the optimisation after adjusting the symmetry. The point shown in this summary table is D&amp;lt;sub&amp;gt;3h&amp;lt;/sub&amp;gt;, which is the correct for BH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;. &lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Items table&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
Below is the items table taken from the optimisation with the correct point group.&lt;br /&gt;
&lt;br /&gt;
&amp;lt;pre&amp;gt;&lt;br /&gt;
Item               Value     Threshold  Converged?&lt;br /&gt;
 Maximum Force            0.000015     0.000450     YES&lt;br /&gt;
 RMS     Force            0.000010     0.000300     YES&lt;br /&gt;
 Maximum Displacement     0.000058     0.001800     YES&lt;br /&gt;
 RMS     Displacement     0.000038     0.001200     YES&lt;br /&gt;
&amp;lt;/pre&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Frequency log file&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
[[Media:HYC116 BH3 FREQ.LOG]] &lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Frequencies&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;pre&amp;gt;&lt;br /&gt;
Low frequencies ---  -10.3498   -3.4492   -1.2454   -0.0055    0.4779    3.2165&lt;br /&gt;
Low frequencies --- 1162.9519 1213.1527 1213.1554&lt;br /&gt;
&amp;lt;/pre&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;jmol of BH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;&#039;&#039;&#039;&lt;br /&gt;
&amp;lt;jmol&amp;gt;&amp;lt;jmolApplet&amp;gt;&lt;br /&gt;
  &amp;lt;title&amp;gt;optimised BH3&amp;lt;/title&amp;gt;&lt;br /&gt;
  &amp;lt;color&amp;gt;black&amp;lt;/color&amp;gt;&lt;br /&gt;
  &amp;lt;size&amp;gt;200&amp;lt;/size&amp;gt;&lt;br /&gt;
  &amp;lt;uploadedFileContents&amp;gt;HYC116_BH3_FREQ.LOG&amp;lt;/uploadedFileContents&amp;gt;&lt;br /&gt;
&amp;lt;/jmolApplet&amp;gt;&amp;lt;/jmol&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
===Vibrational spectrum===&lt;br /&gt;
&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot;&lt;br /&gt;
!wavenumber (cm&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;)&lt;br /&gt;
!Intensity (arbitrary units)&lt;br /&gt;
!symmetry&lt;br /&gt;
!IR active?&lt;br /&gt;
!type&lt;br /&gt;
|-&lt;br /&gt;
|1163&lt;br /&gt;
|93&lt;br /&gt;
|A&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;&#039; &#039;&lt;br /&gt;
|Yes&lt;br /&gt;
|Out of plane bend&lt;br /&gt;
|-&lt;br /&gt;
|1213&lt;br /&gt;
|14&lt;br /&gt;
|E&#039;&lt;br /&gt;
|Very slight&lt;br /&gt;
|Bend&lt;br /&gt;
|-&lt;br /&gt;
|1213&lt;br /&gt;
|14&lt;br /&gt;
|E&#039;&lt;br /&gt;
|Very slight&lt;br /&gt;
|Bend&lt;br /&gt;
|-&lt;br /&gt;
|2582&lt;br /&gt;
|0&lt;br /&gt;
|A&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;&#039;&lt;br /&gt;
|No&lt;br /&gt;
|Symmetric stretch&lt;br /&gt;
|-&lt;br /&gt;
|2716&lt;br /&gt;
|126&lt;br /&gt;
|E&#039;&lt;br /&gt;
|Yes&lt;br /&gt;
|Asymmetric stretch&lt;br /&gt;
|-&lt;br /&gt;
|2716&lt;br /&gt;
|126&lt;br /&gt;
|E&#039;&lt;br /&gt;
|Yes&lt;br /&gt;
|Asymmetric stretch&lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;IR spectrum&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
[[file:Hyc116_ir_bh3.png|400*600]]&lt;br /&gt;
&lt;br /&gt;
There are only three peaks on the IR spectrum of BH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;, despite that there are 6 vibrational modes for the molecule. As shown in the table above, the symmetric stretching mode with A1 symmetry at 2582 cm&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt; is not IR active; naturally, that vibrational mode doesn’t give a peak on the IR spectrum. As shown from the table, two pairs of vibrational modes, the bond angle deformation/bend at 1213 cm&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt; and the asymmetric bond stretch at 2716 cm&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;, are degenerate with the symmetry label E. This means that they have the same energy, and hence give the same wavenumber on the IR spectrum. Each pair of degenerate vibrational modes give rise to one peak. This leaves three peaks, as confirmed by the IR spectrum above.&lt;br /&gt;
&lt;br /&gt;
===Molecular orbitals of BH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;===&lt;br /&gt;
&lt;br /&gt;
[[file:hyc116_bh3_MO_diagram.png]]&lt;br /&gt;
&lt;br /&gt;
The above molecular orbital diagram was taken from Dr Patricia Hunt&#039;s &amp;lt;i&amp;gt;Lecture 4 Tutorial Problem Model Answers&amp;lt;/i&amp;gt;. &amp;lt;ref&amp;gt;P. Hunt, &amp;quot;Lecture 4 Tutorial Problem Model Answers&amp;quot;, 2 (2018)&amp;lt;/ref&amp;gt;. Diagrams of the &amp;quot;real&amp;quot; MOs were obtained from Gaussian.&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
There is no significant difference between the LCAO MOs and the real ones. Features such as orbital phases are shown clearly on both the LCAO MOs and the real MOs, illustrating the bonding/anti-bonding characters of the molecular orbitals. This suggests that the the qualitative MO theory is highly accurate and useful when studying the molecular orbitals of molecules.&lt;br /&gt;
&lt;br /&gt;
==Associated energies: ammonium borane==&lt;br /&gt;
&lt;br /&gt;
===NH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;===&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;Calculation type&amp;lt;/b&amp;gt;: Optimisation&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;Calculation Method&amp;lt;/b&amp;gt;: B3LYP&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;Basis set&amp;lt;/b&amp;gt;: 6-31G(d,p) &lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Summary table&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
[[file:Hyc116_nh3_631g_summarytable.png]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Items table&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;pre&amp;gt;&lt;br /&gt;
Item               Value     Threshold  Converged?&lt;br /&gt;
 Maximum Force            0.000006     0.000450     YES&lt;br /&gt;
 RMS     Force            0.000004     0.000300     YES&lt;br /&gt;
 Maximum Displacement     0.000012     0.001800     YES&lt;br /&gt;
 RMS     Displacement     0.000008     0.001200     YES&lt;br /&gt;
&amp;lt;/pre&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Frequency log file&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
[[Media:HYC116_NH3_FREQ.LOG]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Frequencies&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;pre&amp;gt;&lt;br /&gt;
Low frequencies ---   -8.5646   -8.5588   -0.0047    0.0454    0.1784   26.4183&lt;br /&gt;
Low frequencies --- 1089.7603 1694.1865 1694.1865&lt;br /&gt;
&amp;lt;/pre&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;jmol of NH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;&#039;&#039;&#039;&lt;br /&gt;
&amp;lt;jmol&amp;gt;&amp;lt;jmolApplet&amp;gt;&lt;br /&gt;
  &amp;lt;title&amp;gt;optimised NH3&amp;lt;/title&amp;gt;&lt;br /&gt;
  &amp;lt;color&amp;gt;black&amp;lt;/color&amp;gt;&lt;br /&gt;
  &amp;lt;size&amp;gt;200&amp;lt;/size&amp;gt;&lt;br /&gt;
  &amp;lt;uploadedFileContents&amp;gt;HYC116_NH3_FREQ.LOG&amp;lt;/uploadedFileContents&amp;gt;&lt;br /&gt;
&amp;lt;/jmolApplet&amp;gt;&amp;lt;/jmol&amp;gt;&lt;br /&gt;
&lt;br /&gt;
===NH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;BH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;===&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;Calculation type&amp;lt;/b&amp;gt;: Optimisation&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;Calculation Method&amp;lt;/b&amp;gt;: B3LYP&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;Basis set&amp;lt;/b&amp;gt;: 6-31G(d,p) &lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Summary table&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
[[file:Hyc116_nh3bh3_631g_summarytable.png]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Items table&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;pre&amp;gt;&lt;br /&gt;
Item               Value     Threshold  Converged?&lt;br /&gt;
 Maximum Force            0.000123     0.000450     YES&lt;br /&gt;
 RMS     Force            0.000058     0.000300     YES&lt;br /&gt;
 Maximum Displacement     0.000515     0.001800     YES&lt;br /&gt;
 RMS     Displacement     0.000296     0.001200     YES&lt;br /&gt;
&amp;lt;/pre&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Frequency log file&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
[[Media:HYC116_NH3BH3_FREQ.LOG]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Frequencies&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;pre&amp;gt;&lt;br /&gt;
Low frequencies ---   -0.0014   -0.0011   -0.0006    6.9624   20.4518   43.5542&lt;br /&gt;
Low frequencies ---  266.4530  632.2458  639.0504&lt;br /&gt;
&amp;lt;/pre&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;jmol of NH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;BH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;&#039;&#039;&#039;&lt;br /&gt;
&amp;lt;jmol&amp;gt;&amp;lt;jmolApplet&amp;gt;&lt;br /&gt;
  &amp;lt;title&amp;gt;optimised NH3BH3&amp;lt;/title&amp;gt;&lt;br /&gt;
  &amp;lt;color&amp;gt;black&amp;lt;/color&amp;gt;&lt;br /&gt;
  &amp;lt;size&amp;gt;200&amp;lt;/size&amp;gt;&lt;br /&gt;
  &amp;lt;uploadedFileContents&amp;gt;HYC116_NH3BH3_FREQ.LOG&amp;lt;/uploadedFileContents&amp;gt;&lt;br /&gt;
&amp;lt;/jmolApplet&amp;gt;&amp;lt;/jmol&amp;gt;&lt;br /&gt;
&lt;br /&gt;
===Association energy===&lt;br /&gt;
&lt;br /&gt;
E(BH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;) (using the optimisation with the correct symmetry) = -26.61532363 a.u. = &amp;lt;b&amp;gt;-26.61532 a.u. (5 d.p.)&amp;lt;/b&amp;gt;&lt;br /&gt;
&lt;br /&gt;
E(NH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;) = -56.55776873 a.u. = &amp;lt;b&amp;gt;-56.55777 a.u. (5 d.p.)&amp;lt;/b&amp;gt;&lt;br /&gt;
&lt;br /&gt;
E(NH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;BH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;) = -83.22468893 a.u. = &amp;lt;b&amp;gt;-83.22469 a.u. (5 d.p.)&amp;lt;/b&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
Carrying out calculations using numbers which has already been rounded up can possibly result in errors in the last digit. Hence, here the calculations were carried out using the numbers provided from the optimisations (i.e. with more decimal places than necessary); the answer was then rounded up to the desired accuracy. &lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
ΔE = E(NH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;BH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;)-[E(NH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;)+E(BH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;)]&lt;br /&gt;
&lt;br /&gt;
ΔE = -83.22468893 - (-56.55776873 + -26.61532363) = -0.05159657 a.u. &lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;ΔE = -0.05160 a.u. (5 d.p.)&amp;lt;/b&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Converting energy from a.u. to kJ/mol&#039;&#039;&#039;&lt;br /&gt;
An atomic unit for energy is Hartree, which is equal to 2625.5 kJ/mol. &amp;lt;ref&amp;gt;https://cccbdb.nist.gov/hartree.asp (Accessed: 22.05.2018)&amp;lt;/ref&amp;gt;&lt;br /&gt;
&lt;br /&gt;
So ΔE in kJ/mol = -0.05159657 * 2625.5 = -135.466794535 kJ/mol&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;ΔE = -135 kJ/mol (nearest integer)&amp;lt;/b&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
The energy difference calculated above comes from the formation of the B-N dative bond. It is a relatively weak bond. According to a bond energy data sheet provided by the University of California, &amp;lt;ref&amp;gt;https://labs.chem.ucsb.edu/zakarian/armen/11---bonddissociationenergy.pdf (Accessed on 24.05.2018)&amp;lt;/ref&amp;gt; the bond energy of the C-C bond of an ethane molecule is 368 kJ/mol. This is a fair comparison to the NH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;BH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt; molecule as the two molecules have the same structure, only with the carbon atoms on ethane swapped for Boron and Nitrogen in NH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;BH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;&lt;br /&gt;
&lt;br /&gt;
==Using a mixture of basis-sets and pseudo-potentials==&lt;br /&gt;
&lt;br /&gt;
===BBr&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;===&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;Calculation type&amp;lt;/b&amp;gt;: Optimisation&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;Calculation Method&amp;lt;/b&amp;gt;: B3LYP&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;Basis set&amp;lt;/b&amp;gt;: Boron: 6-31G(d,p) ; Br: LANL2DZ&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Summary table&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
[[file:Hyc116_bbr3_opt_summarytable.png]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Items table&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;pre&amp;gt;&lt;br /&gt;
Item               Value     Threshold  Converged?&lt;br /&gt;
 Maximum Force            0.000008     0.000450     YES&lt;br /&gt;
 RMS     Force            0.000005     0.000300     YES&lt;br /&gt;
 Maximum Displacement     0.000036     0.001800     YES&lt;br /&gt;
 RMS     Displacement     0.000023     0.001200     YES&lt;br /&gt;
&amp;lt;/pre&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Frequency log file&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
[[Media:Hyc116_bbr3_freq.log]]&lt;br /&gt;
&lt;br /&gt;
Attached above is the frequency file saved onto the computer from the SCAN server portal. The frequency file was also published on the chemistry database DSpace. {{DOI|10042/202442}}&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Frequencies&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;pre&amp;gt;&lt;br /&gt;
Low frequencies ---   -0.0137   -0.0064   -0.0046    2.4315    2.4315    4.8421&lt;br /&gt;
Low frequencies ---  155.9631  155.9651  267.7052&lt;br /&gt;
&amp;lt;/pre&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;jmol of BBr&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;&#039;&#039;&#039;&lt;br /&gt;
&amp;lt;jmol&amp;gt;&amp;lt;jmolApplet&amp;gt;&lt;br /&gt;
  &amp;lt;title&amp;gt;optimised BBr3&amp;lt;/title&amp;gt;&lt;br /&gt;
  &amp;lt;color&amp;gt;black&amp;lt;/color&amp;gt;&lt;br /&gt;
  &amp;lt;size&amp;gt;200&amp;lt;/size&amp;gt;&lt;br /&gt;
  &amp;lt;uploadedFileContents&amp;gt;Hyc116_bbr3_freq.log&amp;lt;/uploadedFileContents&amp;gt;&lt;br /&gt;
&amp;lt;/jmolApplet&amp;gt;&amp;lt;/jmol&amp;gt;&lt;br /&gt;
&lt;br /&gt;
==Aromaticity==&lt;br /&gt;
&lt;br /&gt;
===Benzene===&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;Calculation type&amp;lt;/b&amp;gt;: Optimisation&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;Calculation Method&amp;lt;/b&amp;gt;: B3LYP&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;Basis set&amp;lt;/b&amp;gt;: 6-31G(d,p) &lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Summary table&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
[[file:Hyc116_c6h6_summarytable.png]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Items table&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;pre&amp;gt;&lt;br /&gt;
Item               Value     Threshold  Converged?&lt;br /&gt;
 Maximum Force            0.000193     0.000450     YES&lt;br /&gt;
 RMS     Force            0.000079     0.000300     YES&lt;br /&gt;
 Maximum Displacement     0.000830     0.001800     YES&lt;br /&gt;
 RMS     Displacement     0.000294     0.001200     YES&lt;br /&gt;
&amp;lt;/pre&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Frequency log file&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
[[Media:HYC116_C6H6_FREQ.LOG]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Frequencies&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;pre&amp;gt;&lt;br /&gt;
Low frequencies ---   -3.5606   -3.5606   -0.0089   -0.0043   -0.0043   10.0905&lt;br /&gt;
Low frequencies ---  413.9582  413.9582  621.1416&lt;br /&gt;
&amp;lt;/pre&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;jmol of C&amp;lt;sub&amp;gt;6&amp;lt;/sub&amp;gt;H&amp;lt;sub&amp;gt;6&amp;lt;/sub&amp;gt;&#039;&#039;&#039;&lt;br /&gt;
&amp;lt;jmol&amp;gt;&amp;lt;jmolApplet&amp;gt;&lt;br /&gt;
  &amp;lt;title&amp;gt;optimised Benzene&amp;lt;/title&amp;gt;&lt;br /&gt;
  &amp;lt;color&amp;gt;black&amp;lt;/color&amp;gt;&lt;br /&gt;
  &amp;lt;size&amp;gt;200&amp;lt;/size&amp;gt;&lt;br /&gt;
  &amp;lt;uploadedFileContents&amp;gt;HYC116_C6H6_FREQ.LOG&amp;lt;/uploadedFileContents&amp;gt;&lt;br /&gt;
&amp;lt;/jmolApplet&amp;gt;&amp;lt;/jmol&amp;gt;&lt;br /&gt;
&lt;br /&gt;
===Borazine===&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;Calculation type&amp;lt;/b&amp;gt;: Optimisation&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;Calculation Method&amp;lt;/b&amp;gt;: B3LYP&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;Basis set&amp;lt;/b&amp;gt;: 6-31G(d,p) &lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Summary table&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
[[file:Hyc116_borazine_summarytable.png]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Items table&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;pre&amp;gt;&lt;br /&gt;
Item               Value     Threshold  Converged?&lt;br /&gt;
 Maximum Force            0.000085     0.000450     YES&lt;br /&gt;
 RMS     Force            0.000033     0.000300     YES&lt;br /&gt;
 Maximum Displacement     0.000250     0.001800     YES&lt;br /&gt;
 RMS     Displacement     0.000074     0.001200     YES&lt;br /&gt;
&amp;lt;/pre&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Frequency log file&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
[[Media:HYC116_BORAZINE_FREQ.LOG]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Frequencies&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;pre&amp;gt;&lt;br /&gt;
Low frequencies ---  -12.6626  -12.6626   -8.9272   -0.0211   -0.0104   -0.0104&lt;br /&gt;
Low frequencies ---  289.1112  289.1112  403.8613&lt;br /&gt;
&amp;lt;/pre&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;jmol of Borazine&#039;&#039;&#039;&lt;br /&gt;
&amp;lt;jmol&amp;gt;&amp;lt;jmolApplet&amp;gt;&lt;br /&gt;
  &amp;lt;title&amp;gt;optimised Borazine&amp;lt;/title&amp;gt;&lt;br /&gt;
  &amp;lt;color&amp;gt;black&amp;lt;/color&amp;gt;&lt;br /&gt;
  &amp;lt;size&amp;gt;200&amp;lt;/size&amp;gt;&lt;br /&gt;
  &amp;lt;uploadedFileContents&amp;gt;HYC116_BORAZINE_FREQ.LOG&amp;lt;/uploadedFileContents&amp;gt;&lt;br /&gt;
&amp;lt;/jmolApplet&amp;gt;&amp;lt;/jmol&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
===Charge distribution===&lt;br /&gt;
&lt;br /&gt;
An NBO charge analysis was carried out on both the optimised benzene and borazine. Visualisations of the charge distribution are shown in the table below, with the colour range going from -1.102 to 1.102 for both molecule. This large scale was chosen as it allows direct comparison of the charge on any atoms in these two molecules and shows the relative magnitude of charges on all these atoms. Negative charges are shown in red, and positive charges are shown in green. A neutral charge is displayed in black, so the smaller a charge is (positive or negative), the darker its colour representation is. Larger charges are shown in brighter colours. The charges are also displayed on the atoms as numbers with a neutral charge being zero. Negative charges are shown as negative number and positive charges are shown as positive numbers. &lt;br /&gt;
&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot;&lt;br /&gt;
!&lt;br /&gt;
!Benzene&lt;br /&gt;
!Borazine&lt;br /&gt;
|-&lt;br /&gt;
!Visualisation of charge distribution&lt;br /&gt;
|[[File:Hyc116_benzene_charge_distribution1.png|500x500px|thumb|centre|Charge distribution of Benzene visualisation]]&lt;br /&gt;
|[[File:Hyc116_borazine_charge_distribution1.png|500x500px|thumb|centre|Charge distribution of Borazine visualisation]]&lt;br /&gt;
|-&lt;br /&gt;
!Charge &lt;br /&gt;
|Carbon: -0.239&lt;br /&gt;
&lt;br /&gt;
Hydrogen: 0.239&lt;br /&gt;
|Nitrogen: -1.102 &lt;br /&gt;
&lt;br /&gt;
Boron: 0.747&lt;br /&gt;
&lt;br /&gt;
Hydrogen (bonded to N): 0.432&lt;br /&gt;
&lt;br /&gt;
Hydrogen (bonded to B): -0.077&lt;br /&gt;
|-&lt;br /&gt;
!Discussion&lt;br /&gt;
|From the visualisation, it is shown that there is a slightly negative charge on the carbon atoms, and a positive charge of the same magnitude on the hydrogen atoms. All the carbon atoms have the same charge as they are in identical environments. The same applies to all the hydrogen atoms. This is due to the highly symmetrical structure of benzene. Since the same colour scale was used for both benzene and borazine, and the charges are much smaller in magnitude on atoms in benzene than atoms on borazine, the colours on the charge distribution visualisation is much darker. &lt;br /&gt;
|From the colours displayed on the charge distribution visualisation as well as the charge values, it is shown that nitrogen has a relatively large negative charge, while boron has a positive charge. This is due to the difference in electrogenativity between these atoms: nitrogen atoms are more electronegative than boron and tends to attract electrons towards themselves. It is worth noting that the hydrogen atoms do not all have the same charge. The hydrogen atoms bonded to boron have a slightly negative charge, and the ones bonded to nitrogen have a small positive charge. &lt;br /&gt;
&lt;br /&gt;
The fact that the same colour scale was used for both molecules comes in helpful here. It allows the charges on atoms to be compared directly. For example, just from looking at the colours, one can tell that or example, even though both carbon and nitrogen are electronegative, nitrogen is much more electronegative, which is quantitatively shown by Pauling&#039;s electronegativity scale.&amp;lt;ref&amp;gt;http://www.tutor-homework.com/Chemistry_Help/electronegativity_table/electronegativity.html (Date accessed: 24.0502018&amp;lt;/ref&amp;gt;&lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
===Comparative MOs of Benzene and Borazine===&lt;br /&gt;
&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot;&lt;br /&gt;
!&lt;br /&gt;
!Benzene&lt;br /&gt;
!Borazine&lt;br /&gt;
!Comparison and Discussion&lt;br /&gt;
|-&lt;br /&gt;
!1st comparative pair&lt;br /&gt;
|[[File:Hyc116_benzene_1st_MO_pair_7.png|200x200px|centre]]&lt;br /&gt;
|[[File:Hyc116_borazine_1st_MO_pair_level9.png|200x200px|centre]]&lt;br /&gt;
|MO 9 of both benzene and borazine are comparable. They both show delocalised molecular orbital with an overall bonding character. There is a nodal plane across the molecular orbitals for both benzene and borazine. For benzene, there is contribution from all the carbon and hydrogen s orbitals. Moreover, the molecular orbitals are symmetric to their counterpart of opposite phase. That is not the case for borazine; they are less symmetric in borazine. Nitrogen atoms are more electronegative than boron atoms and pull electron density towards themselves, resulting in a larger MO. There is contribution from all the boron and nitrogen s orbitals, and three of the hydrogen s orbitals, though not all of them. &lt;br /&gt;
|-&lt;br /&gt;
!2nd comparative pair&lt;br /&gt;
|[[File:Hyc116_benzene_2nd_MO_pair_10.png|200x200px|centre]]&lt;br /&gt;
|[[File:Hyc116_borazine_2nd_MO_pair_level11.png|200x200px|centre]]&lt;br /&gt;
|&lt;br /&gt;
|-&lt;br /&gt;
!3rd comparative pair&lt;br /&gt;
|[[File:Hyc116_benzene_3rd_MO_pair_21.png|200x200px|centre]]&lt;br /&gt;
|[[File:Hyc116_borazine_3rd_MO_pair_level21.png|200x200px|centre]]&lt;br /&gt;
|&lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
===Aromaticity: some theories===&lt;br /&gt;
&lt;br /&gt;
==Reference==&lt;/div&gt;</summary>
		<author><name>Hyc116</name></author>
	</entry>
	<entry>
		<id>https://chemwiki.ch.ic.ac.uk/index.php?title=MO_hyc116&amp;diff=730077</id>
		<title>MO hyc116</title>
		<link rel="alternate" type="text/html" href="https://chemwiki.ch.ic.ac.uk/index.php?title=MO_hyc116&amp;diff=730077"/>
		<updated>2018-05-24T17:03:40Z</updated>

		<summary type="html">&lt;p&gt;Hyc116: /* Comparative MOs of Benzene and Borazine */&lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;==BH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;==&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;Calculation type&amp;lt;/b&amp;gt;: Optimisation&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;Calculation Method&amp;lt;/b&amp;gt;: B3LYP&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;Basis set&amp;lt;/b&amp;gt;: 6-31G(d,p) &lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Summary table&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
[[file:Hyc116_bh3_631g_opt_summarytable.png]]&lt;br /&gt;
&lt;br /&gt;
The above summary table was obtained after the 2nd optimisation of BH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt; (after the initial optimisation using the 3-21G basis set). Notice how the symmetry is incorrect and shown as Cs. This is because the symmetry was manually broken at the beginning by changing the bond length of B-H bonds. The point group was manually adjusted and the molecule was optimised again before the frequency analysis and the new summary table is attached below.&lt;br /&gt;
&lt;br /&gt;
[[file:Hyc116_bh3_correctsummarytable.png]]&lt;br /&gt;
&lt;br /&gt;
The above summary table was obtained from the optimisation after adjusting the symmetry. The point shown in this summary table is D&amp;lt;sub&amp;gt;3h&amp;lt;/sub&amp;gt;, which is the correct for BH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;. &lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Items table&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
Below is the items table taken from the optimisation with the correct point group.&lt;br /&gt;
&lt;br /&gt;
&amp;lt;pre&amp;gt;&lt;br /&gt;
Item               Value     Threshold  Converged?&lt;br /&gt;
 Maximum Force            0.000015     0.000450     YES&lt;br /&gt;
 RMS     Force            0.000010     0.000300     YES&lt;br /&gt;
 Maximum Displacement     0.000058     0.001800     YES&lt;br /&gt;
 RMS     Displacement     0.000038     0.001200     YES&lt;br /&gt;
&amp;lt;/pre&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Frequency log file&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
[[Media:HYC116 BH3 FREQ.LOG]] &lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Frequencies&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;pre&amp;gt;&lt;br /&gt;
Low frequencies ---  -10.3498   -3.4492   -1.2454   -0.0055    0.4779    3.2165&lt;br /&gt;
Low frequencies --- 1162.9519 1213.1527 1213.1554&lt;br /&gt;
&amp;lt;/pre&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;jmol of BH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;&#039;&#039;&#039;&lt;br /&gt;
&amp;lt;jmol&amp;gt;&amp;lt;jmolApplet&amp;gt;&lt;br /&gt;
  &amp;lt;title&amp;gt;optimised BH3&amp;lt;/title&amp;gt;&lt;br /&gt;
  &amp;lt;color&amp;gt;black&amp;lt;/color&amp;gt;&lt;br /&gt;
  &amp;lt;size&amp;gt;200&amp;lt;/size&amp;gt;&lt;br /&gt;
  &amp;lt;uploadedFileContents&amp;gt;HYC116_BH3_FREQ.LOG&amp;lt;/uploadedFileContents&amp;gt;&lt;br /&gt;
&amp;lt;/jmolApplet&amp;gt;&amp;lt;/jmol&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
===Vibrational spectrum===&lt;br /&gt;
&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot;&lt;br /&gt;
!wavenumber (cm&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;)&lt;br /&gt;
!Intensity (arbitrary units)&lt;br /&gt;
!symmetry&lt;br /&gt;
!IR active?&lt;br /&gt;
!type&lt;br /&gt;
|-&lt;br /&gt;
|1163&lt;br /&gt;
|93&lt;br /&gt;
|A&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;&#039; &#039;&lt;br /&gt;
|Yes&lt;br /&gt;
|Out of plane bend&lt;br /&gt;
|-&lt;br /&gt;
|1213&lt;br /&gt;
|14&lt;br /&gt;
|E&#039;&lt;br /&gt;
|Very slight&lt;br /&gt;
|Bend&lt;br /&gt;
|-&lt;br /&gt;
|1213&lt;br /&gt;
|14&lt;br /&gt;
|E&#039;&lt;br /&gt;
|Very slight&lt;br /&gt;
|Bend&lt;br /&gt;
|-&lt;br /&gt;
|2582&lt;br /&gt;
|0&lt;br /&gt;
|A&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;&#039;&lt;br /&gt;
|No&lt;br /&gt;
|Symmetric stretch&lt;br /&gt;
|-&lt;br /&gt;
|2716&lt;br /&gt;
|126&lt;br /&gt;
|E&#039;&lt;br /&gt;
|Yes&lt;br /&gt;
|Asymmetric stretch&lt;br /&gt;
|-&lt;br /&gt;
|2716&lt;br /&gt;
|126&lt;br /&gt;
|E&#039;&lt;br /&gt;
|Yes&lt;br /&gt;
|Asymmetric stretch&lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;IR spectrum&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
[[file:Hyc116_ir_bh3.png|400*600]]&lt;br /&gt;
&lt;br /&gt;
There are only three peaks on the IR spectrum of BH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;, despite that there are 6 vibrational modes for the molecule. As shown in the table above, the symmetric stretching mode with A1 symmetry at 2582 cm&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt; is not IR active; naturally, that vibrational mode doesn’t give a peak on the IR spectrum. As shown from the table, two pairs of vibrational modes, the bond angle deformation/bend at 1213 cm&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt; and the asymmetric bond stretch at 2716 cm&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;, are degenerate with the symmetry label E. This means that they have the same energy, and hence give the same wavenumber on the IR spectrum. Each pair of degenerate vibrational modes give rise to one peak. This leaves three peaks, as confirmed by the IR spectrum above.&lt;br /&gt;
&lt;br /&gt;
===Molecular orbitals of BH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;===&lt;br /&gt;
&lt;br /&gt;
[[file:hyc116_bh3_MO_diagram.png]]&lt;br /&gt;
&lt;br /&gt;
The above molecular orbital diagram was taken from Dr Patricia Hunt&#039;s &amp;lt;i&amp;gt;Lecture 4 Tutorial Problem Model Answers&amp;lt;/i&amp;gt;. &amp;lt;ref&amp;gt;P. Hunt, &amp;quot;Lecture 4 Tutorial Problem Model Answers&amp;quot;, 2 (2018)&amp;lt;/ref&amp;gt;. Diagrams of the &amp;quot;real&amp;quot; MOs were obtained from Gaussian.&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
There is no significant difference between the LCAO MOs and the real ones. Features such as orbital phases are shown clearly on both the LCAO MOs and the real MOs, illustrating the bonding/anti-bonding characters of the molecular orbitals. This suggests that the the qualitative MO theory is highly accurate and useful when studying the molecular orbitals of molecules.&lt;br /&gt;
&lt;br /&gt;
==Associated energies: ammonium borane==&lt;br /&gt;
&lt;br /&gt;
===NH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;===&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;Calculation type&amp;lt;/b&amp;gt;: Optimisation&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;Calculation Method&amp;lt;/b&amp;gt;: B3LYP&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;Basis set&amp;lt;/b&amp;gt;: 6-31G(d,p) &lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Summary table&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
[[file:Hyc116_nh3_631g_summarytable.png]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Items table&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;pre&amp;gt;&lt;br /&gt;
Item               Value     Threshold  Converged?&lt;br /&gt;
 Maximum Force            0.000006     0.000450     YES&lt;br /&gt;
 RMS     Force            0.000004     0.000300     YES&lt;br /&gt;
 Maximum Displacement     0.000012     0.001800     YES&lt;br /&gt;
 RMS     Displacement     0.000008     0.001200     YES&lt;br /&gt;
&amp;lt;/pre&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Frequency log file&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
[[Media:HYC116_NH3_FREQ.LOG]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Frequencies&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;pre&amp;gt;&lt;br /&gt;
Low frequencies ---   -8.5646   -8.5588   -0.0047    0.0454    0.1784   26.4183&lt;br /&gt;
Low frequencies --- 1089.7603 1694.1865 1694.1865&lt;br /&gt;
&amp;lt;/pre&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;jmol of NH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;&#039;&#039;&#039;&lt;br /&gt;
&amp;lt;jmol&amp;gt;&amp;lt;jmolApplet&amp;gt;&lt;br /&gt;
  &amp;lt;title&amp;gt;optimised NH3&amp;lt;/title&amp;gt;&lt;br /&gt;
  &amp;lt;color&amp;gt;black&amp;lt;/color&amp;gt;&lt;br /&gt;
  &amp;lt;size&amp;gt;200&amp;lt;/size&amp;gt;&lt;br /&gt;
  &amp;lt;uploadedFileContents&amp;gt;HYC116_NH3_FREQ.LOG&amp;lt;/uploadedFileContents&amp;gt;&lt;br /&gt;
&amp;lt;/jmolApplet&amp;gt;&amp;lt;/jmol&amp;gt;&lt;br /&gt;
&lt;br /&gt;
===NH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;BH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;===&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;Calculation type&amp;lt;/b&amp;gt;: Optimisation&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;Calculation Method&amp;lt;/b&amp;gt;: B3LYP&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;Basis set&amp;lt;/b&amp;gt;: 6-31G(d,p) &lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Summary table&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
[[file:Hyc116_nh3bh3_631g_summarytable.png]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Items table&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;pre&amp;gt;&lt;br /&gt;
Item               Value     Threshold  Converged?&lt;br /&gt;
 Maximum Force            0.000123     0.000450     YES&lt;br /&gt;
 RMS     Force            0.000058     0.000300     YES&lt;br /&gt;
 Maximum Displacement     0.000515     0.001800     YES&lt;br /&gt;
 RMS     Displacement     0.000296     0.001200     YES&lt;br /&gt;
&amp;lt;/pre&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Frequency log file&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
[[Media:HYC116_NH3BH3_FREQ.LOG]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Frequencies&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;pre&amp;gt;&lt;br /&gt;
Low frequencies ---   -0.0014   -0.0011   -0.0006    6.9624   20.4518   43.5542&lt;br /&gt;
Low frequencies ---  266.4530  632.2458  639.0504&lt;br /&gt;
&amp;lt;/pre&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;jmol of NH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;BH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;&#039;&#039;&#039;&lt;br /&gt;
&amp;lt;jmol&amp;gt;&amp;lt;jmolApplet&amp;gt;&lt;br /&gt;
  &amp;lt;title&amp;gt;optimised NH3BH3&amp;lt;/title&amp;gt;&lt;br /&gt;
  &amp;lt;color&amp;gt;black&amp;lt;/color&amp;gt;&lt;br /&gt;
  &amp;lt;size&amp;gt;200&amp;lt;/size&amp;gt;&lt;br /&gt;
  &amp;lt;uploadedFileContents&amp;gt;HYC116_NH3BH3_FREQ.LOG&amp;lt;/uploadedFileContents&amp;gt;&lt;br /&gt;
&amp;lt;/jmolApplet&amp;gt;&amp;lt;/jmol&amp;gt;&lt;br /&gt;
&lt;br /&gt;
===Association energy===&lt;br /&gt;
&lt;br /&gt;
E(BH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;) (using the optimisation with the correct symmetry) = -26.61532363 a.u. = &amp;lt;b&amp;gt;-26.61532 a.u. (5 d.p.)&amp;lt;/b&amp;gt;&lt;br /&gt;
&lt;br /&gt;
E(NH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;) = -56.55776873 a.u. = &amp;lt;b&amp;gt;-56.55777 a.u. (5 d.p.)&amp;lt;/b&amp;gt;&lt;br /&gt;
&lt;br /&gt;
E(NH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;BH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;) = -83.22468893 a.u. = &amp;lt;b&amp;gt;-83.22469 a.u. (5 d.p.)&amp;lt;/b&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
Carrying out calculations using numbers which has already been rounded up can possibly result in errors in the last digit. Hence, here the calculations were carried out using the numbers provided from the optimisations (i.e. with more decimal places than necessary); the answer was then rounded up to the desired accuracy. &lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
ΔE = E(NH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;BH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;)-[E(NH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;)+E(BH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;)]&lt;br /&gt;
&lt;br /&gt;
ΔE = -83.22468893 - (-56.55776873 + -26.61532363) = -0.05159657 a.u. &lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;ΔE = -0.05160 a.u. (5 d.p.)&amp;lt;/b&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Converting energy from a.u. to kJ/mol&#039;&#039;&#039;&lt;br /&gt;
An atomic unit for energy is Hartree, which is equal to 2625.5 kJ/mol. &amp;lt;ref&amp;gt;https://cccbdb.nist.gov/hartree.asp (Accessed: 22.05.2018)&amp;lt;/ref&amp;gt;&lt;br /&gt;
&lt;br /&gt;
So ΔE in kJ/mol = -0.05159657 * 2625.5 = -135.466794535 kJ/mol&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;ΔE = -135 kJ/mol (nearest integer)&amp;lt;/b&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
The energy difference calculated above comes from the formation of the B-N dative bond. It is a relatively weak bond. According to a bond energy data sheet provided by the University of California, &amp;lt;ref&amp;gt;https://labs.chem.ucsb.edu/zakarian/armen/11---bonddissociationenergy.pdf (Accessed on 24.05.2018)&amp;lt;/ref&amp;gt; the bond energy of the C-C bond of an ethane molecule is 368 kJ/mol. This is a fair comparison to the NH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;BH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt; molecule as the two molecules have the same structure, only with the carbon atoms on ethane swapped for Boron and Nitrogen in NH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;BH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;&lt;br /&gt;
&lt;br /&gt;
==Using a mixture of basis-sets and pseudo-potentials==&lt;br /&gt;
&lt;br /&gt;
===BBr&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;===&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;Calculation type&amp;lt;/b&amp;gt;: Optimisation&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;Calculation Method&amp;lt;/b&amp;gt;: B3LYP&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;Basis set&amp;lt;/b&amp;gt;: Boron: 6-31G(d,p) ; Br: LANL2DZ&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Summary table&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
[[file:Hyc116_bbr3_opt_summarytable.png]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Items table&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;pre&amp;gt;&lt;br /&gt;
Item               Value     Threshold  Converged?&lt;br /&gt;
 Maximum Force            0.000008     0.000450     YES&lt;br /&gt;
 RMS     Force            0.000005     0.000300     YES&lt;br /&gt;
 Maximum Displacement     0.000036     0.001800     YES&lt;br /&gt;
 RMS     Displacement     0.000023     0.001200     YES&lt;br /&gt;
&amp;lt;/pre&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Frequency log file&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
[[Media:Hyc116_bbr3_freq.log]]&lt;br /&gt;
&lt;br /&gt;
Attached above is the frequency file saved onto the computer from the SCAN server portal. The frequency file was also published on the chemistry database DSpace. {{DOI|10042/202442}}&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Frequencies&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;pre&amp;gt;&lt;br /&gt;
Low frequencies ---   -0.0137   -0.0064   -0.0046    2.4315    2.4315    4.8421&lt;br /&gt;
Low frequencies ---  155.9631  155.9651  267.7052&lt;br /&gt;
&amp;lt;/pre&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;jmol of BBr&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;&#039;&#039;&#039;&lt;br /&gt;
&amp;lt;jmol&amp;gt;&amp;lt;jmolApplet&amp;gt;&lt;br /&gt;
  &amp;lt;title&amp;gt;optimised BBr3&amp;lt;/title&amp;gt;&lt;br /&gt;
  &amp;lt;color&amp;gt;black&amp;lt;/color&amp;gt;&lt;br /&gt;
  &amp;lt;size&amp;gt;200&amp;lt;/size&amp;gt;&lt;br /&gt;
  &amp;lt;uploadedFileContents&amp;gt;Hyc116_bbr3_freq.log&amp;lt;/uploadedFileContents&amp;gt;&lt;br /&gt;
&amp;lt;/jmolApplet&amp;gt;&amp;lt;/jmol&amp;gt;&lt;br /&gt;
&lt;br /&gt;
==Aromaticity==&lt;br /&gt;
&lt;br /&gt;
===Benzene===&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;Calculation type&amp;lt;/b&amp;gt;: Optimisation&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;Calculation Method&amp;lt;/b&amp;gt;: B3LYP&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;Basis set&amp;lt;/b&amp;gt;: 6-31G(d,p) &lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Summary table&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
[[file:Hyc116_c6h6_summarytable.png]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Items table&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;pre&amp;gt;&lt;br /&gt;
Item               Value     Threshold  Converged?&lt;br /&gt;
 Maximum Force            0.000193     0.000450     YES&lt;br /&gt;
 RMS     Force            0.000079     0.000300     YES&lt;br /&gt;
 Maximum Displacement     0.000830     0.001800     YES&lt;br /&gt;
 RMS     Displacement     0.000294     0.001200     YES&lt;br /&gt;
&amp;lt;/pre&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Frequency log file&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
[[Media:HYC116_C6H6_FREQ.LOG]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Frequencies&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;pre&amp;gt;&lt;br /&gt;
Low frequencies ---   -3.5606   -3.5606   -0.0089   -0.0043   -0.0043   10.0905&lt;br /&gt;
Low frequencies ---  413.9582  413.9582  621.1416&lt;br /&gt;
&amp;lt;/pre&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;jmol of C&amp;lt;sub&amp;gt;6&amp;lt;/sub&amp;gt;H&amp;lt;sub&amp;gt;6&amp;lt;/sub&amp;gt;&#039;&#039;&#039;&lt;br /&gt;
&amp;lt;jmol&amp;gt;&amp;lt;jmolApplet&amp;gt;&lt;br /&gt;
  &amp;lt;title&amp;gt;optimised Benzene&amp;lt;/title&amp;gt;&lt;br /&gt;
  &amp;lt;color&amp;gt;black&amp;lt;/color&amp;gt;&lt;br /&gt;
  &amp;lt;size&amp;gt;200&amp;lt;/size&amp;gt;&lt;br /&gt;
  &amp;lt;uploadedFileContents&amp;gt;HYC116_C6H6_FREQ.LOG&amp;lt;/uploadedFileContents&amp;gt;&lt;br /&gt;
&amp;lt;/jmolApplet&amp;gt;&amp;lt;/jmol&amp;gt;&lt;br /&gt;
&lt;br /&gt;
===Borazine===&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;Calculation type&amp;lt;/b&amp;gt;: Optimisation&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;Calculation Method&amp;lt;/b&amp;gt;: B3LYP&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;Basis set&amp;lt;/b&amp;gt;: 6-31G(d,p) &lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Summary table&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
[[file:Hyc116_borazine_summarytable.png]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Items table&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;pre&amp;gt;&lt;br /&gt;
Item               Value     Threshold  Converged?&lt;br /&gt;
 Maximum Force            0.000085     0.000450     YES&lt;br /&gt;
 RMS     Force            0.000033     0.000300     YES&lt;br /&gt;
 Maximum Displacement     0.000250     0.001800     YES&lt;br /&gt;
 RMS     Displacement     0.000074     0.001200     YES&lt;br /&gt;
&amp;lt;/pre&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Frequency log file&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
[[Media:HYC116_BORAZINE_FREQ.LOG]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Frequencies&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;pre&amp;gt;&lt;br /&gt;
Low frequencies ---  -12.6626  -12.6626   -8.9272   -0.0211   -0.0104   -0.0104&lt;br /&gt;
Low frequencies ---  289.1112  289.1112  403.8613&lt;br /&gt;
&amp;lt;/pre&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;jmol of Borazine&#039;&#039;&#039;&lt;br /&gt;
&amp;lt;jmol&amp;gt;&amp;lt;jmolApplet&amp;gt;&lt;br /&gt;
  &amp;lt;title&amp;gt;optimised Borazine&amp;lt;/title&amp;gt;&lt;br /&gt;
  &amp;lt;color&amp;gt;black&amp;lt;/color&amp;gt;&lt;br /&gt;
  &amp;lt;size&amp;gt;200&amp;lt;/size&amp;gt;&lt;br /&gt;
  &amp;lt;uploadedFileContents&amp;gt;HYC116_BORAZINE_FREQ.LOG&amp;lt;/uploadedFileContents&amp;gt;&lt;br /&gt;
&amp;lt;/jmolApplet&amp;gt;&amp;lt;/jmol&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
===Charge distribution===&lt;br /&gt;
&lt;br /&gt;
An NBO charge analysis was carried out on both the optimised benzene and borazine. Visualisations of the charge distribution are shown in the table below, with the colour range going from -1.102 to 1.102 for both molecule. This large scale was chosen as it allows direct comparison of the charge on any atoms in these two molecules and shows the relative magnitude of charges on all these atoms. Negative charges are shown in red, and positive charges are shown in green. A neutral charge is displayed in black, so the smaller a charge is (positive or negative), the darker its colour representation is. Larger charges are shown in brighter colours. The charges are also displayed on the atoms as numbers with a neutral charge being zero. Negative charges are shown as negative number and positive charges are shown as positive numbers. &lt;br /&gt;
&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot;&lt;br /&gt;
!&lt;br /&gt;
!Benzene&lt;br /&gt;
!Borazine&lt;br /&gt;
|-&lt;br /&gt;
!Visualisation of charge distribution&lt;br /&gt;
|[[File:Hyc116_benzene_charge_distribution1.png|500x500px|thumb|centre|Charge distribution of Benzene visualisation]]&lt;br /&gt;
|[[File:Hyc116_borazine_charge_distribution1.png|500x500px|thumb|centre|Charge distribution of Borazine visualisation]]&lt;br /&gt;
|-&lt;br /&gt;
!Charge &lt;br /&gt;
|Carbon: -0.239&lt;br /&gt;
&lt;br /&gt;
Hydrogen: 0.239&lt;br /&gt;
|Nitrogen: -1.102 &lt;br /&gt;
&lt;br /&gt;
Boron: 0.747&lt;br /&gt;
&lt;br /&gt;
Hydrogen (bonded to N): 0.432&lt;br /&gt;
&lt;br /&gt;
Hydrogen (bonded to B): -0.077&lt;br /&gt;
|-&lt;br /&gt;
!Discussion&lt;br /&gt;
|From the visualisation, it is shown that there is a slightly negative charge on the carbon atoms, and a positive charge of the same magnitude on the hydrogen atoms. All the carbon atoms have the same charge as they are in identical environments. The same applies to all the hydrogen atoms. This is due to the highly symmetrical structure of benzene. Since the same colour scale was used for both benzene and borazine, and the charges are much smaller in magnitude on atoms in benzene than atoms on borazine, the colours on the charge distribution visualisation is much darker. &lt;br /&gt;
|#explain&lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
===Comparative MOs of Benzene and Borazine===&lt;br /&gt;
&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot;&lt;br /&gt;
!&lt;br /&gt;
!Benzene&lt;br /&gt;
!Borazine&lt;br /&gt;
!Comparison and Discussion&lt;br /&gt;
|-&lt;br /&gt;
!1st comparative pair&lt;br /&gt;
|[[File:Hyc116_benzene_1st_MO_pair_7.png|200x200px|centre]]&lt;br /&gt;
|[[File:Hyc116_borazine_1st_MO_pair_level9.png|200x200px|centre]]&lt;br /&gt;
|MO 9 of both benzene and borazine are comparable. They both show delocalised molecular orbital with an overall bonding character. There is a nodal plane across the molecular orbitals for both benzene and borazine. For benzene, there is contribution from all the carbon and hydrogen s orbitals. Moreover, the molecular orbitals are symmetric to their counterpart of opposite phase. That is not the case for borazine; they are less symmetric in borazine. Nitrogen atoms are more electronegative than boron atoms and pull electron density towards themselves, resulting in a larger MO. There is contribution from all the boron and nitrogen s orbitals, and three of the hydrogen s orbitals, though not all of them. &lt;br /&gt;
|-&lt;br /&gt;
!2nd comparative pair&lt;br /&gt;
|[[File:Hyc116_benzene_2nd_MO_pair_10.png|200x200px|centre]]&lt;br /&gt;
|[[File:Hyc116_borazine_2nd_MO_pair_level11.png|200x200px|centre]]&lt;br /&gt;
|&lt;br /&gt;
|-&lt;br /&gt;
!3rd comparative pair&lt;br /&gt;
|[[File:Hyc116_benzene_3rd_MO_pair_21.png|200x200px|centre]]&lt;br /&gt;
|[[File:Hyc116_borazine_3rd_MO_pair_level21.png|200x200px|centre]]&lt;br /&gt;
|&lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
===Aromaticity: some theories===&lt;br /&gt;
&lt;br /&gt;
==Reference==&lt;/div&gt;</summary>
		<author><name>Hyc116</name></author>
	</entry>
	<entry>
		<id>https://chemwiki.ch.ic.ac.uk/index.php?title=MO_hyc116&amp;diff=730040</id>
		<title>MO hyc116</title>
		<link rel="alternate" type="text/html" href="https://chemwiki.ch.ic.ac.uk/index.php?title=MO_hyc116&amp;diff=730040"/>
		<updated>2018-05-24T16:54:44Z</updated>

		<summary type="html">&lt;p&gt;Hyc116: /* Comparative MOs of Benzene and Borazine */&lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;==BH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;==&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;Calculation type&amp;lt;/b&amp;gt;: Optimisation&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;Calculation Method&amp;lt;/b&amp;gt;: B3LYP&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;Basis set&amp;lt;/b&amp;gt;: 6-31G(d,p) &lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Summary table&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
[[file:Hyc116_bh3_631g_opt_summarytable.png]]&lt;br /&gt;
&lt;br /&gt;
The above summary table was obtained after the 2nd optimisation of BH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt; (after the initial optimisation using the 3-21G basis set). Notice how the symmetry is incorrect and shown as Cs. This is because the symmetry was manually broken at the beginning by changing the bond length of B-H bonds. The point group was manually adjusted and the molecule was optimised again before the frequency analysis and the new summary table is attached below.&lt;br /&gt;
&lt;br /&gt;
[[file:Hyc116_bh3_correctsummarytable.png]]&lt;br /&gt;
&lt;br /&gt;
The above summary table was obtained from the optimisation after adjusting the symmetry. The point shown in this summary table is D&amp;lt;sub&amp;gt;3h&amp;lt;/sub&amp;gt;, which is the correct for BH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;. &lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Items table&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
Below is the items table taken from the optimisation with the correct point group.&lt;br /&gt;
&lt;br /&gt;
&amp;lt;pre&amp;gt;&lt;br /&gt;
Item               Value     Threshold  Converged?&lt;br /&gt;
 Maximum Force            0.000015     0.000450     YES&lt;br /&gt;
 RMS     Force            0.000010     0.000300     YES&lt;br /&gt;
 Maximum Displacement     0.000058     0.001800     YES&lt;br /&gt;
 RMS     Displacement     0.000038     0.001200     YES&lt;br /&gt;
&amp;lt;/pre&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Frequency log file&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
[[Media:HYC116 BH3 FREQ.LOG]] &lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Frequencies&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;pre&amp;gt;&lt;br /&gt;
Low frequencies ---  -10.3498   -3.4492   -1.2454   -0.0055    0.4779    3.2165&lt;br /&gt;
Low frequencies --- 1162.9519 1213.1527 1213.1554&lt;br /&gt;
&amp;lt;/pre&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;jmol of BH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;&#039;&#039;&#039;&lt;br /&gt;
&amp;lt;jmol&amp;gt;&amp;lt;jmolApplet&amp;gt;&lt;br /&gt;
  &amp;lt;title&amp;gt;optimised BH3&amp;lt;/title&amp;gt;&lt;br /&gt;
  &amp;lt;color&amp;gt;black&amp;lt;/color&amp;gt;&lt;br /&gt;
  &amp;lt;size&amp;gt;200&amp;lt;/size&amp;gt;&lt;br /&gt;
  &amp;lt;uploadedFileContents&amp;gt;HYC116_BH3_FREQ.LOG&amp;lt;/uploadedFileContents&amp;gt;&lt;br /&gt;
&amp;lt;/jmolApplet&amp;gt;&amp;lt;/jmol&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
===Vibrational spectrum===&lt;br /&gt;
&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot;&lt;br /&gt;
!wavenumber (cm&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;)&lt;br /&gt;
!Intensity (arbitrary units)&lt;br /&gt;
!symmetry&lt;br /&gt;
!IR active?&lt;br /&gt;
!type&lt;br /&gt;
|-&lt;br /&gt;
|1163&lt;br /&gt;
|93&lt;br /&gt;
|A&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;&#039; &#039;&lt;br /&gt;
|Yes&lt;br /&gt;
|Out of plane bend&lt;br /&gt;
|-&lt;br /&gt;
|1213&lt;br /&gt;
|14&lt;br /&gt;
|E&#039;&lt;br /&gt;
|Very slight&lt;br /&gt;
|Bend&lt;br /&gt;
|-&lt;br /&gt;
|1213&lt;br /&gt;
|14&lt;br /&gt;
|E&#039;&lt;br /&gt;
|Very slight&lt;br /&gt;
|Bend&lt;br /&gt;
|-&lt;br /&gt;
|2582&lt;br /&gt;
|0&lt;br /&gt;
|A&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;&#039;&lt;br /&gt;
|No&lt;br /&gt;
|Symmetric stretch&lt;br /&gt;
|-&lt;br /&gt;
|2716&lt;br /&gt;
|126&lt;br /&gt;
|E&#039;&lt;br /&gt;
|Yes&lt;br /&gt;
|Asymmetric stretch&lt;br /&gt;
|-&lt;br /&gt;
|2716&lt;br /&gt;
|126&lt;br /&gt;
|E&#039;&lt;br /&gt;
|Yes&lt;br /&gt;
|Asymmetric stretch&lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;IR spectrum&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
[[file:Hyc116_ir_bh3.png|400*600]]&lt;br /&gt;
&lt;br /&gt;
There are only three peaks on the IR spectrum of BH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;, despite that there are 6 vibrational modes for the molecule. As shown in the table above, the symmetric stretching mode with A1 symmetry at 2582 cm&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt; is not IR active; naturally, that vibrational mode doesn’t give a peak on the IR spectrum. As shown from the table, two pairs of vibrational modes, the bond angle deformation/bend at 1213 cm&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt; and the asymmetric bond stretch at 2716 cm&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;, are degenerate with the symmetry label E. This means that they have the same energy, and hence give the same wavenumber on the IR spectrum. Each pair of degenerate vibrational modes give rise to one peak. This leaves three peaks, as confirmed by the IR spectrum above.&lt;br /&gt;
&lt;br /&gt;
===Molecular orbitals of BH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;===&lt;br /&gt;
&lt;br /&gt;
[[file:hyc116_bh3_MO_diagram.png]]&lt;br /&gt;
&lt;br /&gt;
The above molecular orbital diagram was taken from Dr Patricia Hunt&#039;s &amp;lt;i&amp;gt;Lecture 4 Tutorial Problem Model Answers&amp;lt;/i&amp;gt;. &amp;lt;ref&amp;gt;P. Hunt, &amp;quot;Lecture 4 Tutorial Problem Model Answers&amp;quot;, 2 (2018)&amp;lt;/ref&amp;gt;. Diagrams of the &amp;quot;real&amp;quot; MOs were obtained from Gaussian.&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
There is no significant difference between the LCAO MOs and the real ones. Features such as orbital phases are shown clearly on both the LCAO MOs and the real MOs, illustrating the bonding/anti-bonding characters of the molecular orbitals. This suggests that the the qualitative MO theory is highly accurate and useful when studying the molecular orbitals of molecules.&lt;br /&gt;
&lt;br /&gt;
==Associated energies: ammonium borane==&lt;br /&gt;
&lt;br /&gt;
===NH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;===&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;Calculation type&amp;lt;/b&amp;gt;: Optimisation&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;Calculation Method&amp;lt;/b&amp;gt;: B3LYP&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;Basis set&amp;lt;/b&amp;gt;: 6-31G(d,p) &lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Summary table&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
[[file:Hyc116_nh3_631g_summarytable.png]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Items table&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;pre&amp;gt;&lt;br /&gt;
Item               Value     Threshold  Converged?&lt;br /&gt;
 Maximum Force            0.000006     0.000450     YES&lt;br /&gt;
 RMS     Force            0.000004     0.000300     YES&lt;br /&gt;
 Maximum Displacement     0.000012     0.001800     YES&lt;br /&gt;
 RMS     Displacement     0.000008     0.001200     YES&lt;br /&gt;
&amp;lt;/pre&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Frequency log file&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
[[Media:HYC116_NH3_FREQ.LOG]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Frequencies&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;pre&amp;gt;&lt;br /&gt;
Low frequencies ---   -8.5646   -8.5588   -0.0047    0.0454    0.1784   26.4183&lt;br /&gt;
Low frequencies --- 1089.7603 1694.1865 1694.1865&lt;br /&gt;
&amp;lt;/pre&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;jmol of NH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;&#039;&#039;&#039;&lt;br /&gt;
&amp;lt;jmol&amp;gt;&amp;lt;jmolApplet&amp;gt;&lt;br /&gt;
  &amp;lt;title&amp;gt;optimised NH3&amp;lt;/title&amp;gt;&lt;br /&gt;
  &amp;lt;color&amp;gt;black&amp;lt;/color&amp;gt;&lt;br /&gt;
  &amp;lt;size&amp;gt;200&amp;lt;/size&amp;gt;&lt;br /&gt;
  &amp;lt;uploadedFileContents&amp;gt;HYC116_NH3_FREQ.LOG&amp;lt;/uploadedFileContents&amp;gt;&lt;br /&gt;
&amp;lt;/jmolApplet&amp;gt;&amp;lt;/jmol&amp;gt;&lt;br /&gt;
&lt;br /&gt;
===NH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;BH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;===&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;Calculation type&amp;lt;/b&amp;gt;: Optimisation&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;Calculation Method&amp;lt;/b&amp;gt;: B3LYP&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;Basis set&amp;lt;/b&amp;gt;: 6-31G(d,p) &lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Summary table&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
[[file:Hyc116_nh3bh3_631g_summarytable.png]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Items table&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;pre&amp;gt;&lt;br /&gt;
Item               Value     Threshold  Converged?&lt;br /&gt;
 Maximum Force            0.000123     0.000450     YES&lt;br /&gt;
 RMS     Force            0.000058     0.000300     YES&lt;br /&gt;
 Maximum Displacement     0.000515     0.001800     YES&lt;br /&gt;
 RMS     Displacement     0.000296     0.001200     YES&lt;br /&gt;
&amp;lt;/pre&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Frequency log file&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
[[Media:HYC116_NH3BH3_FREQ.LOG]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Frequencies&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;pre&amp;gt;&lt;br /&gt;
Low frequencies ---   -0.0014   -0.0011   -0.0006    6.9624   20.4518   43.5542&lt;br /&gt;
Low frequencies ---  266.4530  632.2458  639.0504&lt;br /&gt;
&amp;lt;/pre&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;jmol of NH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;BH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;&#039;&#039;&#039;&lt;br /&gt;
&amp;lt;jmol&amp;gt;&amp;lt;jmolApplet&amp;gt;&lt;br /&gt;
  &amp;lt;title&amp;gt;optimised NH3BH3&amp;lt;/title&amp;gt;&lt;br /&gt;
  &amp;lt;color&amp;gt;black&amp;lt;/color&amp;gt;&lt;br /&gt;
  &amp;lt;size&amp;gt;200&amp;lt;/size&amp;gt;&lt;br /&gt;
  &amp;lt;uploadedFileContents&amp;gt;HYC116_NH3BH3_FREQ.LOG&amp;lt;/uploadedFileContents&amp;gt;&lt;br /&gt;
&amp;lt;/jmolApplet&amp;gt;&amp;lt;/jmol&amp;gt;&lt;br /&gt;
&lt;br /&gt;
===Association energy===&lt;br /&gt;
&lt;br /&gt;
E(BH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;) (using the optimisation with the correct symmetry) = -26.61532363 a.u. = &amp;lt;b&amp;gt;-26.61532 a.u. (5 d.p.)&amp;lt;/b&amp;gt;&lt;br /&gt;
&lt;br /&gt;
E(NH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;) = -56.55776873 a.u. = &amp;lt;b&amp;gt;-56.55777 a.u. (5 d.p.)&amp;lt;/b&amp;gt;&lt;br /&gt;
&lt;br /&gt;
E(NH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;BH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;) = -83.22468893 a.u. = &amp;lt;b&amp;gt;-83.22469 a.u. (5 d.p.)&amp;lt;/b&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
Carrying out calculations using numbers which has already been rounded up can possibly result in errors in the last digit. Hence, here the calculations were carried out using the numbers provided from the optimisations (i.e. with more decimal places than necessary); the answer was then rounded up to the desired accuracy. &lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
ΔE = E(NH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;BH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;)-[E(NH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;)+E(BH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;)]&lt;br /&gt;
&lt;br /&gt;
ΔE = -83.22468893 - (-56.55776873 + -26.61532363) = -0.05159657 a.u. &lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;ΔE = -0.05160 a.u. (5 d.p.)&amp;lt;/b&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Converting energy from a.u. to kJ/mol&#039;&#039;&#039;&lt;br /&gt;
An atomic unit for energy is Hartree, which is equal to 2625.5 kJ/mol. &amp;lt;ref&amp;gt;https://cccbdb.nist.gov/hartree.asp (Accessed: 22.05.2018)&amp;lt;/ref&amp;gt;&lt;br /&gt;
&lt;br /&gt;
So ΔE in kJ/mol = -0.05159657 * 2625.5 = -135.466794535 kJ/mol&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;ΔE = -135 kJ/mol (nearest integer)&amp;lt;/b&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
The energy difference calculated above comes from the formation of the B-N dative bond. It is a relatively weak bond. According to a bond energy data sheet provided by the University of California, &amp;lt;ref&amp;gt;https://labs.chem.ucsb.edu/zakarian/armen/11---bonddissociationenergy.pdf (Accessed on 24.05.2018)&amp;lt;/ref&amp;gt; the bond energy of the C-C bond of an ethane molecule is 368 kJ/mol. This is a fair comparison to the NH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;BH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt; molecule as the two molecules have the same structure, only with the carbon atoms on ethane swapped for Boron and Nitrogen in NH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;BH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;&lt;br /&gt;
&lt;br /&gt;
==Using a mixture of basis-sets and pseudo-potentials==&lt;br /&gt;
&lt;br /&gt;
===BBr&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;===&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;Calculation type&amp;lt;/b&amp;gt;: Optimisation&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;Calculation Method&amp;lt;/b&amp;gt;: B3LYP&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;Basis set&amp;lt;/b&amp;gt;: Boron: 6-31G(d,p) ; Br: LANL2DZ&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Summary table&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
[[file:Hyc116_bbr3_opt_summarytable.png]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Items table&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;pre&amp;gt;&lt;br /&gt;
Item               Value     Threshold  Converged?&lt;br /&gt;
 Maximum Force            0.000008     0.000450     YES&lt;br /&gt;
 RMS     Force            0.000005     0.000300     YES&lt;br /&gt;
 Maximum Displacement     0.000036     0.001800     YES&lt;br /&gt;
 RMS     Displacement     0.000023     0.001200     YES&lt;br /&gt;
&amp;lt;/pre&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Frequency log file&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
[[Media:Hyc116_bbr3_freq.log]]&lt;br /&gt;
&lt;br /&gt;
Attached above is the frequency file saved onto the computer from the SCAN server portal. The frequency file was also published on the chemistry database DSpace. {{DOI|10042/202442}}&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Frequencies&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;pre&amp;gt;&lt;br /&gt;
Low frequencies ---   -0.0137   -0.0064   -0.0046    2.4315    2.4315    4.8421&lt;br /&gt;
Low frequencies ---  155.9631  155.9651  267.7052&lt;br /&gt;
&amp;lt;/pre&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;jmol of BBr&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;&#039;&#039;&#039;&lt;br /&gt;
&amp;lt;jmol&amp;gt;&amp;lt;jmolApplet&amp;gt;&lt;br /&gt;
  &amp;lt;title&amp;gt;optimised BBr3&amp;lt;/title&amp;gt;&lt;br /&gt;
  &amp;lt;color&amp;gt;black&amp;lt;/color&amp;gt;&lt;br /&gt;
  &amp;lt;size&amp;gt;200&amp;lt;/size&amp;gt;&lt;br /&gt;
  &amp;lt;uploadedFileContents&amp;gt;Hyc116_bbr3_freq.log&amp;lt;/uploadedFileContents&amp;gt;&lt;br /&gt;
&amp;lt;/jmolApplet&amp;gt;&amp;lt;/jmol&amp;gt;&lt;br /&gt;
&lt;br /&gt;
==Aromaticity==&lt;br /&gt;
&lt;br /&gt;
===Benzene===&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;Calculation type&amp;lt;/b&amp;gt;: Optimisation&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;Calculation Method&amp;lt;/b&amp;gt;: B3LYP&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;Basis set&amp;lt;/b&amp;gt;: 6-31G(d,p) &lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Summary table&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
[[file:Hyc116_c6h6_summarytable.png]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Items table&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;pre&amp;gt;&lt;br /&gt;
Item               Value     Threshold  Converged?&lt;br /&gt;
 Maximum Force            0.000193     0.000450     YES&lt;br /&gt;
 RMS     Force            0.000079     0.000300     YES&lt;br /&gt;
 Maximum Displacement     0.000830     0.001800     YES&lt;br /&gt;
 RMS     Displacement     0.000294     0.001200     YES&lt;br /&gt;
&amp;lt;/pre&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Frequency log file&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
[[Media:HYC116_C6H6_FREQ.LOG]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Frequencies&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;pre&amp;gt;&lt;br /&gt;
Low frequencies ---   -3.5606   -3.5606   -0.0089   -0.0043   -0.0043   10.0905&lt;br /&gt;
Low frequencies ---  413.9582  413.9582  621.1416&lt;br /&gt;
&amp;lt;/pre&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;jmol of C&amp;lt;sub&amp;gt;6&amp;lt;/sub&amp;gt;H&amp;lt;sub&amp;gt;6&amp;lt;/sub&amp;gt;&#039;&#039;&#039;&lt;br /&gt;
&amp;lt;jmol&amp;gt;&amp;lt;jmolApplet&amp;gt;&lt;br /&gt;
  &amp;lt;title&amp;gt;optimised Benzene&amp;lt;/title&amp;gt;&lt;br /&gt;
  &amp;lt;color&amp;gt;black&amp;lt;/color&amp;gt;&lt;br /&gt;
  &amp;lt;size&amp;gt;200&amp;lt;/size&amp;gt;&lt;br /&gt;
  &amp;lt;uploadedFileContents&amp;gt;HYC116_C6H6_FREQ.LOG&amp;lt;/uploadedFileContents&amp;gt;&lt;br /&gt;
&amp;lt;/jmolApplet&amp;gt;&amp;lt;/jmol&amp;gt;&lt;br /&gt;
&lt;br /&gt;
===Borazine===&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;Calculation type&amp;lt;/b&amp;gt;: Optimisation&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;Calculation Method&amp;lt;/b&amp;gt;: B3LYP&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;Basis set&amp;lt;/b&amp;gt;: 6-31G(d,p) &lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Summary table&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
[[file:Hyc116_borazine_summarytable.png]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Items table&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;pre&amp;gt;&lt;br /&gt;
Item               Value     Threshold  Converged?&lt;br /&gt;
 Maximum Force            0.000085     0.000450     YES&lt;br /&gt;
 RMS     Force            0.000033     0.000300     YES&lt;br /&gt;
 Maximum Displacement     0.000250     0.001800     YES&lt;br /&gt;
 RMS     Displacement     0.000074     0.001200     YES&lt;br /&gt;
&amp;lt;/pre&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Frequency log file&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
[[Media:HYC116_BORAZINE_FREQ.LOG]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Frequencies&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;pre&amp;gt;&lt;br /&gt;
Low frequencies ---  -12.6626  -12.6626   -8.9272   -0.0211   -0.0104   -0.0104&lt;br /&gt;
Low frequencies ---  289.1112  289.1112  403.8613&lt;br /&gt;
&amp;lt;/pre&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;jmol of Borazine&#039;&#039;&#039;&lt;br /&gt;
&amp;lt;jmol&amp;gt;&amp;lt;jmolApplet&amp;gt;&lt;br /&gt;
  &amp;lt;title&amp;gt;optimised Borazine&amp;lt;/title&amp;gt;&lt;br /&gt;
  &amp;lt;color&amp;gt;black&amp;lt;/color&amp;gt;&lt;br /&gt;
  &amp;lt;size&amp;gt;200&amp;lt;/size&amp;gt;&lt;br /&gt;
  &amp;lt;uploadedFileContents&amp;gt;HYC116_BORAZINE_FREQ.LOG&amp;lt;/uploadedFileContents&amp;gt;&lt;br /&gt;
&amp;lt;/jmolApplet&amp;gt;&amp;lt;/jmol&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
===Charge distribution===&lt;br /&gt;
&lt;br /&gt;
An NBO charge analysis was carried out on both the optimised benzene and borazine. Visualisations of the charge distribution are shown in the table below, with the colour range going from -1.102 to 1.102 for both molecule. This large scale was chosen as it allows direct comparison of the charge on any atoms in these two molecules and shows the relative magnitude of charges on all these atoms. Negative charges are shown in red, and positive charges are shown in green. A neutral charge is displayed in black, so the smaller a charge is (positive or negative), the darker its colour representation is. Larger charges are shown in brighter colours. The charges are also displayed on the atoms as numbers with a neutral charge being zero. Negative charges are shown as negative number and positive charges are shown as positive numbers. &lt;br /&gt;
&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot;&lt;br /&gt;
!&lt;br /&gt;
!Benzene&lt;br /&gt;
!Borazine&lt;br /&gt;
|-&lt;br /&gt;
!Visualisation of charge distribution&lt;br /&gt;
|[[File:Hyc116_benzene_charge_distribution1.png|500x500px|thumb|centre|Charge distribution of Benzene visualisation]]&lt;br /&gt;
|[[File:Hyc116_borazine_charge_distribution1.png|500x500px|thumb|centre|Charge distribution of Borazine visualisation]]&lt;br /&gt;
|-&lt;br /&gt;
!Charge &lt;br /&gt;
|Carbon: -0.239&lt;br /&gt;
&lt;br /&gt;
Hydrogen: 0.239&lt;br /&gt;
|Nitrogen: -1.102 &lt;br /&gt;
&lt;br /&gt;
Boron: 0.747&lt;br /&gt;
&lt;br /&gt;
Hydrogen (bonded to N): 0.432&lt;br /&gt;
&lt;br /&gt;
Hydrogen (bonded to B): -0.077&lt;br /&gt;
|-&lt;br /&gt;
!Discussion&lt;br /&gt;
|From the visualisation, it is shown that there is a slightly negative charge on the carbon atoms, and a positive charge of the same magnitude on the hydrogen atoms. All the carbon atoms have the same charge as they are in identical environments. The same applies to all the hydrogen atoms. This is due to the highly symmetrical structure of benzene. Since the same colour scale was used for both benzene and borazine, and the charges are much smaller in magnitude on atoms in benzene than atoms on borazine, the colours on the charge distribution visualisation is much darker. &lt;br /&gt;
|#explain&lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
===Comparative MOs of Benzene and Borazine===&lt;br /&gt;
&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot;&lt;br /&gt;
!&lt;br /&gt;
!Benzene&lt;br /&gt;
!Borazine&lt;br /&gt;
!Comparison and Discussion&lt;br /&gt;
|-&lt;br /&gt;
!1st comparative pair&lt;br /&gt;
|[[File:Hyc116_benzene_1st_MO_pair_7.png|200x200px|centre]]&lt;br /&gt;
|[[File:Hyc116_borazine_1st_MO_pair_level9.png|200x200px|centre]]&lt;br /&gt;
|MO 9 of both benzene and borazine are comparable. They both show delocalised molecular orbitals with a little antibonding character. There is a nodal plane across the molecular orbitals for both benzene and borazine. For benzene, the molecular orbitals are symmetric to their counterpart of opposite phase. That is not the case for borazine; they are less symmetric in borazine. Nitrogen atoms are more electronegative than boron atoms and pull electron density towards themselves, resulting in a larger MO. Also, there is no contribution from some of the hydrogen atoms on borazine.&lt;br /&gt;
|-&lt;br /&gt;
!2nd comparative pair&lt;br /&gt;
|[[File:Hyc116_benzene_2nd_MO_pair_10.png|200x200px|centre]]&lt;br /&gt;
|[[File:Hyc116_borazine_2nd_MO_pair_level11.png|200x200px|centre]]&lt;br /&gt;
|&lt;br /&gt;
|-&lt;br /&gt;
!3rd comparative pair&lt;br /&gt;
|[[File:Hyc116_benzene_3rd_MO_pair_21.png|200x200px|centre]]&lt;br /&gt;
|[[File:Hyc116_borazine_3rd_MO_pair_level21.png|200x200px|centre]]&lt;br /&gt;
|&lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
===Aromaticity: some theories===&lt;br /&gt;
&lt;br /&gt;
==Reference==&lt;/div&gt;</summary>
		<author><name>Hyc116</name></author>
	</entry>
	<entry>
		<id>https://chemwiki.ch.ic.ac.uk/index.php?title=MO_hyc116&amp;diff=729845</id>
		<title>MO hyc116</title>
		<link rel="alternate" type="text/html" href="https://chemwiki.ch.ic.ac.uk/index.php?title=MO_hyc116&amp;diff=729845"/>
		<updated>2018-05-24T16:10:50Z</updated>

		<summary type="html">&lt;p&gt;Hyc116: /* Comparative MOs of Benzene and Borazine */&lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;==BH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;==&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;Calculation type&amp;lt;/b&amp;gt;: Optimisation&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;Calculation Method&amp;lt;/b&amp;gt;: B3LYP&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;Basis set&amp;lt;/b&amp;gt;: 6-31G(d,p) &lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Summary table&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
[[file:Hyc116_bh3_631g_opt_summarytable.png]]&lt;br /&gt;
&lt;br /&gt;
The above summary table was obtained after the 2nd optimisation of BH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt; (after the initial optimisation using the 3-21G basis set). Notice how the symmetry is incorrect and shown as Cs. This is because the symmetry was manually broken at the beginning by changing the bond length of B-H bonds. The point group was manually adjusted and the molecule was optimised again before the frequency analysis and the new summary table is attached below.&lt;br /&gt;
&lt;br /&gt;
[[file:Hyc116_bh3_correctsummarytable.png]]&lt;br /&gt;
&lt;br /&gt;
The above summary table was obtained from the optimisation after adjusting the symmetry. The point shown in this summary table is D&amp;lt;sub&amp;gt;3h&amp;lt;/sub&amp;gt;, which is the correct for BH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;. &lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Items table&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
Below is the items table taken from the optimisation with the correct point group.&lt;br /&gt;
&lt;br /&gt;
&amp;lt;pre&amp;gt;&lt;br /&gt;
Item               Value     Threshold  Converged?&lt;br /&gt;
 Maximum Force            0.000015     0.000450     YES&lt;br /&gt;
 RMS     Force            0.000010     0.000300     YES&lt;br /&gt;
 Maximum Displacement     0.000058     0.001800     YES&lt;br /&gt;
 RMS     Displacement     0.000038     0.001200     YES&lt;br /&gt;
&amp;lt;/pre&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Frequency log file&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
[[Media:HYC116 BH3 FREQ.LOG]] &lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Frequencies&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;pre&amp;gt;&lt;br /&gt;
Low frequencies ---  -10.3498   -3.4492   -1.2454   -0.0055    0.4779    3.2165&lt;br /&gt;
Low frequencies --- 1162.9519 1213.1527 1213.1554&lt;br /&gt;
&amp;lt;/pre&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;jmol of BH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;&#039;&#039;&#039;&lt;br /&gt;
&amp;lt;jmol&amp;gt;&amp;lt;jmolApplet&amp;gt;&lt;br /&gt;
  &amp;lt;title&amp;gt;optimised BH3&amp;lt;/title&amp;gt;&lt;br /&gt;
  &amp;lt;color&amp;gt;black&amp;lt;/color&amp;gt;&lt;br /&gt;
  &amp;lt;size&amp;gt;200&amp;lt;/size&amp;gt;&lt;br /&gt;
  &amp;lt;uploadedFileContents&amp;gt;HYC116_BH3_FREQ.LOG&amp;lt;/uploadedFileContents&amp;gt;&lt;br /&gt;
&amp;lt;/jmolApplet&amp;gt;&amp;lt;/jmol&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
===Vibrational spectrum===&lt;br /&gt;
&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot;&lt;br /&gt;
!wavenumber (cm&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;)&lt;br /&gt;
!Intensity (arbitrary units)&lt;br /&gt;
!symmetry&lt;br /&gt;
!IR active?&lt;br /&gt;
!type&lt;br /&gt;
|-&lt;br /&gt;
|1163&lt;br /&gt;
|93&lt;br /&gt;
|A&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;&#039; &#039;&lt;br /&gt;
|Yes&lt;br /&gt;
|Out of plane bend&lt;br /&gt;
|-&lt;br /&gt;
|1213&lt;br /&gt;
|14&lt;br /&gt;
|E&#039;&lt;br /&gt;
|Very slight&lt;br /&gt;
|Bend&lt;br /&gt;
|-&lt;br /&gt;
|1213&lt;br /&gt;
|14&lt;br /&gt;
|E&#039;&lt;br /&gt;
|Very slight&lt;br /&gt;
|Bend&lt;br /&gt;
|-&lt;br /&gt;
|2582&lt;br /&gt;
|0&lt;br /&gt;
|A&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;&#039;&lt;br /&gt;
|No&lt;br /&gt;
|Symmetric stretch&lt;br /&gt;
|-&lt;br /&gt;
|2716&lt;br /&gt;
|126&lt;br /&gt;
|E&#039;&lt;br /&gt;
|Yes&lt;br /&gt;
|Asymmetric stretch&lt;br /&gt;
|-&lt;br /&gt;
|2716&lt;br /&gt;
|126&lt;br /&gt;
|E&#039;&lt;br /&gt;
|Yes&lt;br /&gt;
|Asymmetric stretch&lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;IR spectrum&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
[[file:Hyc116_ir_bh3.png|400*600]]&lt;br /&gt;
&lt;br /&gt;
There are only three peaks on the IR spectrum of BH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;, despite that there are 6 vibrational modes for the molecule. As shown in the table above, the symmetric stretching mode with A1 symmetry at 2582 cm&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt; is not IR active; naturally, that vibrational mode doesn’t give a peak on the IR spectrum. As shown from the table, two pairs of vibrational modes, the bond angle deformation/bend at 1213 cm&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt; and the asymmetric bond stretch at 2716 cm&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;, are degenerate with the symmetry label E. This means that they have the same energy, and hence give the same wavenumber on the IR spectrum. Each pair of degenerate vibrational modes give rise to one peak. This leaves three peaks, as confirmed by the IR spectrum above.&lt;br /&gt;
&lt;br /&gt;
===Molecular orbitals of BH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;===&lt;br /&gt;
&lt;br /&gt;
[[file:hyc116_bh3_MO_diagram.png]]&lt;br /&gt;
&lt;br /&gt;
The above molecular orbital diagram was taken from Dr Patricia Hunt&#039;s &amp;lt;i&amp;gt;Lecture 4 Tutorial Problem Model Answers&amp;lt;/i&amp;gt;. &amp;lt;ref&amp;gt;P. Hunt, &amp;quot;Lecture 4 Tutorial Problem Model Answers&amp;quot;, 2 (2018)&amp;lt;/ref&amp;gt;. Diagrams of the &amp;quot;real&amp;quot; MOs were obtained from Gaussian.&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
There is no significant difference between the LCAO MOs and the real ones. Features such as orbital phases are shown clearly on both the LCAO MOs and the real MOs, illustrating the bonding/anti-bonding characters of the molecular orbitals. This suggests that the the qualitative MO theory is highly accurate and useful when studying the molecular orbitals of molecules.&lt;br /&gt;
&lt;br /&gt;
==Associated energies: ammonium borane==&lt;br /&gt;
&lt;br /&gt;
===NH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;===&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;Calculation type&amp;lt;/b&amp;gt;: Optimisation&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;Calculation Method&amp;lt;/b&amp;gt;: B3LYP&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;Basis set&amp;lt;/b&amp;gt;: 6-31G(d,p) &lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Summary table&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
[[file:Hyc116_nh3_631g_summarytable.png]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Items table&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;pre&amp;gt;&lt;br /&gt;
Item               Value     Threshold  Converged?&lt;br /&gt;
 Maximum Force            0.000006     0.000450     YES&lt;br /&gt;
 RMS     Force            0.000004     0.000300     YES&lt;br /&gt;
 Maximum Displacement     0.000012     0.001800     YES&lt;br /&gt;
 RMS     Displacement     0.000008     0.001200     YES&lt;br /&gt;
&amp;lt;/pre&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Frequency log file&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
[[Media:HYC116_NH3_FREQ.LOG]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Frequencies&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;pre&amp;gt;&lt;br /&gt;
Low frequencies ---   -8.5646   -8.5588   -0.0047    0.0454    0.1784   26.4183&lt;br /&gt;
Low frequencies --- 1089.7603 1694.1865 1694.1865&lt;br /&gt;
&amp;lt;/pre&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;jmol of NH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;&#039;&#039;&#039;&lt;br /&gt;
&amp;lt;jmol&amp;gt;&amp;lt;jmolApplet&amp;gt;&lt;br /&gt;
  &amp;lt;title&amp;gt;optimised NH3&amp;lt;/title&amp;gt;&lt;br /&gt;
  &amp;lt;color&amp;gt;black&amp;lt;/color&amp;gt;&lt;br /&gt;
  &amp;lt;size&amp;gt;200&amp;lt;/size&amp;gt;&lt;br /&gt;
  &amp;lt;uploadedFileContents&amp;gt;HYC116_NH3_FREQ.LOG&amp;lt;/uploadedFileContents&amp;gt;&lt;br /&gt;
&amp;lt;/jmolApplet&amp;gt;&amp;lt;/jmol&amp;gt;&lt;br /&gt;
&lt;br /&gt;
===NH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;BH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;===&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;Calculation type&amp;lt;/b&amp;gt;: Optimisation&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;Calculation Method&amp;lt;/b&amp;gt;: B3LYP&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;Basis set&amp;lt;/b&amp;gt;: 6-31G(d,p) &lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Summary table&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
[[file:Hyc116_nh3bh3_631g_summarytable.png]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Items table&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;pre&amp;gt;&lt;br /&gt;
Item               Value     Threshold  Converged?&lt;br /&gt;
 Maximum Force            0.000123     0.000450     YES&lt;br /&gt;
 RMS     Force            0.000058     0.000300     YES&lt;br /&gt;
 Maximum Displacement     0.000515     0.001800     YES&lt;br /&gt;
 RMS     Displacement     0.000296     0.001200     YES&lt;br /&gt;
&amp;lt;/pre&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Frequency log file&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
[[Media:HYC116_NH3BH3_FREQ.LOG]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Frequencies&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;pre&amp;gt;&lt;br /&gt;
Low frequencies ---   -0.0014   -0.0011   -0.0006    6.9624   20.4518   43.5542&lt;br /&gt;
Low frequencies ---  266.4530  632.2458  639.0504&lt;br /&gt;
&amp;lt;/pre&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;jmol of NH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;BH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;&#039;&#039;&#039;&lt;br /&gt;
&amp;lt;jmol&amp;gt;&amp;lt;jmolApplet&amp;gt;&lt;br /&gt;
  &amp;lt;title&amp;gt;optimised NH3BH3&amp;lt;/title&amp;gt;&lt;br /&gt;
  &amp;lt;color&amp;gt;black&amp;lt;/color&amp;gt;&lt;br /&gt;
  &amp;lt;size&amp;gt;200&amp;lt;/size&amp;gt;&lt;br /&gt;
  &amp;lt;uploadedFileContents&amp;gt;HYC116_NH3BH3_FREQ.LOG&amp;lt;/uploadedFileContents&amp;gt;&lt;br /&gt;
&amp;lt;/jmolApplet&amp;gt;&amp;lt;/jmol&amp;gt;&lt;br /&gt;
&lt;br /&gt;
===Association energy===&lt;br /&gt;
&lt;br /&gt;
E(BH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;) (using the optimisation with the correct symmetry) = -26.61532363 a.u. = &amp;lt;b&amp;gt;-26.61532 a.u. (5 d.p.)&amp;lt;/b&amp;gt;&lt;br /&gt;
&lt;br /&gt;
E(NH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;) = -56.55776873 a.u. = &amp;lt;b&amp;gt;-56.55777 a.u. (5 d.p.)&amp;lt;/b&amp;gt;&lt;br /&gt;
&lt;br /&gt;
E(NH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;BH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;) = -83.22468893 a.u. = &amp;lt;b&amp;gt;-83.22469 a.u. (5 d.p.)&amp;lt;/b&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
Carrying out calculations using numbers which has already been rounded up can possibly result in errors in the last digit. Hence, here the calculations were carried out using the numbers provided from the optimisations (i.e. with more decimal places than necessary); the answer was then rounded up to the desired accuracy. &lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
ΔE = E(NH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;BH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;)-[E(NH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;)+E(BH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;)]&lt;br /&gt;
&lt;br /&gt;
ΔE = -83.22468893 - (-56.55776873 + -26.61532363) = -0.05159657 a.u. &lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;ΔE = -0.05160 a.u. (5 d.p.)&amp;lt;/b&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Converting energy from a.u. to kJ/mol&#039;&#039;&#039;&lt;br /&gt;
An atomic unit for energy is Hartree, which is equal to 2625.5 kJ/mol. &amp;lt;ref&amp;gt;https://cccbdb.nist.gov/hartree.asp (Accessed: 22.05.2018)&amp;lt;/ref&amp;gt;&lt;br /&gt;
&lt;br /&gt;
So ΔE in kJ/mol = -0.05159657 * 2625.5 = -135.466794535 kJ/mol&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;ΔE = -135 kJ/mol (nearest integer)&amp;lt;/b&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
The energy difference calculated above comes from the formation of the B-N dative bond. It is a relatively weak bond. According to a bond energy data sheet provided by the University of California, &amp;lt;ref&amp;gt;https://labs.chem.ucsb.edu/zakarian/armen/11---bonddissociationenergy.pdf (Accessed on 24.05.2018)&amp;lt;/ref&amp;gt; the bond energy of the C-C bond of an ethane molecule is 368 kJ/mol. This is a fair comparison to the NH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;BH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt; molecule as the two molecules have the same structure, only with the carbon atoms on ethane swapped for Boron and Nitrogen in NH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;BH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;&lt;br /&gt;
&lt;br /&gt;
==Using a mixture of basis-sets and pseudo-potentials==&lt;br /&gt;
&lt;br /&gt;
===BBr&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;===&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;Calculation type&amp;lt;/b&amp;gt;: Optimisation&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;Calculation Method&amp;lt;/b&amp;gt;: B3LYP&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;Basis set&amp;lt;/b&amp;gt;: Boron: 6-31G(d,p) ; Br: LANL2DZ&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Summary table&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
[[file:Hyc116_bbr3_opt_summarytable.png]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Items table&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;pre&amp;gt;&lt;br /&gt;
Item               Value     Threshold  Converged?&lt;br /&gt;
 Maximum Force            0.000008     0.000450     YES&lt;br /&gt;
 RMS     Force            0.000005     0.000300     YES&lt;br /&gt;
 Maximum Displacement     0.000036     0.001800     YES&lt;br /&gt;
 RMS     Displacement     0.000023     0.001200     YES&lt;br /&gt;
&amp;lt;/pre&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Frequency log file&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
[[Media:Hyc116_bbr3_freq.log]]&lt;br /&gt;
&lt;br /&gt;
Attached above is the frequency file saved onto the computer from the SCAN server portal. The frequency file was also published on the chemistry database DSpace. {{DOI|10042/202442}}&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Frequencies&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;pre&amp;gt;&lt;br /&gt;
Low frequencies ---   -0.0137   -0.0064   -0.0046    2.4315    2.4315    4.8421&lt;br /&gt;
Low frequencies ---  155.9631  155.9651  267.7052&lt;br /&gt;
&amp;lt;/pre&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;jmol of BBr&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;&#039;&#039;&#039;&lt;br /&gt;
&amp;lt;jmol&amp;gt;&amp;lt;jmolApplet&amp;gt;&lt;br /&gt;
  &amp;lt;title&amp;gt;optimised BBr3&amp;lt;/title&amp;gt;&lt;br /&gt;
  &amp;lt;color&amp;gt;black&amp;lt;/color&amp;gt;&lt;br /&gt;
  &amp;lt;size&amp;gt;200&amp;lt;/size&amp;gt;&lt;br /&gt;
  &amp;lt;uploadedFileContents&amp;gt;Hyc116_bbr3_freq.log&amp;lt;/uploadedFileContents&amp;gt;&lt;br /&gt;
&amp;lt;/jmolApplet&amp;gt;&amp;lt;/jmol&amp;gt;&lt;br /&gt;
&lt;br /&gt;
==Aromaticity==&lt;br /&gt;
&lt;br /&gt;
===Benzene===&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;Calculation type&amp;lt;/b&amp;gt;: Optimisation&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;Calculation Method&amp;lt;/b&amp;gt;: B3LYP&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;Basis set&amp;lt;/b&amp;gt;: 6-31G(d,p) &lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Summary table&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
[[file:Hyc116_c6h6_summarytable.png]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Items table&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;pre&amp;gt;&lt;br /&gt;
Item               Value     Threshold  Converged?&lt;br /&gt;
 Maximum Force            0.000193     0.000450     YES&lt;br /&gt;
 RMS     Force            0.000079     0.000300     YES&lt;br /&gt;
 Maximum Displacement     0.000830     0.001800     YES&lt;br /&gt;
 RMS     Displacement     0.000294     0.001200     YES&lt;br /&gt;
&amp;lt;/pre&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Frequency log file&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
[[Media:HYC116_C6H6_FREQ.LOG]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Frequencies&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;pre&amp;gt;&lt;br /&gt;
Low frequencies ---   -3.5606   -3.5606   -0.0089   -0.0043   -0.0043   10.0905&lt;br /&gt;
Low frequencies ---  413.9582  413.9582  621.1416&lt;br /&gt;
&amp;lt;/pre&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;jmol of C&amp;lt;sub&amp;gt;6&amp;lt;/sub&amp;gt;H&amp;lt;sub&amp;gt;6&amp;lt;/sub&amp;gt;&#039;&#039;&#039;&lt;br /&gt;
&amp;lt;jmol&amp;gt;&amp;lt;jmolApplet&amp;gt;&lt;br /&gt;
  &amp;lt;title&amp;gt;optimised Benzene&amp;lt;/title&amp;gt;&lt;br /&gt;
  &amp;lt;color&amp;gt;black&amp;lt;/color&amp;gt;&lt;br /&gt;
  &amp;lt;size&amp;gt;200&amp;lt;/size&amp;gt;&lt;br /&gt;
  &amp;lt;uploadedFileContents&amp;gt;HYC116_C6H6_FREQ.LOG&amp;lt;/uploadedFileContents&amp;gt;&lt;br /&gt;
&amp;lt;/jmolApplet&amp;gt;&amp;lt;/jmol&amp;gt;&lt;br /&gt;
&lt;br /&gt;
===Borazine===&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;Calculation type&amp;lt;/b&amp;gt;: Optimisation&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;Calculation Method&amp;lt;/b&amp;gt;: B3LYP&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;Basis set&amp;lt;/b&amp;gt;: 6-31G(d,p) &lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Summary table&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
[[file:Hyc116_borazine_summarytable.png]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Items table&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;pre&amp;gt;&lt;br /&gt;
Item               Value     Threshold  Converged?&lt;br /&gt;
 Maximum Force            0.000085     0.000450     YES&lt;br /&gt;
 RMS     Force            0.000033     0.000300     YES&lt;br /&gt;
 Maximum Displacement     0.000250     0.001800     YES&lt;br /&gt;
 RMS     Displacement     0.000074     0.001200     YES&lt;br /&gt;
&amp;lt;/pre&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Frequency log file&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
[[Media:HYC116_BORAZINE_FREQ.LOG]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Frequencies&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;pre&amp;gt;&lt;br /&gt;
Low frequencies ---  -12.6626  -12.6626   -8.9272   -0.0211   -0.0104   -0.0104&lt;br /&gt;
Low frequencies ---  289.1112  289.1112  403.8613&lt;br /&gt;
&amp;lt;/pre&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;jmol of Borazine&#039;&#039;&#039;&lt;br /&gt;
&amp;lt;jmol&amp;gt;&amp;lt;jmolApplet&amp;gt;&lt;br /&gt;
  &amp;lt;title&amp;gt;optimised Borazine&amp;lt;/title&amp;gt;&lt;br /&gt;
  &amp;lt;color&amp;gt;black&amp;lt;/color&amp;gt;&lt;br /&gt;
  &amp;lt;size&amp;gt;200&amp;lt;/size&amp;gt;&lt;br /&gt;
  &amp;lt;uploadedFileContents&amp;gt;HYC116_BORAZINE_FREQ.LOG&amp;lt;/uploadedFileContents&amp;gt;&lt;br /&gt;
&amp;lt;/jmolApplet&amp;gt;&amp;lt;/jmol&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
===Charge distribution===&lt;br /&gt;
&lt;br /&gt;
An NBO charge analysis was carried out on both the optimised benzene and borazine. Visualisations of the charge distribution are shown in the table below, with the colour range going from -1.102 to 1.102 for both molecule. This large scale was chosen as it allows direct comparison of the charge on any atoms in these two molecules and shows the relative magnitude of charges on all these atoms. Negative charges are shown in red, and positive charges are shown in green. A neutral charge is displayed in black, so the smaller a charge is (positive or negative), the darker its colour representation is. Larger charges are shown in brighter colours. The charges are also displayed on the atoms as numbers with a neutral charge being zero. Negative charges are shown as negative number and positive charges are shown as positive numbers. &lt;br /&gt;
&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot;&lt;br /&gt;
!&lt;br /&gt;
!Benzene&lt;br /&gt;
!Borazine&lt;br /&gt;
|-&lt;br /&gt;
!Visualisation of charge distribution&lt;br /&gt;
|[[File:Hyc116_benzene_charge_distribution1.png|500x500px|thumb|centre|Charge distribution of Benzene visualisation]]&lt;br /&gt;
|[[File:Hyc116_borazine_charge_distribution1.png|500x500px|thumb|centre|Charge distribution of Borazine visualisation]]&lt;br /&gt;
|-&lt;br /&gt;
!Charge &lt;br /&gt;
|Carbon: -0.239&lt;br /&gt;
&lt;br /&gt;
Hydrogen: 0.239&lt;br /&gt;
|Nitrogen: -1.102 &lt;br /&gt;
&lt;br /&gt;
Boron: 0.747&lt;br /&gt;
&lt;br /&gt;
Hydrogen (bonded to N): 0.432&lt;br /&gt;
&lt;br /&gt;
Hydrogen (bonded to B): -0.077&lt;br /&gt;
|-&lt;br /&gt;
!Discussion&lt;br /&gt;
|From the visualisation, it is shown that there is a slightly negative charge on the carbon atoms, and a positive charge of the same magnitude on the hydrogen atoms. All the carbon atoms have the same charge as they are in identical environments. The same applies to all the hydrogen atoms. This is due to the highly symmetrical structure of benzene. Since the same colour scale was used for both benzene and borazine, and the charges are much smaller in magnitude on atoms in benzene than atoms on borazine, the colours on the charge distribution visualisation is much darker. &lt;br /&gt;
|#explain&lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
===Comparative MOs of Benzene and Borazine===&lt;br /&gt;
&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot;&lt;br /&gt;
!&lt;br /&gt;
!Benzene&lt;br /&gt;
!Borazine&lt;br /&gt;
!Comparison and Discussion&lt;br /&gt;
|-&lt;br /&gt;
!1st comparative pair&lt;br /&gt;
|[[File:Hyc116_benzene_1st_MO_pair_7.png|200x200px|centre]]&lt;br /&gt;
|[[File:Hyc116_borazine_1st_MO_pair_level9.png|200x200px|centre]]&lt;br /&gt;
|MO 9 of both benzene and borazine are comparable.&lt;br /&gt;
|-&lt;br /&gt;
!2nd comparative pair&lt;br /&gt;
|[[File:Hyc116_benzene_2nd_MO_pair_10.png|200x200px|centre]]&lt;br /&gt;
|[[File:Hyc116_borazine_2nd_MO_pair_level11.png|200x200px|centre]]&lt;br /&gt;
|&lt;br /&gt;
|-&lt;br /&gt;
!3rd comparative pair&lt;br /&gt;
|[[File:Hyc116_benzene_3rd_MO_pair_21.png|200x200px|centre]]&lt;br /&gt;
|[[File:Hyc116_borazine_3rd_MO_pair_level21.png|200x200px|centre]]&lt;br /&gt;
|&lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
===Aromaticity: some theories===&lt;br /&gt;
&lt;br /&gt;
==Reference==&lt;/div&gt;</summary>
		<author><name>Hyc116</name></author>
	</entry>
	<entry>
		<id>https://chemwiki.ch.ic.ac.uk/index.php?title=MO_hyc116&amp;diff=729756</id>
		<title>MO hyc116</title>
		<link rel="alternate" type="text/html" href="https://chemwiki.ch.ic.ac.uk/index.php?title=MO_hyc116&amp;diff=729756"/>
		<updated>2018-05-24T15:54:32Z</updated>

		<summary type="html">&lt;p&gt;Hyc116: /* Charge distribution */&lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;==BH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;==&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;Calculation type&amp;lt;/b&amp;gt;: Optimisation&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;Calculation Method&amp;lt;/b&amp;gt;: B3LYP&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;Basis set&amp;lt;/b&amp;gt;: 6-31G(d,p) &lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Summary table&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
[[file:Hyc116_bh3_631g_opt_summarytable.png]]&lt;br /&gt;
&lt;br /&gt;
The above summary table was obtained after the 2nd optimisation of BH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt; (after the initial optimisation using the 3-21G basis set). Notice how the symmetry is incorrect and shown as Cs. This is because the symmetry was manually broken at the beginning by changing the bond length of B-H bonds. The point group was manually adjusted and the molecule was optimised again before the frequency analysis and the new summary table is attached below.&lt;br /&gt;
&lt;br /&gt;
[[file:Hyc116_bh3_correctsummarytable.png]]&lt;br /&gt;
&lt;br /&gt;
The above summary table was obtained from the optimisation after adjusting the symmetry. The point shown in this summary table is D&amp;lt;sub&amp;gt;3h&amp;lt;/sub&amp;gt;, which is the correct for BH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;. &lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Items table&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
Below is the items table taken from the optimisation with the correct point group.&lt;br /&gt;
&lt;br /&gt;
&amp;lt;pre&amp;gt;&lt;br /&gt;
Item               Value     Threshold  Converged?&lt;br /&gt;
 Maximum Force            0.000015     0.000450     YES&lt;br /&gt;
 RMS     Force            0.000010     0.000300     YES&lt;br /&gt;
 Maximum Displacement     0.000058     0.001800     YES&lt;br /&gt;
 RMS     Displacement     0.000038     0.001200     YES&lt;br /&gt;
&amp;lt;/pre&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Frequency log file&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
[[Media:HYC116 BH3 FREQ.LOG]] &lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Frequencies&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;pre&amp;gt;&lt;br /&gt;
Low frequencies ---  -10.3498   -3.4492   -1.2454   -0.0055    0.4779    3.2165&lt;br /&gt;
Low frequencies --- 1162.9519 1213.1527 1213.1554&lt;br /&gt;
&amp;lt;/pre&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;jmol of BH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;&#039;&#039;&#039;&lt;br /&gt;
&amp;lt;jmol&amp;gt;&amp;lt;jmolApplet&amp;gt;&lt;br /&gt;
  &amp;lt;title&amp;gt;optimised BH3&amp;lt;/title&amp;gt;&lt;br /&gt;
  &amp;lt;color&amp;gt;black&amp;lt;/color&amp;gt;&lt;br /&gt;
  &amp;lt;size&amp;gt;200&amp;lt;/size&amp;gt;&lt;br /&gt;
  &amp;lt;uploadedFileContents&amp;gt;HYC116_BH3_FREQ.LOG&amp;lt;/uploadedFileContents&amp;gt;&lt;br /&gt;
&amp;lt;/jmolApplet&amp;gt;&amp;lt;/jmol&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
===Vibrational spectrum===&lt;br /&gt;
&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot;&lt;br /&gt;
!wavenumber (cm&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;)&lt;br /&gt;
!Intensity (arbitrary units)&lt;br /&gt;
!symmetry&lt;br /&gt;
!IR active?&lt;br /&gt;
!type&lt;br /&gt;
|-&lt;br /&gt;
|1163&lt;br /&gt;
|93&lt;br /&gt;
|A&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;&#039; &#039;&lt;br /&gt;
|Yes&lt;br /&gt;
|Out of plane bend&lt;br /&gt;
|-&lt;br /&gt;
|1213&lt;br /&gt;
|14&lt;br /&gt;
|E&#039;&lt;br /&gt;
|Very slight&lt;br /&gt;
|Bend&lt;br /&gt;
|-&lt;br /&gt;
|1213&lt;br /&gt;
|14&lt;br /&gt;
|E&#039;&lt;br /&gt;
|Very slight&lt;br /&gt;
|Bend&lt;br /&gt;
|-&lt;br /&gt;
|2582&lt;br /&gt;
|0&lt;br /&gt;
|A&amp;lt;sub&amp;gt;1&amp;lt;/sub&amp;gt;&#039;&lt;br /&gt;
|No&lt;br /&gt;
|Symmetric stretch&lt;br /&gt;
|-&lt;br /&gt;
|2716&lt;br /&gt;
|126&lt;br /&gt;
|E&#039;&lt;br /&gt;
|Yes&lt;br /&gt;
|Asymmetric stretch&lt;br /&gt;
|-&lt;br /&gt;
|2716&lt;br /&gt;
|126&lt;br /&gt;
|E&#039;&lt;br /&gt;
|Yes&lt;br /&gt;
|Asymmetric stretch&lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;IR spectrum&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
[[file:Hyc116_ir_bh3.png|400*600]]&lt;br /&gt;
&lt;br /&gt;
There are only three peaks on the IR spectrum of BH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;, despite that there are 6 vibrational modes for the molecule. As shown in the table above, the symmetric stretching mode with A1 symmetry at 2582 cm&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt; is not IR active; naturally, that vibrational mode doesn’t give a peak on the IR spectrum. As shown from the table, two pairs of vibrational modes, the bond angle deformation/bend at 1213 cm&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt; and the asymmetric bond stretch at 2716 cm&amp;lt;sup&amp;gt;-1&amp;lt;/sup&amp;gt;, are degenerate with the symmetry label E. This means that they have the same energy, and hence give the same wavenumber on the IR spectrum. Each pair of degenerate vibrational modes give rise to one peak. This leaves three peaks, as confirmed by the IR spectrum above.&lt;br /&gt;
&lt;br /&gt;
===Molecular orbitals of BH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;===&lt;br /&gt;
&lt;br /&gt;
[[file:hyc116_bh3_MO_diagram.png]]&lt;br /&gt;
&lt;br /&gt;
The above molecular orbital diagram was taken from Dr Patricia Hunt&#039;s &amp;lt;i&amp;gt;Lecture 4 Tutorial Problem Model Answers&amp;lt;/i&amp;gt;. &amp;lt;ref&amp;gt;P. Hunt, &amp;quot;Lecture 4 Tutorial Problem Model Answers&amp;quot;, 2 (2018)&amp;lt;/ref&amp;gt;. Diagrams of the &amp;quot;real&amp;quot; MOs were obtained from Gaussian.&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
There is no significant difference between the LCAO MOs and the real ones. Features such as orbital phases are shown clearly on both the LCAO MOs and the real MOs, illustrating the bonding/anti-bonding characters of the molecular orbitals. This suggests that the the qualitative MO theory is highly accurate and useful when studying the molecular orbitals of molecules.&lt;br /&gt;
&lt;br /&gt;
==Associated energies: ammonium borane==&lt;br /&gt;
&lt;br /&gt;
===NH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;===&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;Calculation type&amp;lt;/b&amp;gt;: Optimisation&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;Calculation Method&amp;lt;/b&amp;gt;: B3LYP&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;Basis set&amp;lt;/b&amp;gt;: 6-31G(d,p) &lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Summary table&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
[[file:Hyc116_nh3_631g_summarytable.png]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Items table&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;pre&amp;gt;&lt;br /&gt;
Item               Value     Threshold  Converged?&lt;br /&gt;
 Maximum Force            0.000006     0.000450     YES&lt;br /&gt;
 RMS     Force            0.000004     0.000300     YES&lt;br /&gt;
 Maximum Displacement     0.000012     0.001800     YES&lt;br /&gt;
 RMS     Displacement     0.000008     0.001200     YES&lt;br /&gt;
&amp;lt;/pre&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Frequency log file&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
[[Media:HYC116_NH3_FREQ.LOG]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Frequencies&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;pre&amp;gt;&lt;br /&gt;
Low frequencies ---   -8.5646   -8.5588   -0.0047    0.0454    0.1784   26.4183&lt;br /&gt;
Low frequencies --- 1089.7603 1694.1865 1694.1865&lt;br /&gt;
&amp;lt;/pre&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;jmol of NH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;&#039;&#039;&#039;&lt;br /&gt;
&amp;lt;jmol&amp;gt;&amp;lt;jmolApplet&amp;gt;&lt;br /&gt;
  &amp;lt;title&amp;gt;optimised NH3&amp;lt;/title&amp;gt;&lt;br /&gt;
  &amp;lt;color&amp;gt;black&amp;lt;/color&amp;gt;&lt;br /&gt;
  &amp;lt;size&amp;gt;200&amp;lt;/size&amp;gt;&lt;br /&gt;
  &amp;lt;uploadedFileContents&amp;gt;HYC116_NH3_FREQ.LOG&amp;lt;/uploadedFileContents&amp;gt;&lt;br /&gt;
&amp;lt;/jmolApplet&amp;gt;&amp;lt;/jmol&amp;gt;&lt;br /&gt;
&lt;br /&gt;
===NH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;BH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;===&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;Calculation type&amp;lt;/b&amp;gt;: Optimisation&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;Calculation Method&amp;lt;/b&amp;gt;: B3LYP&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;Basis set&amp;lt;/b&amp;gt;: 6-31G(d,p) &lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Summary table&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
[[file:Hyc116_nh3bh3_631g_summarytable.png]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Items table&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;pre&amp;gt;&lt;br /&gt;
Item               Value     Threshold  Converged?&lt;br /&gt;
 Maximum Force            0.000123     0.000450     YES&lt;br /&gt;
 RMS     Force            0.000058     0.000300     YES&lt;br /&gt;
 Maximum Displacement     0.000515     0.001800     YES&lt;br /&gt;
 RMS     Displacement     0.000296     0.001200     YES&lt;br /&gt;
&amp;lt;/pre&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Frequency log file&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
[[Media:HYC116_NH3BH3_FREQ.LOG]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Frequencies&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;pre&amp;gt;&lt;br /&gt;
Low frequencies ---   -0.0014   -0.0011   -0.0006    6.9624   20.4518   43.5542&lt;br /&gt;
Low frequencies ---  266.4530  632.2458  639.0504&lt;br /&gt;
&amp;lt;/pre&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;jmol of NH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;BH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;&#039;&#039;&#039;&lt;br /&gt;
&amp;lt;jmol&amp;gt;&amp;lt;jmolApplet&amp;gt;&lt;br /&gt;
  &amp;lt;title&amp;gt;optimised NH3BH3&amp;lt;/title&amp;gt;&lt;br /&gt;
  &amp;lt;color&amp;gt;black&amp;lt;/color&amp;gt;&lt;br /&gt;
  &amp;lt;size&amp;gt;200&amp;lt;/size&amp;gt;&lt;br /&gt;
  &amp;lt;uploadedFileContents&amp;gt;HYC116_NH3BH3_FREQ.LOG&amp;lt;/uploadedFileContents&amp;gt;&lt;br /&gt;
&amp;lt;/jmolApplet&amp;gt;&amp;lt;/jmol&amp;gt;&lt;br /&gt;
&lt;br /&gt;
===Association energy===&lt;br /&gt;
&lt;br /&gt;
E(BH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;) (using the optimisation with the correct symmetry) = -26.61532363 a.u. = &amp;lt;b&amp;gt;-26.61532 a.u. (5 d.p.)&amp;lt;/b&amp;gt;&lt;br /&gt;
&lt;br /&gt;
E(NH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;) = -56.55776873 a.u. = &amp;lt;b&amp;gt;-56.55777 a.u. (5 d.p.)&amp;lt;/b&amp;gt;&lt;br /&gt;
&lt;br /&gt;
E(NH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;BH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;) = -83.22468893 a.u. = &amp;lt;b&amp;gt;-83.22469 a.u. (5 d.p.)&amp;lt;/b&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
Carrying out calculations using numbers which has already been rounded up can possibly result in errors in the last digit. Hence, here the calculations were carried out using the numbers provided from the optimisations (i.e. with more decimal places than necessary); the answer was then rounded up to the desired accuracy. &lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
ΔE = E(NH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;BH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;)-[E(NH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;)+E(BH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;)]&lt;br /&gt;
&lt;br /&gt;
ΔE = -83.22468893 - (-56.55776873 + -26.61532363) = -0.05159657 a.u. &lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;ΔE = -0.05160 a.u. (5 d.p.)&amp;lt;/b&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Converting energy from a.u. to kJ/mol&#039;&#039;&#039;&lt;br /&gt;
An atomic unit for energy is Hartree, which is equal to 2625.5 kJ/mol. &amp;lt;ref&amp;gt;https://cccbdb.nist.gov/hartree.asp (Accessed: 22.05.2018)&amp;lt;/ref&amp;gt;&lt;br /&gt;
&lt;br /&gt;
So ΔE in kJ/mol = -0.05159657 * 2625.5 = -135.466794535 kJ/mol&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;ΔE = -135 kJ/mol (nearest integer)&amp;lt;/b&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
The energy difference calculated above comes from the formation of the B-N dative bond. It is a relatively weak bond. According to a bond energy data sheet provided by the University of California, &amp;lt;ref&amp;gt;https://labs.chem.ucsb.edu/zakarian/armen/11---bonddissociationenergy.pdf (Accessed on 24.05.2018)&amp;lt;/ref&amp;gt; the bond energy of the C-C bond of an ethane molecule is 368 kJ/mol. This is a fair comparison to the NH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;BH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt; molecule as the two molecules have the same structure, only with the carbon atoms on ethane swapped for Boron and Nitrogen in NH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;BH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;&lt;br /&gt;
&lt;br /&gt;
==Using a mixture of basis-sets and pseudo-potentials==&lt;br /&gt;
&lt;br /&gt;
===BBr&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;===&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;Calculation type&amp;lt;/b&amp;gt;: Optimisation&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;Calculation Method&amp;lt;/b&amp;gt;: B3LYP&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;Basis set&amp;lt;/b&amp;gt;: Boron: 6-31G(d,p) ; Br: LANL2DZ&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Summary table&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
[[file:Hyc116_bbr3_opt_summarytable.png]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Items table&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;pre&amp;gt;&lt;br /&gt;
Item               Value     Threshold  Converged?&lt;br /&gt;
 Maximum Force            0.000008     0.000450     YES&lt;br /&gt;
 RMS     Force            0.000005     0.000300     YES&lt;br /&gt;
 Maximum Displacement     0.000036     0.001800     YES&lt;br /&gt;
 RMS     Displacement     0.000023     0.001200     YES&lt;br /&gt;
&amp;lt;/pre&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Frequency log file&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
[[Media:Hyc116_bbr3_freq.log]]&lt;br /&gt;
&lt;br /&gt;
Attached above is the frequency file saved onto the computer from the SCAN server portal. The frequency file was also published on the chemistry database DSpace. {{DOI|10042/202442}}&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Frequencies&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;pre&amp;gt;&lt;br /&gt;
Low frequencies ---   -0.0137   -0.0064   -0.0046    2.4315    2.4315    4.8421&lt;br /&gt;
Low frequencies ---  155.9631  155.9651  267.7052&lt;br /&gt;
&amp;lt;/pre&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;jmol of BBr&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;&#039;&#039;&#039;&lt;br /&gt;
&amp;lt;jmol&amp;gt;&amp;lt;jmolApplet&amp;gt;&lt;br /&gt;
  &amp;lt;title&amp;gt;optimised BBr3&amp;lt;/title&amp;gt;&lt;br /&gt;
  &amp;lt;color&amp;gt;black&amp;lt;/color&amp;gt;&lt;br /&gt;
  &amp;lt;size&amp;gt;200&amp;lt;/size&amp;gt;&lt;br /&gt;
  &amp;lt;uploadedFileContents&amp;gt;Hyc116_bbr3_freq.log&amp;lt;/uploadedFileContents&amp;gt;&lt;br /&gt;
&amp;lt;/jmolApplet&amp;gt;&amp;lt;/jmol&amp;gt;&lt;br /&gt;
&lt;br /&gt;
==Aromaticity==&lt;br /&gt;
&lt;br /&gt;
===Benzene===&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;Calculation type&amp;lt;/b&amp;gt;: Optimisation&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;Calculation Method&amp;lt;/b&amp;gt;: B3LYP&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;Basis set&amp;lt;/b&amp;gt;: 6-31G(d,p) &lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Summary table&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
[[file:Hyc116_c6h6_summarytable.png]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Items table&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;pre&amp;gt;&lt;br /&gt;
Item               Value     Threshold  Converged?&lt;br /&gt;
 Maximum Force            0.000193     0.000450     YES&lt;br /&gt;
 RMS     Force            0.000079     0.000300     YES&lt;br /&gt;
 Maximum Displacement     0.000830     0.001800     YES&lt;br /&gt;
 RMS     Displacement     0.000294     0.001200     YES&lt;br /&gt;
&amp;lt;/pre&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Frequency log file&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
[[Media:HYC116_C6H6_FREQ.LOG]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Frequencies&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;pre&amp;gt;&lt;br /&gt;
Low frequencies ---   -3.5606   -3.5606   -0.0089   -0.0043   -0.0043   10.0905&lt;br /&gt;
Low frequencies ---  413.9582  413.9582  621.1416&lt;br /&gt;
&amp;lt;/pre&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;jmol of C&amp;lt;sub&amp;gt;6&amp;lt;/sub&amp;gt;H&amp;lt;sub&amp;gt;6&amp;lt;/sub&amp;gt;&#039;&#039;&#039;&lt;br /&gt;
&amp;lt;jmol&amp;gt;&amp;lt;jmolApplet&amp;gt;&lt;br /&gt;
  &amp;lt;title&amp;gt;optimised Benzene&amp;lt;/title&amp;gt;&lt;br /&gt;
  &amp;lt;color&amp;gt;black&amp;lt;/color&amp;gt;&lt;br /&gt;
  &amp;lt;size&amp;gt;200&amp;lt;/size&amp;gt;&lt;br /&gt;
  &amp;lt;uploadedFileContents&amp;gt;HYC116_C6H6_FREQ.LOG&amp;lt;/uploadedFileContents&amp;gt;&lt;br /&gt;
&amp;lt;/jmolApplet&amp;gt;&amp;lt;/jmol&amp;gt;&lt;br /&gt;
&lt;br /&gt;
===Borazine===&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;Calculation type&amp;lt;/b&amp;gt;: Optimisation&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;Calculation Method&amp;lt;/b&amp;gt;: B3LYP&lt;br /&gt;
&lt;br /&gt;
&amp;lt;b&amp;gt;Basis set&amp;lt;/b&amp;gt;: 6-31G(d,p) &lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Summary table&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
[[file:Hyc116_borazine_summarytable.png]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Items table&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;pre&amp;gt;&lt;br /&gt;
Item               Value     Threshold  Converged?&lt;br /&gt;
 Maximum Force            0.000085     0.000450     YES&lt;br /&gt;
 RMS     Force            0.000033     0.000300     YES&lt;br /&gt;
 Maximum Displacement     0.000250     0.001800     YES&lt;br /&gt;
 RMS     Displacement     0.000074     0.001200     YES&lt;br /&gt;
&amp;lt;/pre&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Frequency log file&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
[[Media:HYC116_BORAZINE_FREQ.LOG]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;Frequencies&#039;&#039;&#039;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;pre&amp;gt;&lt;br /&gt;
Low frequencies ---  -12.6626  -12.6626   -8.9272   -0.0211   -0.0104   -0.0104&lt;br /&gt;
Low frequencies ---  289.1112  289.1112  403.8613&lt;br /&gt;
&amp;lt;/pre&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;&#039;jmol of Borazine&#039;&#039;&#039;&lt;br /&gt;
&amp;lt;jmol&amp;gt;&amp;lt;jmolApplet&amp;gt;&lt;br /&gt;
  &amp;lt;title&amp;gt;optimised Borazine&amp;lt;/title&amp;gt;&lt;br /&gt;
  &amp;lt;color&amp;gt;black&amp;lt;/color&amp;gt;&lt;br /&gt;
  &amp;lt;size&amp;gt;200&amp;lt;/size&amp;gt;&lt;br /&gt;
  &amp;lt;uploadedFileContents&amp;gt;HYC116_BORAZINE_FREQ.LOG&amp;lt;/uploadedFileContents&amp;gt;&lt;br /&gt;
&amp;lt;/jmolApplet&amp;gt;&amp;lt;/jmol&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
===Charge distribution===&lt;br /&gt;
&lt;br /&gt;
An NBO charge analysis was carried out on both the optimised benzene and borazine. Visualisations of the charge distribution are shown in the table below, with the colour range going from -1.102 to 1.102 for both molecule. This large scale was chosen as it allows direct comparison of the charge on any atoms in these two molecules and shows the relative magnitude of charges on all these atoms. Negative charges are shown in red, and positive charges are shown in green. A neutral charge is displayed in black, so the smaller a charge is (positive or negative), the darker its colour representation is. Larger charges are shown in brighter colours. The charges are also displayed on the atoms as numbers with a neutral charge being zero. Negative charges are shown as negative number and positive charges are shown as positive numbers. &lt;br /&gt;
&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot;&lt;br /&gt;
!&lt;br /&gt;
!Benzene&lt;br /&gt;
!Borazine&lt;br /&gt;
|-&lt;br /&gt;
!Visualisation of charge distribution&lt;br /&gt;
|[[File:Hyc116_benzene_charge_distribution1.png|500x500px|thumb|centre|Charge distribution of Benzene visualisation]]&lt;br /&gt;
|[[File:Hyc116_borazine_charge_distribution1.png|500x500px|thumb|centre|Charge distribution of Borazine visualisation]]&lt;br /&gt;
|-&lt;br /&gt;
!Charge &lt;br /&gt;
|Carbon: -0.239&lt;br /&gt;
&lt;br /&gt;
Hydrogen: 0.239&lt;br /&gt;
|Nitrogen: -1.102 &lt;br /&gt;
&lt;br /&gt;
Boron: 0.747&lt;br /&gt;
&lt;br /&gt;
Hydrogen (bonded to N): 0.432&lt;br /&gt;
&lt;br /&gt;
Hydrogen (bonded to B): -0.077&lt;br /&gt;
|-&lt;br /&gt;
!Discussion&lt;br /&gt;
|From the visualisation, it is shown that there is a slightly negative charge on the carbon atoms, and a positive charge of the same magnitude on the hydrogen atoms. All the carbon atoms have the same charge as they are in identical environments. The same applies to all the hydrogen atoms. This is due to the highly symmetrical structure of benzene. Since the same colour scale was used for both benzene and borazine, and the charges are much smaller in magnitude on atoms in benzene than atoms on borazine, the colours on the charge distribution visualisation is much darker. &lt;br /&gt;
|#explain&lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
===Comparative MOs of Benzene and Borazine===&lt;br /&gt;
&lt;br /&gt;
{| class=&amp;quot;wikitable&amp;quot;&lt;br /&gt;
!&lt;br /&gt;
!Benzene&lt;br /&gt;
!Borazine&lt;br /&gt;
!Comparison and Discussion&lt;br /&gt;
|-&lt;br /&gt;
!1st comparative pair&lt;br /&gt;
|[[File:Hyc116_benzene_1st_MO_pair_7.png|200x200px|centre]]&lt;br /&gt;
|[[File:Hyc116_borazine_1st_MO_pair_level9.png|200x200px|centre]]&lt;br /&gt;
|&lt;br /&gt;
|-&lt;br /&gt;
!2nd comparative pair&lt;br /&gt;
|[[File:Hyc116_benzene_2nd_MO_pair_10.png|200x200px|centre]]&lt;br /&gt;
|[[File:Hyc116_borazine_2nd_MO_pair_level11.png|200x200px|centre]]&lt;br /&gt;
|&lt;br /&gt;
|-&lt;br /&gt;
!3rd comparative pair&lt;br /&gt;
|[[File:Hyc116_benzene_3rd_MO_pair_21.png|200x200px|centre]]&lt;br /&gt;
|[[File:Hyc116_borazine_3rd_MO_pair_level21.png|200x200px|centre]]&lt;br /&gt;
|&lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
===Aromaticity: some theories===&lt;br /&gt;
&lt;br /&gt;
==Reference==&lt;/div&gt;</summary>
		<author><name>Hyc116</name></author>
	</entry>
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