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	<id>https://chemwiki.ch.ic.ac.uk/api.php?action=feedcontributions&amp;feedformat=atom&amp;user=Ap5817</id>
	<title>ChemWiki - User contributions [en]</title>
	<link rel="self" type="application/atom+xml" href="https://chemwiki.ch.ic.ac.uk/api.php?action=feedcontributions&amp;feedformat=atom&amp;user=Ap5817"/>
	<link rel="alternate" type="text/html" href="https://chemwiki.ch.ic.ac.uk/wiki/Special:Contributions/Ap5817"/>
	<updated>2026-04-20T18:10:28Z</updated>
	<subtitle>User contributions</subtitle>
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	<entry>
		<id>https://chemwiki.ch.ic.ac.uk/index.php?title=User:Ap5817&amp;diff=680687</id>
		<title>User:Ap5817</title>
		<link rel="alternate" type="text/html" href="https://chemwiki.ch.ic.ac.uk/index.php?title=User:Ap5817&amp;diff=680687"/>
		<updated>2018-03-08T16:37:03Z</updated>

		<summary type="html">&lt;p&gt;Ap5817: &lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;== NH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt; molecule ==&lt;br /&gt;
=== NH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt; calculations ===&lt;br /&gt;
Calculation method:RB3LYP&lt;br /&gt;
&lt;br /&gt;
Basis Set = 6-31G(d,p)&lt;br /&gt;
&lt;br /&gt;
Final Energy: E(RB3LYP) = -56.557768 a.u.&lt;br /&gt;
&lt;br /&gt;
Bond length:1.01789 Å&lt;br /&gt;
&lt;br /&gt;
Bond angle: 105.741 °C&lt;br /&gt;
&lt;br /&gt;
Point Group: C3v&amp;lt;pre&amp;gt;&lt;br /&gt;
Item               Value     Threshold  Converged?&lt;br /&gt;
 Maximum Force            0.000004     0.000450     YES&lt;br /&gt;
 RMS     Force            0.000004     0.000300     YES&lt;br /&gt;
 Maximum Displacement     0.000072     0.001800     YES&lt;br /&gt;
 RMS     Displacement     0.000035     0.001200     YES&lt;br /&gt;
&amp;lt;/pre&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&amp;lt;jmol&amp;gt;&amp;lt;jmolApplet&amp;gt;&lt;br /&gt;
&amp;lt;script&amp;gt;frame x.y&amp;lt;/script&amp;gt;&lt;br /&gt;
  &amp;lt;title&amp;gt;test molecule&amp;lt;/title&amp;gt;&lt;br /&gt;
  &amp;lt;color&amp;gt;black&amp;lt;/color&amp;gt;&lt;br /&gt;
  &amp;lt;size&amp;gt;200&amp;lt;/size&amp;gt;&lt;br /&gt;
  &amp;lt;uploadedFileContents&amp;gt;ADRIAN_POPESCU_PHUNT_NH3_OPTF_POP.LOG&amp;lt;/uploadedFileContents&amp;gt;&lt;br /&gt;
&amp;lt;/jmolApplet&amp;gt;&amp;lt;/jmol&amp;gt;&lt;br /&gt;
&lt;br /&gt;
[[Media:ADRIAN_POPESCU_PHUNT_NH3_OPTF_POP.LOG]]&lt;br /&gt;
&lt;br /&gt;
==Vibration analysis of NH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;==&lt;br /&gt;
[[File:Adrian_Popescu_Vibrations3.png|400px|thumb|Vibrational modes of NH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;|centre]]&lt;br /&gt;
===Vibrational modes===&lt;br /&gt;
Number of vibrational modes: 6&lt;br /&gt;
&lt;br /&gt;
Number of degenerate modes: 4 (2 pairs of degenerate vibrational modes )&lt;br /&gt;
&lt;br /&gt;
Number of bending motions: 3&lt;br /&gt;
&lt;br /&gt;
Number of stretching motions: 3&lt;br /&gt;
&lt;br /&gt;
The most symmetric vibrational mode: mode #4&lt;br /&gt;
&lt;br /&gt;
The &#039;&#039;umbrella mode&#039;&#039;: mode #1&lt;br /&gt;
&lt;br /&gt;
Number of bands expected to be seen in an experimental spectrum of gaseous ammonia: 5&lt;br /&gt;
===Charge Analysis===&lt;br /&gt;
[[File:Adrian_Popescu_Charges2.png|400px|center|thumb|Charge distribution of NH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;]]&lt;br /&gt;
&lt;br /&gt;
Charge on the N atom: -1.125&lt;br /&gt;
&lt;br /&gt;
Charge on the H atom: 0.375&lt;br /&gt;
&lt;br /&gt;
As Nitrogen has an electronegativity value of 3.04, which is significantly larger than the one of Hidrogen (2.2), it is expected that on the Nitrogen there will be a negative charge and on Hidrogen a possitive charge.&lt;br /&gt;
&lt;br /&gt;
==Reactivity of the Haber-Bosch process==&lt;br /&gt;
===Analysis of H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;===&lt;br /&gt;
Calculation method: RB3LYP&lt;br /&gt;
&lt;br /&gt;
Basis Set = 6-31G(d,p)&lt;br /&gt;
&lt;br /&gt;
Final Energy: E(RB3LYP) = -1.1785393 a.u.&lt;br /&gt;
&lt;br /&gt;
Bond length: 0.7428 Å&lt;br /&gt;
&amp;lt;pre&amp;gt;&lt;br /&gt;
Item               Value     Threshold  Converged?&lt;br /&gt;
 Maximum Force            0.000004     0.000450     YES&lt;br /&gt;
 RMS     Force            0.000004     0.000300     YES&lt;br /&gt;
 Maximum Displacement     0.000005     0.001800     YES&lt;br /&gt;
 RMS     Displacement     0.000007     0.001200     YES&amp;lt;/pre&amp;gt;&lt;br /&gt;
&amp;lt;pre&amp;gt;&lt;br /&gt;
Vibrational mode    Frequency    Infrared&lt;br /&gt;
#1             4465.6       0.0000&lt;br /&gt;
&amp;lt;/pre&amp;gt;&lt;br /&gt;
There are no vibrational modes with negative frequencies&lt;br /&gt;
&lt;br /&gt;
===Analysis of N&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;===&lt;br /&gt;
Calculation method: RB3LYP&lt;br /&gt;
&lt;br /&gt;
Basis Set = 6-31G(d,p)&lt;br /&gt;
&lt;br /&gt;
Final Energy: E(RB3LYP) = -109.5241268 a.u.&lt;br /&gt;
&lt;br /&gt;
Bond length: 1.1055 Å&lt;br /&gt;
&amp;lt;pre&amp;gt;&lt;br /&gt;
Item               Value     Threshold  Converged?&lt;br /&gt;
 Maximum Force            0.000001     0.000450     YES&lt;br /&gt;
 RMS     Force            0.000001     0.000300     YES&lt;br /&gt;
 Maximum Displacement     0.000000     0.001800     YES&lt;br /&gt;
 RMS     Displacement     0.000000     0.001200     YES&lt;br /&gt;
&amp;lt;/pre&amp;gt;&lt;br /&gt;
&amp;lt;pre&amp;gt;&lt;br /&gt;
Vibrational mode    Frequency    Infrared&lt;br /&gt;
#1             2457.33       0.0000&lt;br /&gt;
&amp;lt;/pre&amp;gt;&lt;br /&gt;
There are no vibrational modes with negative frequencies.&lt;br /&gt;
&lt;br /&gt;
===Calculation of the energy of the Haber-Bosch process===&lt;br /&gt;
N&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; + 3H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; -&amp;gt; 2NH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;&lt;br /&gt;
&lt;br /&gt;
E(NH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;)= -56.557768 a.u.&lt;br /&gt;
&lt;br /&gt;
2*E(NH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;)= -113.115536 a.u.&lt;br /&gt;
&lt;br /&gt;
E(N&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;)= -109.5251268 a.u.&lt;br /&gt;
&lt;br /&gt;
E(H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;)= -1.1785393 a.u.&lt;br /&gt;
&lt;br /&gt;
3*E(H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;)= -3.5359617 a.u.&lt;br /&gt;
&lt;br /&gt;
ΔE= 2*E(NH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;) - [E(N&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;) + 3*E(H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;)] = -145.57 kj/mol&lt;br /&gt;
&lt;br /&gt;
As the reaction is exothermic, the ammonia product is more stable than the gaseous reactants.&lt;br /&gt;
&lt;br /&gt;
The literature value of the Haber-Bosch process is ΔE= -45.8 kj/mol &amp;lt;ref name=&amp;quot;LazyDog&amp;quot; /&amp;gt;, which indicates that the process is still exothermic, but the amount of energy released is significantly smaller.&lt;br /&gt;
&lt;br /&gt;
==Analysis of Cl&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;==&lt;br /&gt;
===General Analysis===&lt;br /&gt;
Calculation method: RB3LYP&lt;br /&gt;
&lt;br /&gt;
Basis Set = 6-31G(d,p)&lt;br /&gt;
&lt;br /&gt;
Final Energy: E(RB3LYP) = -920.3498788 a.u.&lt;br /&gt;
&lt;br /&gt;
Bond length: 2.0417 Å&lt;br /&gt;
===Vibrational Analysis===&lt;br /&gt;
&amp;lt;pre&amp;gt;&lt;br /&gt;
 Item               Value     Threshold  Converged?&lt;br /&gt;
 Maximum Force            0.000043     0.000450     YES&lt;br /&gt;
 RMS     Force            0.000043     0.000300     YES&lt;br /&gt;
 Maximum Displacement     0.000121     0.001800     YES&lt;br /&gt;
 RMS     Displacement     0.000172     0.001200     YES&lt;br /&gt;
&lt;br /&gt;
&amp;lt;/pre&amp;gt;&lt;br /&gt;
&amp;lt;pre&amp;gt;&lt;br /&gt;
Vibrational mode    Frequency    Infrared&lt;br /&gt;
#1             520.32       0.0000&lt;br /&gt;
&amp;lt;/pre&amp;gt;&lt;br /&gt;
There are no vibrational modes with negative frequencies&lt;br /&gt;
===Charge Analysis===&lt;br /&gt;
[[File:Adrian_Popescu_Cl2_Charges2.png|400px|center|thumb|Charge distribution of Cl&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;]]&lt;br /&gt;
As the Cl&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; molecule is made up of identical Cl atoms, the bond between them will be 100% covalent, the electrons that form the sigma bond are equally shared between the Cl atoms, so the charge on each Cl atom is zero.&lt;br /&gt;
&lt;br /&gt;
===Molecular orbitals Analysis===&lt;br /&gt;
[[File:orbital1_.png|400px|thumb|center|2σ&amp;lt;sub&amp;gt;g&amp;lt;/sub&amp;gt; bonding orbital]]&lt;br /&gt;
The 2σ&amp;lt;sub&amp;gt;g&amp;lt;/sub&amp;gt; bonding orbital is deep in energy, occupied, and corresponds to the bonding orbital formed by the 2s AOs of the Cl atoms.&lt;br /&gt;
[[File:Adrian_Popescu_orbital2.png|400px|thumb|center|2σ&amp;lt;sub&amp;gt;u*&amp;lt;/sub&amp;gt; antibonding orbital]]&lt;br /&gt;
The 2σ&amp;lt;sub&amp;gt;u*&amp;lt;/sub&amp;gt; orbital is higher in energy than the 2σ&amp;lt;sub&amp;gt;g&amp;lt;/sub&amp;gt; orbital, is occupied, and corresponds to the antibonding orbital formed by the 2s AOs of the Cl atoms.&lt;br /&gt;
[[File:Adrian_Popescu_orbital3.png|400px|thumb|center|3σ&amp;lt;sub&amp;gt;g&amp;lt;/sub&amp;gt; bonding orbital]]&lt;br /&gt;
The 3σ&amp;lt;sub&amp;gt;g&amp;lt;/sub&amp;gt; orbital is deep in energy, occupied, and corresponds to the bonding orbital formed by the 3p&amp;lt;sub&amp;gt;x&amp;lt;/sub&amp;gt; AOs of the Cl atoms.&lt;br /&gt;
[[File:Adrian_Popescu_homo.png|400px|thumb|center|1π&amp;lt;sub&amp;gt;g*&amp;lt;/sub&amp;gt; antibonding orbital]]&lt;br /&gt;
The 1π&amp;lt;sub&amp;gt;g*&amp;lt;/sub&amp;gt; orbital is high in energy, and is the HOMO (Highest Occupied Molecular Orbital). It corresponds to the antibonding orbital formed by the 3p&amp;lt;sub&amp;gt;y&amp;lt;/sub&amp;gt; (or 3p&amp;lt;sub&amp;gt;z&amp;lt;/sub&amp;gt;, as the orbitals are degenerate) AOs of the Cl atoms.&lt;br /&gt;
[[File:Adrian_Popescu_lumo.png|400px|thumb|center|3σ&amp;lt;sub&amp;gt;u*&amp;lt;/sub&amp;gt; antibonding orbital]]&lt;br /&gt;
The 3σ&amp;lt;sub&amp;gt;u*&amp;lt;/sub&amp;gt; orbital is high in energy, and is the LUMO (Lowest Unoccupied Molecular Orbital). It corresponds to the antibonding orbital formed by the 3p&amp;lt;sub&amp;gt;x&amp;lt;/sub&amp;gt; AOs of the Cl atoms.&lt;br /&gt;
==References==&lt;br /&gt;
&amp;lt;references&amp;gt;&lt;br /&gt;
&amp;lt;ref name=&amp;quot;LazyDog&amp;quot;&amp;gt;https://en.wikipedia.org/wiki/Haber_process.&amp;lt;/ref&amp;gt;&lt;br /&gt;
&amp;lt;/references&amp;gt;&lt;/div&gt;</summary>
		<author><name>Ap5817</name></author>
	</entry>
	<entry>
		<id>https://chemwiki.ch.ic.ac.uk/index.php?title=User:Ap5817&amp;diff=680685</id>
		<title>User:Ap5817</title>
		<link rel="alternate" type="text/html" href="https://chemwiki.ch.ic.ac.uk/index.php?title=User:Ap5817&amp;diff=680685"/>
		<updated>2018-03-08T16:36:38Z</updated>

		<summary type="html">&lt;p&gt;Ap5817: /* Calculation of the energy of the Haber-Bosch process */&lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;== NH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt; molecule ==&lt;br /&gt;
=== NH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt; calculations ===&lt;br /&gt;
Calculation method:RB3LYP&lt;br /&gt;
&lt;br /&gt;
Basis Set = 6-31G(d,p)&lt;br /&gt;
&lt;br /&gt;
Final Energy: E(RB3LYP) = -56.557768 a.u.&lt;br /&gt;
&lt;br /&gt;
Bond length:1.01789 Å&lt;br /&gt;
&lt;br /&gt;
Bond angle: 105.741 °C&lt;br /&gt;
&lt;br /&gt;
Point Group: C3v&amp;lt;pre&amp;gt;&lt;br /&gt;
Item               Value     Threshold  Converged?&lt;br /&gt;
 Maximum Force            0.000004     0.000450     YES&lt;br /&gt;
 RMS     Force            0.000004     0.000300     YES&lt;br /&gt;
 Maximum Displacement     0.000072     0.001800     YES&lt;br /&gt;
 RMS     Displacement     0.000035     0.001200     YES&lt;br /&gt;
&amp;lt;/pre&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&amp;lt;jmol&amp;gt;&amp;lt;jmolApplet&amp;gt;&lt;br /&gt;
&amp;lt;script&amp;gt;frame x.y&amp;lt;/script&amp;gt;&lt;br /&gt;
  &amp;lt;title&amp;gt;test molecule&amp;lt;/title&amp;gt;&lt;br /&gt;
  &amp;lt;color&amp;gt;black&amp;lt;/color&amp;gt;&lt;br /&gt;
  &amp;lt;size&amp;gt;200&amp;lt;/size&amp;gt;&lt;br /&gt;
  &amp;lt;uploadedFileContents&amp;gt;ADRIAN_POPESCU_PHUNT_NH3_OPTF_POP.LOG&amp;lt;/uploadedFileContents&amp;gt;&lt;br /&gt;
&amp;lt;/jmolApplet&amp;gt;&amp;lt;/jmol&amp;gt;&lt;br /&gt;
&lt;br /&gt;
[[Media:ADRIAN_POPESCU_PHUNT_NH3_OPTF_POP.LOG]]&lt;br /&gt;
&lt;br /&gt;
==Vibration analysis of NH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;==&lt;br /&gt;
[[File:Adrian_Popescu_Vibrations3.png|400px|thumb|Vibrational modes of NH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;|centre]]&lt;br /&gt;
===Vibrational modes===&lt;br /&gt;
Number of vibrational modes: 6&lt;br /&gt;
&lt;br /&gt;
Number of degenerate modes: 4 (2 pairs of degenerate vibrational modes )&lt;br /&gt;
&lt;br /&gt;
Number of bending motions: 3&lt;br /&gt;
&lt;br /&gt;
Number of stretching motions: 3&lt;br /&gt;
&lt;br /&gt;
The most symmetric vibrational mode: mode #4&lt;br /&gt;
&lt;br /&gt;
The &#039;&#039;umbrella mode&#039;&#039;: mode #1&lt;br /&gt;
&lt;br /&gt;
Number of bands expected to be seen in an experimental spectrum of gaseous ammonia: 5&lt;br /&gt;
===Charge Analysis===&lt;br /&gt;
[[File:Adrian_Popescu_Charges2.png|400px|center|thumb|Charge distribution of NH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;]]&lt;br /&gt;
&lt;br /&gt;
Charge on the N atom: -1.125&lt;br /&gt;
&lt;br /&gt;
Charge on the H atom: 0.375&lt;br /&gt;
&lt;br /&gt;
As Nitrogen has an electronegativity value of 3.04, which is significantly larger than the one of Hidrogen (2.2), it is expected that on the Nitrogen there will be a negative charge and on Hidrogen a possitive charge.&lt;br /&gt;
&lt;br /&gt;
==Reactivity of the Haber-Bosch process==&lt;br /&gt;
===Analysis of H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;===&lt;br /&gt;
Calculation method: RB3LYP&lt;br /&gt;
&lt;br /&gt;
Basis Set = 6-31G(d,p)&lt;br /&gt;
&lt;br /&gt;
Final Energy: E(RB3LYP) = -1.1785393 a.u.&lt;br /&gt;
&lt;br /&gt;
Bond length: 0.7428 Å&lt;br /&gt;
&amp;lt;pre&amp;gt;&lt;br /&gt;
Item               Value     Threshold  Converged?&lt;br /&gt;
 Maximum Force            0.000004     0.000450     YES&lt;br /&gt;
 RMS     Force            0.000004     0.000300     YES&lt;br /&gt;
 Maximum Displacement     0.000005     0.001800     YES&lt;br /&gt;
 RMS     Displacement     0.000007     0.001200     YES&amp;lt;/pre&amp;gt;&lt;br /&gt;
&amp;lt;pre&amp;gt;&lt;br /&gt;
Vibrational mode    Frequency    Infrared&lt;br /&gt;
#1             4465.6       0.0000&lt;br /&gt;
&amp;lt;/pre&amp;gt;&lt;br /&gt;
There are no vibrational modes with negative frequencies&lt;br /&gt;
&lt;br /&gt;
===Analysis of N&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;===&lt;br /&gt;
Calculation method: RB3LYP&lt;br /&gt;
&lt;br /&gt;
Basis Set = 6-31G(d,p)&lt;br /&gt;
&lt;br /&gt;
Final Energy: E(RB3LYP) = -109.5241268 a.u.&lt;br /&gt;
&lt;br /&gt;
Bond length: 1.1055 Å&lt;br /&gt;
&amp;lt;pre&amp;gt;&lt;br /&gt;
Item               Value     Threshold  Converged?&lt;br /&gt;
 Maximum Force            0.000001     0.000450     YES&lt;br /&gt;
 RMS     Force            0.000001     0.000300     YES&lt;br /&gt;
 Maximum Displacement     0.000000     0.001800     YES&lt;br /&gt;
 RMS     Displacement     0.000000     0.001200     YES&lt;br /&gt;
&amp;lt;/pre&amp;gt;&lt;br /&gt;
&amp;lt;pre&amp;gt;&lt;br /&gt;
Vibrational mode    Frequency    Infrared&lt;br /&gt;
#1             2457.33       0.0000&lt;br /&gt;
&amp;lt;/pre&amp;gt;&lt;br /&gt;
There are no vibrational modes with negative frequencies.&lt;br /&gt;
&lt;br /&gt;
===Calculation of the energy of the Haber-Bosch process===&lt;br /&gt;
N&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; + 3H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; -&amp;gt; 2NH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;&lt;br /&gt;
&lt;br /&gt;
E(NH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;)= -56.557768 a.u.&lt;br /&gt;
&lt;br /&gt;
2*E(NH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;)= -113.115536 a.u.&lt;br /&gt;
&lt;br /&gt;
E(N&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;)= -109.5251268 a.u.&lt;br /&gt;
&lt;br /&gt;
E(H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;)= -1.1785393 a.u.&lt;br /&gt;
&lt;br /&gt;
3*E(H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;)= -3.5359617 a.u.&lt;br /&gt;
&lt;br /&gt;
ΔE= 2*E(NH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;) - [E(N&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;) + 3*E(H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;)] = -145.57 kj/mol&lt;br /&gt;
&lt;br /&gt;
As the reaction is exothermic, the ammonia product is more stable than the gaseous reactants.&lt;br /&gt;
&lt;br /&gt;
The literature value of the Haber-Bosch process is ΔE= -45.8 kj/mol &amp;lt;ref name=&amp;quot;LazyDog&amp;quot; /&amp;gt;, which indicates that the process is still exothermic, but the amount of energy released is significantly smaller.&lt;br /&gt;
&lt;br /&gt;
==Analysis of Cl&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;==&lt;br /&gt;
===General Analysis===&lt;br /&gt;
Calculation method: RB3LYP&lt;br /&gt;
&lt;br /&gt;
Basis Set = 6-31G(d,p)&lt;br /&gt;
&lt;br /&gt;
Final Energy: E(RB3LYP) = -920.3498788 a.u.&lt;br /&gt;
&lt;br /&gt;
Bond length: 2.0417 Å&lt;br /&gt;
===Vibrational Analysis===&lt;br /&gt;
&amp;lt;pre&amp;gt;&lt;br /&gt;
 Item               Value     Threshold  Converged?&lt;br /&gt;
 Maximum Force            0.000043     0.000450     YES&lt;br /&gt;
 RMS     Force            0.000043     0.000300     YES&lt;br /&gt;
 Maximum Displacement     0.000121     0.001800     YES&lt;br /&gt;
 RMS     Displacement     0.000172     0.001200     YES&lt;br /&gt;
&lt;br /&gt;
&amp;lt;/pre&amp;gt;&lt;br /&gt;
&amp;lt;pre&amp;gt;&lt;br /&gt;
Vibrational mode    Frequency    Infrared&lt;br /&gt;
#1             520.32       0.0000&lt;br /&gt;
&amp;lt;/pre&amp;gt;&lt;br /&gt;
There are no vibrational modes with negative frequencies&lt;br /&gt;
===Charge Analysis===&lt;br /&gt;
[[File:Adrian_Popescu_Cl2_Charges2.png|400px|center|thumb|Charge distribution of Cl&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;]]&lt;br /&gt;
As the Cl&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; molecule is made up of identical Cl atoms, the bond between them will be 100% covalent, the electrons that form the sigma bond are equally shared between the Cl atoms, so the charge on each Cl atom is zero.&lt;br /&gt;
&lt;br /&gt;
===Molecular orbitals Analysis===&lt;br /&gt;
[[File:orbital1_.png|400px|thumb|center|2σ&amp;lt;sub&amp;gt;g&amp;lt;/sub&amp;gt; bonding orbital]]&lt;br /&gt;
The 2σ&amp;lt;sub&amp;gt;g&amp;lt;/sub&amp;gt; bonding orbital is deep in energy, occupied, and corresponds to the bonding orbital formed by the 2s AOs of the Cl atoms.&lt;br /&gt;
[[File:Adrian_Popescu_orbital2.png|400px|thumb|center|2σ&amp;lt;sub&amp;gt;u*&amp;lt;/sub&amp;gt; antibonding orbital]]&lt;br /&gt;
The 2σ&amp;lt;sub&amp;gt;u*&amp;lt;/sub&amp;gt; orbital is higher in energy than the 2σ&amp;lt;sub&amp;gt;g&amp;lt;/sub&amp;gt; orbital, is occupied, and corresponds to the antibonding orbital formed by the 2s AOs of the Cl atoms.&lt;br /&gt;
[[File:Adrian_Popescu_orbital3.png|400px|thumb|center|3σ&amp;lt;sub&amp;gt;g&amp;lt;/sub&amp;gt; bonding orbital]]&lt;br /&gt;
The 3σ&amp;lt;sub&amp;gt;g&amp;lt;/sub&amp;gt; orbital is deep in energy, occupied, and corresponds to the bonding orbital formed by the 3p&amp;lt;sub&amp;gt;x&amp;lt;/sub&amp;gt; AOs of the Cl atoms.&lt;br /&gt;
[[File:Adrian_Popescu_homo.png|400px|thumb|center|1π&amp;lt;sub&amp;gt;g*&amp;lt;/sub&amp;gt; antibonding orbital]]&lt;br /&gt;
The 1π&amp;lt;sub&amp;gt;g*&amp;lt;/sub&amp;gt; orbital is high in energy, and is the HOMO (Highest Occupied Molecular Orbital). It corresponds to the antibonding orbital formed by the 3p&amp;lt;sub&amp;gt;y&amp;lt;/sub&amp;gt; (or 3p&amp;lt;sub&amp;gt;z&amp;lt;/sub&amp;gt;, as the orbitals are degenerate) AOs of the Cl atoms.&lt;br /&gt;
[[File:Adrian_Popescu_lumo.png|400px|thumb|center|3σ&amp;lt;sub&amp;gt;u*&amp;lt;/sub&amp;gt; antibonding orbital]]&lt;br /&gt;
The 3σ&amp;lt;sub&amp;gt;u*&amp;lt;/sub&amp;gt; orbital is high in energy, and is the LUMO (Lowest Unoccupied Molecular Orbital). It corresponds to the antibonding orbital formed by the 3p&amp;lt;sub&amp;gt;x&amp;lt;/sub&amp;gt; AOs of the Cl atoms.&lt;/div&gt;</summary>
		<author><name>Ap5817</name></author>
	</entry>
	<entry>
		<id>https://chemwiki.ch.ic.ac.uk/index.php?title=User:Ap5817&amp;diff=680684</id>
		<title>User:Ap5817</title>
		<link rel="alternate" type="text/html" href="https://chemwiki.ch.ic.ac.uk/index.php?title=User:Ap5817&amp;diff=680684"/>
		<updated>2018-03-08T16:35:20Z</updated>

		<summary type="html">&lt;p&gt;Ap5817: &lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;== NH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt; molecule ==&lt;br /&gt;
=== NH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt; calculations ===&lt;br /&gt;
Calculation method:RB3LYP&lt;br /&gt;
&lt;br /&gt;
Basis Set = 6-31G(d,p)&lt;br /&gt;
&lt;br /&gt;
Final Energy: E(RB3LYP) = -56.557768 a.u.&lt;br /&gt;
&lt;br /&gt;
Bond length:1.01789 Å&lt;br /&gt;
&lt;br /&gt;
Bond angle: 105.741 °C&lt;br /&gt;
&lt;br /&gt;
Point Group: C3v&amp;lt;pre&amp;gt;&lt;br /&gt;
Item               Value     Threshold  Converged?&lt;br /&gt;
 Maximum Force            0.000004     0.000450     YES&lt;br /&gt;
 RMS     Force            0.000004     0.000300     YES&lt;br /&gt;
 Maximum Displacement     0.000072     0.001800     YES&lt;br /&gt;
 RMS     Displacement     0.000035     0.001200     YES&lt;br /&gt;
&amp;lt;/pre&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&amp;lt;jmol&amp;gt;&amp;lt;jmolApplet&amp;gt;&lt;br /&gt;
&amp;lt;script&amp;gt;frame x.y&amp;lt;/script&amp;gt;&lt;br /&gt;
  &amp;lt;title&amp;gt;test molecule&amp;lt;/title&amp;gt;&lt;br /&gt;
  &amp;lt;color&amp;gt;black&amp;lt;/color&amp;gt;&lt;br /&gt;
  &amp;lt;size&amp;gt;200&amp;lt;/size&amp;gt;&lt;br /&gt;
  &amp;lt;uploadedFileContents&amp;gt;ADRIAN_POPESCU_PHUNT_NH3_OPTF_POP.LOG&amp;lt;/uploadedFileContents&amp;gt;&lt;br /&gt;
&amp;lt;/jmolApplet&amp;gt;&amp;lt;/jmol&amp;gt;&lt;br /&gt;
&lt;br /&gt;
[[Media:ADRIAN_POPESCU_PHUNT_NH3_OPTF_POP.LOG]]&lt;br /&gt;
&lt;br /&gt;
==Vibration analysis of NH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;==&lt;br /&gt;
[[File:Adrian_Popescu_Vibrations3.png|400px|thumb|Vibrational modes of NH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;|centre]]&lt;br /&gt;
===Vibrational modes===&lt;br /&gt;
Number of vibrational modes: 6&lt;br /&gt;
&lt;br /&gt;
Number of degenerate modes: 4 (2 pairs of degenerate vibrational modes )&lt;br /&gt;
&lt;br /&gt;
Number of bending motions: 3&lt;br /&gt;
&lt;br /&gt;
Number of stretching motions: 3&lt;br /&gt;
&lt;br /&gt;
The most symmetric vibrational mode: mode #4&lt;br /&gt;
&lt;br /&gt;
The &#039;&#039;umbrella mode&#039;&#039;: mode #1&lt;br /&gt;
&lt;br /&gt;
Number of bands expected to be seen in an experimental spectrum of gaseous ammonia: 5&lt;br /&gt;
===Charge Analysis===&lt;br /&gt;
[[File:Adrian_Popescu_Charges2.png|400px|center|thumb|Charge distribution of NH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;]]&lt;br /&gt;
&lt;br /&gt;
Charge on the N atom: -1.125&lt;br /&gt;
&lt;br /&gt;
Charge on the H atom: 0.375&lt;br /&gt;
&lt;br /&gt;
As Nitrogen has an electronegativity value of 3.04, which is significantly larger than the one of Hidrogen (2.2), it is expected that on the Nitrogen there will be a negative charge and on Hidrogen a possitive charge.&lt;br /&gt;
&lt;br /&gt;
==Reactivity of the Haber-Bosch process==&lt;br /&gt;
===Analysis of H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;===&lt;br /&gt;
Calculation method: RB3LYP&lt;br /&gt;
&lt;br /&gt;
Basis Set = 6-31G(d,p)&lt;br /&gt;
&lt;br /&gt;
Final Energy: E(RB3LYP) = -1.1785393 a.u.&lt;br /&gt;
&lt;br /&gt;
Bond length: 0.7428 Å&lt;br /&gt;
&amp;lt;pre&amp;gt;&lt;br /&gt;
Item               Value     Threshold  Converged?&lt;br /&gt;
 Maximum Force            0.000004     0.000450     YES&lt;br /&gt;
 RMS     Force            0.000004     0.000300     YES&lt;br /&gt;
 Maximum Displacement     0.000005     0.001800     YES&lt;br /&gt;
 RMS     Displacement     0.000007     0.001200     YES&amp;lt;/pre&amp;gt;&lt;br /&gt;
&amp;lt;pre&amp;gt;&lt;br /&gt;
Vibrational mode    Frequency    Infrared&lt;br /&gt;
#1             4465.6       0.0000&lt;br /&gt;
&amp;lt;/pre&amp;gt;&lt;br /&gt;
There are no vibrational modes with negative frequencies&lt;br /&gt;
&lt;br /&gt;
===Analysis of N&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;===&lt;br /&gt;
Calculation method: RB3LYP&lt;br /&gt;
&lt;br /&gt;
Basis Set = 6-31G(d,p)&lt;br /&gt;
&lt;br /&gt;
Final Energy: E(RB3LYP) = -109.5241268 a.u.&lt;br /&gt;
&lt;br /&gt;
Bond length: 1.1055 Å&lt;br /&gt;
&amp;lt;pre&amp;gt;&lt;br /&gt;
Item               Value     Threshold  Converged?&lt;br /&gt;
 Maximum Force            0.000001     0.000450     YES&lt;br /&gt;
 RMS     Force            0.000001     0.000300     YES&lt;br /&gt;
 Maximum Displacement     0.000000     0.001800     YES&lt;br /&gt;
 RMS     Displacement     0.000000     0.001200     YES&lt;br /&gt;
&amp;lt;/pre&amp;gt;&lt;br /&gt;
&amp;lt;pre&amp;gt;&lt;br /&gt;
Vibrational mode    Frequency    Infrared&lt;br /&gt;
#1             2457.33       0.0000&lt;br /&gt;
&amp;lt;/pre&amp;gt;&lt;br /&gt;
There are no vibrational modes with negative frequencies.&lt;br /&gt;
&lt;br /&gt;
===Calculation of the energy of the Haber-Bosch process===&lt;br /&gt;
N&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; + 3H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; -&amp;gt; 2NH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;&lt;br /&gt;
&lt;br /&gt;
E(NH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;)= -56.557768 a.u.&lt;br /&gt;
&lt;br /&gt;
2*E(NH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;)= -113.115536 a.u.&lt;br /&gt;
&lt;br /&gt;
E(N&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;)= -109.5251268 a.u.&lt;br /&gt;
&lt;br /&gt;
E(H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;)= -1.1785393 a.u.&lt;br /&gt;
&lt;br /&gt;
3*E(H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;)= -3.5359617 a.u.&lt;br /&gt;
&lt;br /&gt;
ΔE= 2*E(NH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;) - [E(N&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;) + 3*E(H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;)] = -145.57 kj/mol&lt;br /&gt;
&lt;br /&gt;
As the reaction is exothermic, the ammonia product is more stable than the gaseous reactants.&lt;br /&gt;
&lt;br /&gt;
The literature value of the Haber-Bosch process is ΔE= -45.8 kj/mol &amp;lt;ref name=&amp;quot;LazyDog&amp;quot; /&amp;gt;&lt;br /&gt;
&amp;lt;references&amp;gt;&lt;br /&gt;
&amp;lt;ref name=&amp;quot;LazyDog&amp;quot;&amp;gt;https://en.wikipedia.org/wiki/Haber_process.&amp;lt;/ref&amp;gt;&lt;br /&gt;
&amp;lt;/references&amp;gt;, which indicates that the process is still exothermic, but the amount of energy released is significantly smaller.&lt;br /&gt;
&lt;br /&gt;
==Analysis of Cl&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;==&lt;br /&gt;
===General Analysis===&lt;br /&gt;
Calculation method: RB3LYP&lt;br /&gt;
&lt;br /&gt;
Basis Set = 6-31G(d,p)&lt;br /&gt;
&lt;br /&gt;
Final Energy: E(RB3LYP) = -920.3498788 a.u.&lt;br /&gt;
&lt;br /&gt;
Bond length: 2.0417 Å&lt;br /&gt;
===Vibrational Analysis===&lt;br /&gt;
&amp;lt;pre&amp;gt;&lt;br /&gt;
 Item               Value     Threshold  Converged?&lt;br /&gt;
 Maximum Force            0.000043     0.000450     YES&lt;br /&gt;
 RMS     Force            0.000043     0.000300     YES&lt;br /&gt;
 Maximum Displacement     0.000121     0.001800     YES&lt;br /&gt;
 RMS     Displacement     0.000172     0.001200     YES&lt;br /&gt;
&lt;br /&gt;
&amp;lt;/pre&amp;gt;&lt;br /&gt;
&amp;lt;pre&amp;gt;&lt;br /&gt;
Vibrational mode    Frequency    Infrared&lt;br /&gt;
#1             520.32       0.0000&lt;br /&gt;
&amp;lt;/pre&amp;gt;&lt;br /&gt;
There are no vibrational modes with negative frequencies&lt;br /&gt;
===Charge Analysis===&lt;br /&gt;
[[File:Adrian_Popescu_Cl2_Charges2.png|400px|center|thumb|Charge distribution of Cl&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;]]&lt;br /&gt;
As the Cl&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; molecule is made up of identical Cl atoms, the bond between them will be 100% covalent, the electrons that form the sigma bond are equally shared between the Cl atoms, so the charge on each Cl atom is zero.&lt;br /&gt;
&lt;br /&gt;
===Molecular orbitals Analysis===&lt;br /&gt;
[[File:orbital1_.png|400px|thumb|center|2σ&amp;lt;sub&amp;gt;g&amp;lt;/sub&amp;gt; bonding orbital]]&lt;br /&gt;
The 2σ&amp;lt;sub&amp;gt;g&amp;lt;/sub&amp;gt; bonding orbital is deep in energy, occupied, and corresponds to the bonding orbital formed by the 2s AOs of the Cl atoms.&lt;br /&gt;
[[File:Adrian_Popescu_orbital2.png|400px|thumb|center|2σ&amp;lt;sub&amp;gt;u*&amp;lt;/sub&amp;gt; antibonding orbital]]&lt;br /&gt;
The 2σ&amp;lt;sub&amp;gt;u*&amp;lt;/sub&amp;gt; orbital is higher in energy than the 2σ&amp;lt;sub&amp;gt;g&amp;lt;/sub&amp;gt; orbital, is occupied, and corresponds to the antibonding orbital formed by the 2s AOs of the Cl atoms.&lt;br /&gt;
[[File:Adrian_Popescu_orbital3.png|400px|thumb|center|3σ&amp;lt;sub&amp;gt;g&amp;lt;/sub&amp;gt; bonding orbital]]&lt;br /&gt;
The 3σ&amp;lt;sub&amp;gt;g&amp;lt;/sub&amp;gt; orbital is deep in energy, occupied, and corresponds to the bonding orbital formed by the 3p&amp;lt;sub&amp;gt;x&amp;lt;/sub&amp;gt; AOs of the Cl atoms.&lt;br /&gt;
[[File:Adrian_Popescu_homo.png|400px|thumb|center|1π&amp;lt;sub&amp;gt;g*&amp;lt;/sub&amp;gt; antibonding orbital]]&lt;br /&gt;
The 1π&amp;lt;sub&amp;gt;g*&amp;lt;/sub&amp;gt; orbital is high in energy, and is the HOMO (Highest Occupied Molecular Orbital). It corresponds to the antibonding orbital formed by the 3p&amp;lt;sub&amp;gt;y&amp;lt;/sub&amp;gt; (or 3p&amp;lt;sub&amp;gt;z&amp;lt;/sub&amp;gt;, as the orbitals are degenerate) AOs of the Cl atoms.&lt;br /&gt;
[[File:Adrian_Popescu_lumo.png|400px|thumb|center|3σ&amp;lt;sub&amp;gt;u*&amp;lt;/sub&amp;gt; antibonding orbital]]&lt;br /&gt;
The 3σ&amp;lt;sub&amp;gt;u*&amp;lt;/sub&amp;gt; orbital is high in energy, and is the LUMO (Lowest Unoccupied Molecular Orbital). It corresponds to the antibonding orbital formed by the 3p&amp;lt;sub&amp;gt;x&amp;lt;/sub&amp;gt; AOs of the Cl atoms.&lt;/div&gt;</summary>
		<author><name>Ap5817</name></author>
	</entry>
	<entry>
		<id>https://chemwiki.ch.ic.ac.uk/index.php?title=User:Ap5817&amp;diff=680680</id>
		<title>User:Ap5817</title>
		<link rel="alternate" type="text/html" href="https://chemwiki.ch.ic.ac.uk/index.php?title=User:Ap5817&amp;diff=680680"/>
		<updated>2018-03-08T16:33:09Z</updated>

		<summary type="html">&lt;p&gt;Ap5817: &lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;== NH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt; molecule ==&lt;br /&gt;
=== NH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt; calculations ===&lt;br /&gt;
Calculation method:RB3LYP&lt;br /&gt;
&lt;br /&gt;
Basis Set = 6-31G(d,p)&lt;br /&gt;
&lt;br /&gt;
Final Energy: E(RB3LYP) = -56.557768 a.u.&lt;br /&gt;
&lt;br /&gt;
Bond length:1.01789 Å&lt;br /&gt;
&lt;br /&gt;
Bond angle: 105.741 °C&lt;br /&gt;
&lt;br /&gt;
Point Group: C3v&amp;lt;pre&amp;gt;&lt;br /&gt;
Item               Value     Threshold  Converged?&lt;br /&gt;
 Maximum Force            0.000004     0.000450     YES&lt;br /&gt;
 RMS     Force            0.000004     0.000300     YES&lt;br /&gt;
 Maximum Displacement     0.000072     0.001800     YES&lt;br /&gt;
 RMS     Displacement     0.000035     0.001200     YES&lt;br /&gt;
&amp;lt;/pre&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&amp;lt;jmol&amp;gt;&amp;lt;jmolApplet&amp;gt;&lt;br /&gt;
&amp;lt;script&amp;gt;frame x.y&amp;lt;/script&amp;gt;&lt;br /&gt;
  &amp;lt;title&amp;gt;test molecule&amp;lt;/title&amp;gt;&lt;br /&gt;
  &amp;lt;color&amp;gt;black&amp;lt;/color&amp;gt;&lt;br /&gt;
  &amp;lt;size&amp;gt;200&amp;lt;/size&amp;gt;&lt;br /&gt;
  &amp;lt;uploadedFileContents&amp;gt;ADRIAN_POPESCU_PHUNT_NH3_OPTF_POP.LOG&amp;lt;/uploadedFileContents&amp;gt;&lt;br /&gt;
&amp;lt;/jmolApplet&amp;gt;&amp;lt;/jmol&amp;gt;&lt;br /&gt;
&lt;br /&gt;
[[Media:ADRIAN_POPESCU_PHUNT_NH3_OPTF_POP.LOG]]&lt;br /&gt;
&lt;br /&gt;
==Vibration analysis of NH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;==&lt;br /&gt;
[[File:Adrian_Popescu_Vibrations3.png|400px|thumb|Vibrational modes of NH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;|centre]]&lt;br /&gt;
===Vibrational modes===&lt;br /&gt;
Number of vibrational modes: 6&lt;br /&gt;
&lt;br /&gt;
Number of degenerate modes: 4 (2 pairs of degenerate vibrational modes )&lt;br /&gt;
&lt;br /&gt;
Number of bending motions: 3&lt;br /&gt;
&lt;br /&gt;
Number of stretching motions: 3&lt;br /&gt;
&lt;br /&gt;
The most symmetric vibrational mode: mode #4&lt;br /&gt;
&lt;br /&gt;
The &#039;&#039;umbrella mode&#039;&#039;: mode #1&lt;br /&gt;
&lt;br /&gt;
Number of bands expected to be seen in an experimental spectrum of gaseous ammonia: 5&lt;br /&gt;
===Charge Analysis===&lt;br /&gt;
[[File:Adrian_Popescu_Charges2.png|400px|center|thumb|Charge distribution of NH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;]]&lt;br /&gt;
&lt;br /&gt;
Charge on the N atom: -1.125&lt;br /&gt;
&lt;br /&gt;
Charge on the H atom: 0.375&lt;br /&gt;
&lt;br /&gt;
As Nitrogen has an electronegativity value of 3.04, which is significantly larger than the one of Hidrogen (2.2), it is expected that on the Nitrogen there will be a negative charge and on Hidrogen a possitive charge.&lt;br /&gt;
&lt;br /&gt;
==Reactivity of the Haber-Bosch process==&lt;br /&gt;
===Analysis of H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;===&lt;br /&gt;
Calculation method: RB3LYP&lt;br /&gt;
&lt;br /&gt;
Basis Set = 6-31G(d,p)&lt;br /&gt;
&lt;br /&gt;
Final Energy: E(RB3LYP) = -1.1785393 a.u.&lt;br /&gt;
&lt;br /&gt;
Bond length: 0.7428 Å&lt;br /&gt;
&amp;lt;pre&amp;gt;&lt;br /&gt;
Item               Value     Threshold  Converged?&lt;br /&gt;
 Maximum Force            0.000004     0.000450     YES&lt;br /&gt;
 RMS     Force            0.000004     0.000300     YES&lt;br /&gt;
 Maximum Displacement     0.000005     0.001800     YES&lt;br /&gt;
 RMS     Displacement     0.000007     0.001200     YES&amp;lt;/pre&amp;gt;&lt;br /&gt;
&amp;lt;pre&amp;gt;&lt;br /&gt;
Vibrational mode    Frequency    Infrared&lt;br /&gt;
#1             4465.6       0.0000&lt;br /&gt;
&amp;lt;/pre&amp;gt;&lt;br /&gt;
There are no vibrational modes with negative frequencies&lt;br /&gt;
&lt;br /&gt;
===Analysis of N&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;===&lt;br /&gt;
Calculation method: RB3LYP&lt;br /&gt;
&lt;br /&gt;
Basis Set = 6-31G(d,p)&lt;br /&gt;
&lt;br /&gt;
Final Energy: E(RB3LYP) = -109.5241268 a.u.&lt;br /&gt;
&lt;br /&gt;
Bond length: 1.1055 Å&lt;br /&gt;
&amp;lt;pre&amp;gt;&lt;br /&gt;
Item               Value     Threshold  Converged?&lt;br /&gt;
 Maximum Force            0.000001     0.000450     YES&lt;br /&gt;
 RMS     Force            0.000001     0.000300     YES&lt;br /&gt;
 Maximum Displacement     0.000000     0.001800     YES&lt;br /&gt;
 RMS     Displacement     0.000000     0.001200     YES&lt;br /&gt;
&amp;lt;/pre&amp;gt;&lt;br /&gt;
&amp;lt;pre&amp;gt;&lt;br /&gt;
Vibrational mode    Frequency    Infrared&lt;br /&gt;
#1             2457.33       0.0000&lt;br /&gt;
&amp;lt;/pre&amp;gt;&lt;br /&gt;
There are no vibrational modes with negative frequencies.&lt;br /&gt;
&lt;br /&gt;
===Calculation of the energy of the Haber-Bosch process===&lt;br /&gt;
N&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; + 3H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; -&amp;gt; 2NH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;&lt;br /&gt;
&lt;br /&gt;
E(NH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;)= -56.557768 a.u.&lt;br /&gt;
&lt;br /&gt;
2*E(NH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;)= -113.115536 a.u.&lt;br /&gt;
&lt;br /&gt;
E(N&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;)= -109.5251268 a.u.&lt;br /&gt;
&lt;br /&gt;
E(H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;)= -1.1785393 a.u.&lt;br /&gt;
&lt;br /&gt;
3*E(H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;)= -3.5359617 a.u.&lt;br /&gt;
&lt;br /&gt;
ΔE= 2*E(NH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;) - [E(N&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;) + 3*E(H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;)] = -145.57 kj/mol&lt;br /&gt;
&lt;br /&gt;
As the reaction is exothermic, the ammonia product is more stable than the gaseous reactants.&lt;br /&gt;
&lt;br /&gt;
The literature value of the Haber-Bosch process is ΔE= -45.8 kj/mol &amp;lt;references/&amp;gt;, which indicates that the process is still exothermic, but the amount of energy released is significantly smaller.&lt;br /&gt;
&lt;br /&gt;
==Analysis of Cl&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;==&lt;br /&gt;
===General Analysis===&lt;br /&gt;
Calculation method: RB3LYP&lt;br /&gt;
&lt;br /&gt;
Basis Set = 6-31G(d,p)&lt;br /&gt;
&lt;br /&gt;
Final Energy: E(RB3LYP) = -920.3498788 a.u.&lt;br /&gt;
&lt;br /&gt;
Bond length: 2.0417 Å&lt;br /&gt;
===Vibrational Analysis===&lt;br /&gt;
&amp;lt;pre&amp;gt;&lt;br /&gt;
 Item               Value     Threshold  Converged?&lt;br /&gt;
 Maximum Force            0.000043     0.000450     YES&lt;br /&gt;
 RMS     Force            0.000043     0.000300     YES&lt;br /&gt;
 Maximum Displacement     0.000121     0.001800     YES&lt;br /&gt;
 RMS     Displacement     0.000172     0.001200     YES&lt;br /&gt;
&lt;br /&gt;
&amp;lt;/pre&amp;gt;&lt;br /&gt;
&amp;lt;pre&amp;gt;&lt;br /&gt;
Vibrational mode    Frequency    Infrared&lt;br /&gt;
#1             520.32       0.0000&lt;br /&gt;
&amp;lt;/pre&amp;gt;&lt;br /&gt;
There are no vibrational modes with negative frequencies&lt;br /&gt;
===Charge Analysis===&lt;br /&gt;
[[File:Adrian_Popescu_Cl2_Charges2.png|400px|center|thumb|Charge distribution of Cl&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;]]&lt;br /&gt;
As the Cl&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; molecule is made up of identical Cl atoms, the bond between them will be 100% covalent, the electrons that form the sigma bond are equally shared between the Cl atoms, so the charge on each Cl atom is zero.&lt;br /&gt;
&lt;br /&gt;
===Molecular orbitals Analysis===&lt;br /&gt;
[[File:orbital1_.png|400px|thumb|center|2σ&amp;lt;sub&amp;gt;g&amp;lt;/sub&amp;gt; bonding orbital]]&lt;br /&gt;
The 2σ&amp;lt;sub&amp;gt;g&amp;lt;/sub&amp;gt; bonding orbital is deep in energy, occupied, and corresponds to the bonding orbital formed by the 2s AOs of the Cl atoms.&lt;br /&gt;
[[File:Adrian_Popescu_orbital2.png|400px|thumb|center|2σ&amp;lt;sub&amp;gt;u*&amp;lt;/sub&amp;gt; antibonding orbital]]&lt;br /&gt;
The 2σ&amp;lt;sub&amp;gt;u*&amp;lt;/sub&amp;gt; orbital is higher in energy than the 2σ&amp;lt;sub&amp;gt;g&amp;lt;/sub&amp;gt; orbital, is occupied, and corresponds to the antibonding orbital formed by the 2s AOs of the Cl atoms.&lt;br /&gt;
[[File:Adrian_Popescu_orbital3.png|400px|thumb|center|3σ&amp;lt;sub&amp;gt;g&amp;lt;/sub&amp;gt; bonding orbital]]&lt;br /&gt;
The 3σ&amp;lt;sub&amp;gt;g&amp;lt;/sub&amp;gt; orbital is deep in energy, occupied, and corresponds to the bonding orbital formed by the 3p&amp;lt;sub&amp;gt;x&amp;lt;/sub&amp;gt; AOs of the Cl atoms.&lt;br /&gt;
[[File:Adrian_Popescu_homo.png|400px|thumb|center|1π&amp;lt;sub&amp;gt;g*&amp;lt;/sub&amp;gt; antibonding orbital]]&lt;br /&gt;
The 1π&amp;lt;sub&amp;gt;g*&amp;lt;/sub&amp;gt; orbital is high in energy, and is the HOMO (Highest Occupied Molecular Orbital). It corresponds to the antibonding orbital formed by the 3p&amp;lt;sub&amp;gt;y&amp;lt;/sub&amp;gt; (or 3p&amp;lt;sub&amp;gt;z&amp;lt;/sub&amp;gt;, as the orbitals are degenerate) AOs of the Cl atoms.&lt;br /&gt;
[[File:Adrian_Popescu_lumo.png|400px|thumb|center|3σ&amp;lt;sub&amp;gt;u*&amp;lt;/sub&amp;gt; antibonding orbital]]&lt;br /&gt;
The 3σ&amp;lt;sub&amp;gt;u*&amp;lt;/sub&amp;gt; orbital is high in energy, and is the LUMO (Lowest Unoccupied Molecular Orbital). It corresponds to the antibonding orbital formed by the 3p&amp;lt;sub&amp;gt;x&amp;lt;/sub&amp;gt; AOs of the Cl atoms.&lt;br /&gt;
The quick brown fox jumps over the lazy dog.&amp;lt;ref name=&amp;quot;LazyDog&amp;quot; /&amp;gt;&lt;br /&gt;
&amp;lt;references&amp;gt;&lt;br /&gt;
&amp;lt;ref name=&amp;quot;LazyDog&amp;quot;&amp;gt;This is the lazy dog reference.&amp;lt;/ref&amp;gt;&lt;br /&gt;
&amp;lt;/references&amp;gt;&lt;/div&gt;</summary>
		<author><name>Ap5817</name></author>
	</entry>
	<entry>
		<id>https://chemwiki.ch.ic.ac.uk/index.php?title=User:Ap5817&amp;diff=680678</id>
		<title>User:Ap5817</title>
		<link rel="alternate" type="text/html" href="https://chemwiki.ch.ic.ac.uk/index.php?title=User:Ap5817&amp;diff=680678"/>
		<updated>2018-03-08T16:32:20Z</updated>

		<summary type="html">&lt;p&gt;Ap5817: /* Calculation of the energy of the Haber-Bosch process */&lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;== NH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt; molecule ==&lt;br /&gt;
=== NH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt; calculations ===&lt;br /&gt;
Calculation method:RB3LYP&lt;br /&gt;
&lt;br /&gt;
Basis Set = 6-31G(d,p)&lt;br /&gt;
&lt;br /&gt;
Final Energy: E(RB3LYP) = -56.557768 a.u.&lt;br /&gt;
&lt;br /&gt;
Bond length:1.01789 Å&lt;br /&gt;
&lt;br /&gt;
Bond angle: 105.741 °C&lt;br /&gt;
&lt;br /&gt;
Point Group: C3v&amp;lt;pre&amp;gt;&lt;br /&gt;
Item               Value     Threshold  Converged?&lt;br /&gt;
 Maximum Force            0.000004     0.000450     YES&lt;br /&gt;
 RMS     Force            0.000004     0.000300     YES&lt;br /&gt;
 Maximum Displacement     0.000072     0.001800     YES&lt;br /&gt;
 RMS     Displacement     0.000035     0.001200     YES&lt;br /&gt;
&amp;lt;/pre&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&amp;lt;jmol&amp;gt;&amp;lt;jmolApplet&amp;gt;&lt;br /&gt;
&amp;lt;script&amp;gt;frame x.y&amp;lt;/script&amp;gt;&lt;br /&gt;
  &amp;lt;title&amp;gt;test molecule&amp;lt;/title&amp;gt;&lt;br /&gt;
  &amp;lt;color&amp;gt;black&amp;lt;/color&amp;gt;&lt;br /&gt;
  &amp;lt;size&amp;gt;200&amp;lt;/size&amp;gt;&lt;br /&gt;
  &amp;lt;uploadedFileContents&amp;gt;ADRIAN_POPESCU_PHUNT_NH3_OPTF_POP.LOG&amp;lt;/uploadedFileContents&amp;gt;&lt;br /&gt;
&amp;lt;/jmolApplet&amp;gt;&amp;lt;/jmol&amp;gt;&lt;br /&gt;
&lt;br /&gt;
[[Media:ADRIAN_POPESCU_PHUNT_NH3_OPTF_POP.LOG]]&lt;br /&gt;
&lt;br /&gt;
==Vibration analysis of NH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;==&lt;br /&gt;
[[File:Adrian_Popescu_Vibrations3.png|400px|thumb|Vibrational modes of NH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;|centre]]&lt;br /&gt;
===Vibrational modes===&lt;br /&gt;
Number of vibrational modes: 6&lt;br /&gt;
&lt;br /&gt;
Number of degenerate modes: 4 (2 pairs of degenerate vibrational modes )&lt;br /&gt;
&lt;br /&gt;
Number of bending motions: 3&lt;br /&gt;
&lt;br /&gt;
Number of stretching motions: 3&lt;br /&gt;
&lt;br /&gt;
The most symmetric vibrational mode: mode #4&lt;br /&gt;
&lt;br /&gt;
The &#039;&#039;umbrella mode&#039;&#039;: mode #1&lt;br /&gt;
&lt;br /&gt;
Number of bands expected to be seen in an experimental spectrum of gaseous ammonia: 5&lt;br /&gt;
===Charge Analysis===&lt;br /&gt;
[[File:Adrian_Popescu_Charges2.png|400px|center|thumb|Charge distribution of NH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;]]&lt;br /&gt;
&lt;br /&gt;
Charge on the N atom: -1.125&lt;br /&gt;
&lt;br /&gt;
Charge on the H atom: 0.375&lt;br /&gt;
&lt;br /&gt;
As Nitrogen has an electronegativity value of 3.04, which is significantly larger than the one of Hidrogen (2.2), it is expected that on the Nitrogen there will be a negative charge and on Hidrogen a possitive charge.&lt;br /&gt;
&lt;br /&gt;
==Reactivity of the Haber-Bosch process==&lt;br /&gt;
===Analysis of H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;===&lt;br /&gt;
Calculation method: RB3LYP&lt;br /&gt;
&lt;br /&gt;
Basis Set = 6-31G(d,p)&lt;br /&gt;
&lt;br /&gt;
Final Energy: E(RB3LYP) = -1.1785393 a.u.&lt;br /&gt;
&lt;br /&gt;
Bond length: 0.7428 Å&lt;br /&gt;
&amp;lt;pre&amp;gt;&lt;br /&gt;
Item               Value     Threshold  Converged?&lt;br /&gt;
 Maximum Force            0.000004     0.000450     YES&lt;br /&gt;
 RMS     Force            0.000004     0.000300     YES&lt;br /&gt;
 Maximum Displacement     0.000005     0.001800     YES&lt;br /&gt;
 RMS     Displacement     0.000007     0.001200     YES&amp;lt;/pre&amp;gt;&lt;br /&gt;
&amp;lt;pre&amp;gt;&lt;br /&gt;
Vibrational mode    Frequency    Infrared&lt;br /&gt;
#1             4465.6       0.0000&lt;br /&gt;
&amp;lt;/pre&amp;gt;&lt;br /&gt;
There are no vibrational modes with negative frequencies&lt;br /&gt;
&lt;br /&gt;
===Analysis of N&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;===&lt;br /&gt;
Calculation method: RB3LYP&lt;br /&gt;
&lt;br /&gt;
Basis Set = 6-31G(d,p)&lt;br /&gt;
&lt;br /&gt;
Final Energy: E(RB3LYP) = -109.5241268 a.u.&lt;br /&gt;
&lt;br /&gt;
Bond length: 1.1055 Å&lt;br /&gt;
&amp;lt;pre&amp;gt;&lt;br /&gt;
Item               Value     Threshold  Converged?&lt;br /&gt;
 Maximum Force            0.000001     0.000450     YES&lt;br /&gt;
 RMS     Force            0.000001     0.000300     YES&lt;br /&gt;
 Maximum Displacement     0.000000     0.001800     YES&lt;br /&gt;
 RMS     Displacement     0.000000     0.001200     YES&lt;br /&gt;
&amp;lt;/pre&amp;gt;&lt;br /&gt;
&amp;lt;pre&amp;gt;&lt;br /&gt;
Vibrational mode    Frequency    Infrared&lt;br /&gt;
#1             2457.33       0.0000&lt;br /&gt;
&amp;lt;/pre&amp;gt;&lt;br /&gt;
There are no vibrational modes with negative frequencies.&lt;br /&gt;
&lt;br /&gt;
===Calculation of the energy of the Haber-Bosch process===&lt;br /&gt;
N&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; + 3H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; -&amp;gt; 2NH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;&lt;br /&gt;
&lt;br /&gt;
E(NH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;)= -56.557768 a.u.&lt;br /&gt;
&lt;br /&gt;
2*E(NH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;)= -113.115536 a.u.&lt;br /&gt;
&lt;br /&gt;
E(N&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;)= -109.5251268 a.u.&lt;br /&gt;
&lt;br /&gt;
E(H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;)= -1.1785393 a.u.&lt;br /&gt;
&lt;br /&gt;
3*E(H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;)= -3.5359617 a.u.&lt;br /&gt;
&lt;br /&gt;
ΔE= 2*E(NH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;) - [E(N&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;) + 3*E(H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;)] = -145.57 kj/mol&lt;br /&gt;
&lt;br /&gt;
As the reaction is exothermic, the ammonia product is more stable than the gaseous reactants.&lt;br /&gt;
&lt;br /&gt;
The literature value of the Haber-Bosch process is ΔE= -45.8 kj/mol &amp;lt;references/&amp;gt;, which indicates that the process is still exothermic, but the amount of energy released is significantly smaller.&lt;br /&gt;
&lt;br /&gt;
==Analysis of Cl&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;==&lt;br /&gt;
===General Analysis===&lt;br /&gt;
Calculation method: RB3LYP&lt;br /&gt;
&lt;br /&gt;
Basis Set = 6-31G(d,p)&lt;br /&gt;
&lt;br /&gt;
Final Energy: E(RB3LYP) = -920.3498788 a.u.&lt;br /&gt;
&lt;br /&gt;
Bond length: 2.0417 Å&lt;br /&gt;
===Vibrational Analysis===&lt;br /&gt;
&amp;lt;pre&amp;gt;&lt;br /&gt;
 Item               Value     Threshold  Converged?&lt;br /&gt;
 Maximum Force            0.000043     0.000450     YES&lt;br /&gt;
 RMS     Force            0.000043     0.000300     YES&lt;br /&gt;
 Maximum Displacement     0.000121     0.001800     YES&lt;br /&gt;
 RMS     Displacement     0.000172     0.001200     YES&lt;br /&gt;
&lt;br /&gt;
&amp;lt;/pre&amp;gt;&lt;br /&gt;
&amp;lt;pre&amp;gt;&lt;br /&gt;
Vibrational mode    Frequency    Infrared&lt;br /&gt;
#1             520.32       0.0000&lt;br /&gt;
&amp;lt;/pre&amp;gt;&lt;br /&gt;
There are no vibrational modes with negative frequencies&lt;br /&gt;
===Charge Analysis===&lt;br /&gt;
[[File:Adrian_Popescu_Cl2_Charges2.png|400px|center|thumb|Charge distribution of Cl&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;]]&lt;br /&gt;
As the Cl&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; molecule is made up of identical Cl atoms, the bond between them will be 100% covalent, the electrons that form the sigma bond are equally shared between the Cl atoms, so the charge on each Cl atom is zero.&lt;br /&gt;
&lt;br /&gt;
===Molecular orbitals Analysis===&lt;br /&gt;
[[File:orbital1_.png|400px|thumb|center|2σ&amp;lt;sub&amp;gt;g&amp;lt;/sub&amp;gt; bonding orbital]]&lt;br /&gt;
The 2σ&amp;lt;sub&amp;gt;g&amp;lt;/sub&amp;gt; bonding orbital is deep in energy, occupied, and corresponds to the bonding orbital formed by the 2s AOs of the Cl atoms.&lt;br /&gt;
[[File:Adrian_Popescu_orbital2.png|400px|thumb|center|2σ&amp;lt;sub&amp;gt;u*&amp;lt;/sub&amp;gt; antibonding orbital]]&lt;br /&gt;
The 2σ&amp;lt;sub&amp;gt;u*&amp;lt;/sub&amp;gt; orbital is higher in energy than the 2σ&amp;lt;sub&amp;gt;g&amp;lt;/sub&amp;gt; orbital, is occupied, and corresponds to the antibonding orbital formed by the 2s AOs of the Cl atoms.&lt;br /&gt;
[[File:Adrian_Popescu_orbital3.png|400px|thumb|center|3σ&amp;lt;sub&amp;gt;g&amp;lt;/sub&amp;gt; bonding orbital]]&lt;br /&gt;
The 3σ&amp;lt;sub&amp;gt;g&amp;lt;/sub&amp;gt; orbital is deep in energy, occupied, and corresponds to the bonding orbital formed by the 3p&amp;lt;sub&amp;gt;x&amp;lt;/sub&amp;gt; AOs of the Cl atoms.&lt;br /&gt;
[[File:Adrian_Popescu_homo.png|400px|thumb|center|1π&amp;lt;sub&amp;gt;g*&amp;lt;/sub&amp;gt; antibonding orbital]]&lt;br /&gt;
The 1π&amp;lt;sub&amp;gt;g*&amp;lt;/sub&amp;gt; orbital is high in energy, and is the HOMO (Highest Occupied Molecular Orbital). It corresponds to the antibonding orbital formed by the 3p&amp;lt;sub&amp;gt;y&amp;lt;/sub&amp;gt; (or 3p&amp;lt;sub&amp;gt;z&amp;lt;/sub&amp;gt;, as the orbitals are degenerate) AOs of the Cl atoms.&lt;br /&gt;
[[File:Adrian_Popescu_lumo.png|400px|thumb|center|3σ&amp;lt;sub&amp;gt;u*&amp;lt;/sub&amp;gt; antibonding orbital]]&lt;br /&gt;
The 3σ&amp;lt;sub&amp;gt;u*&amp;lt;/sub&amp;gt; orbital is high in energy, and is the LUMO (Lowest Unoccupied Molecular Orbital). It corresponds to the antibonding orbital formed by the 3p&amp;lt;sub&amp;gt;x&amp;lt;/sub&amp;gt; AOs of the Cl atoms.&lt;/div&gt;</summary>
		<author><name>Ap5817</name></author>
	</entry>
	<entry>
		<id>https://chemwiki.ch.ic.ac.uk/index.php?title=User:Ap5817&amp;diff=680659</id>
		<title>User:Ap5817</title>
		<link rel="alternate" type="text/html" href="https://chemwiki.ch.ic.ac.uk/index.php?title=User:Ap5817&amp;diff=680659"/>
		<updated>2018-03-08T16:23:39Z</updated>

		<summary type="html">&lt;p&gt;Ap5817: /* Charge Analysis */&lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;== NH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt; molecule ==&lt;br /&gt;
=== NH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt; calculations ===&lt;br /&gt;
Calculation method:RB3LYP&lt;br /&gt;
&lt;br /&gt;
Basis Set = 6-31G(d,p)&lt;br /&gt;
&lt;br /&gt;
Final Energy: E(RB3LYP) = -56.557768 a.u.&lt;br /&gt;
&lt;br /&gt;
Bond length:1.01789 Å&lt;br /&gt;
&lt;br /&gt;
Bond angle: 105.741 °C&lt;br /&gt;
&lt;br /&gt;
Point Group: C3v&amp;lt;pre&amp;gt;&lt;br /&gt;
Item               Value     Threshold  Converged?&lt;br /&gt;
 Maximum Force            0.000004     0.000450     YES&lt;br /&gt;
 RMS     Force            0.000004     0.000300     YES&lt;br /&gt;
 Maximum Displacement     0.000072     0.001800     YES&lt;br /&gt;
 RMS     Displacement     0.000035     0.001200     YES&lt;br /&gt;
&amp;lt;/pre&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&amp;lt;jmol&amp;gt;&amp;lt;jmolApplet&amp;gt;&lt;br /&gt;
&amp;lt;script&amp;gt;frame x.y&amp;lt;/script&amp;gt;&lt;br /&gt;
  &amp;lt;title&amp;gt;test molecule&amp;lt;/title&amp;gt;&lt;br /&gt;
  &amp;lt;color&amp;gt;black&amp;lt;/color&amp;gt;&lt;br /&gt;
  &amp;lt;size&amp;gt;200&amp;lt;/size&amp;gt;&lt;br /&gt;
  &amp;lt;uploadedFileContents&amp;gt;ADRIAN_POPESCU_PHUNT_NH3_OPTF_POP.LOG&amp;lt;/uploadedFileContents&amp;gt;&lt;br /&gt;
&amp;lt;/jmolApplet&amp;gt;&amp;lt;/jmol&amp;gt;&lt;br /&gt;
&lt;br /&gt;
[[Media:ADRIAN_POPESCU_PHUNT_NH3_OPTF_POP.LOG]]&lt;br /&gt;
&lt;br /&gt;
==Vibration analysis of NH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;==&lt;br /&gt;
[[File:Adrian_Popescu_Vibrations3.png|400px|thumb|Vibrational modes of NH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;|centre]]&lt;br /&gt;
===Vibrational modes===&lt;br /&gt;
Number of vibrational modes: 6&lt;br /&gt;
&lt;br /&gt;
Number of degenerate modes: 4 (2 pairs of degenerate vibrational modes )&lt;br /&gt;
&lt;br /&gt;
Number of bending motions: 3&lt;br /&gt;
&lt;br /&gt;
Number of stretching motions: 3&lt;br /&gt;
&lt;br /&gt;
The most symmetric vibrational mode: mode #4&lt;br /&gt;
&lt;br /&gt;
The &#039;&#039;umbrella mode&#039;&#039;: mode #1&lt;br /&gt;
&lt;br /&gt;
Number of bands expected to be seen in an experimental spectrum of gaseous ammonia: 5&lt;br /&gt;
===Charge Analysis===&lt;br /&gt;
[[File:Adrian_Popescu_Charges2.png|400px|center|thumb|Charge distribution of NH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;]]&lt;br /&gt;
&lt;br /&gt;
Charge on the N atom: -1.125&lt;br /&gt;
&lt;br /&gt;
Charge on the H atom: 0.375&lt;br /&gt;
&lt;br /&gt;
As Nitrogen has an electronegativity value of 3.04, which is significantly larger than the one of Hidrogen (2.2), it is expected that on the Nitrogen there will be a negative charge and on Hidrogen a possitive charge.&lt;br /&gt;
&lt;br /&gt;
==Reactivity of the Haber-Bosch process==&lt;br /&gt;
===Analysis of H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;===&lt;br /&gt;
Calculation method: RB3LYP&lt;br /&gt;
&lt;br /&gt;
Basis Set = 6-31G(d,p)&lt;br /&gt;
&lt;br /&gt;
Final Energy: E(RB3LYP) = -1.1785393 a.u.&lt;br /&gt;
&lt;br /&gt;
Bond length: 0.7428 Å&lt;br /&gt;
&amp;lt;pre&amp;gt;&lt;br /&gt;
Item               Value     Threshold  Converged?&lt;br /&gt;
 Maximum Force            0.000004     0.000450     YES&lt;br /&gt;
 RMS     Force            0.000004     0.000300     YES&lt;br /&gt;
 Maximum Displacement     0.000005     0.001800     YES&lt;br /&gt;
 RMS     Displacement     0.000007     0.001200     YES&amp;lt;/pre&amp;gt;&lt;br /&gt;
&amp;lt;pre&amp;gt;&lt;br /&gt;
Vibrational mode    Frequency    Infrared&lt;br /&gt;
#1             4465.6       0.0000&lt;br /&gt;
&amp;lt;/pre&amp;gt;&lt;br /&gt;
There are no vibrational modes with negative frequencies&lt;br /&gt;
&lt;br /&gt;
===Analysis of N&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;===&lt;br /&gt;
Calculation method: RB3LYP&lt;br /&gt;
&lt;br /&gt;
Basis Set = 6-31G(d,p)&lt;br /&gt;
&lt;br /&gt;
Final Energy: E(RB3LYP) = -109.5241268 a.u.&lt;br /&gt;
&lt;br /&gt;
Bond length: 1.1055 Å&lt;br /&gt;
&amp;lt;pre&amp;gt;&lt;br /&gt;
Item               Value     Threshold  Converged?&lt;br /&gt;
 Maximum Force            0.000001     0.000450     YES&lt;br /&gt;
 RMS     Force            0.000001     0.000300     YES&lt;br /&gt;
 Maximum Displacement     0.000000     0.001800     YES&lt;br /&gt;
 RMS     Displacement     0.000000     0.001200     YES&lt;br /&gt;
&amp;lt;/pre&amp;gt;&lt;br /&gt;
&amp;lt;pre&amp;gt;&lt;br /&gt;
Vibrational mode    Frequency    Infrared&lt;br /&gt;
#1             2457.33       0.0000&lt;br /&gt;
&amp;lt;/pre&amp;gt;&lt;br /&gt;
There are no vibrational modes with negative frequencies.&lt;br /&gt;
&lt;br /&gt;
===Calculation of the energy of the Haber-Bosch process===&lt;br /&gt;
N&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; + 3H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; -&amp;gt; 2NH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;&lt;br /&gt;
&lt;br /&gt;
E(NH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;)= -56.557768 a.u.&lt;br /&gt;
&lt;br /&gt;
2*E(NH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;)= -113.115536 a.u.&lt;br /&gt;
&lt;br /&gt;
E(N&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;)= -109.5251268 a.u.&lt;br /&gt;
&lt;br /&gt;
E(H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;)= -1.1785393 a.u.&lt;br /&gt;
&lt;br /&gt;
3*E(H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;)= -3.5359617 a.u.&lt;br /&gt;
&lt;br /&gt;
ΔE= 2*E(NH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;) - [E(N&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;) + 3*E(H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;)] = -145.57 kj/mol&lt;br /&gt;
&lt;br /&gt;
As the reaction is exothermic, the ammonia product is more stable than the gaseous reactants.&lt;br /&gt;
&lt;br /&gt;
==Analysis of Cl&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;==&lt;br /&gt;
===General Analysis===&lt;br /&gt;
Calculation method: RB3LYP&lt;br /&gt;
&lt;br /&gt;
Basis Set = 6-31G(d,p)&lt;br /&gt;
&lt;br /&gt;
Final Energy: E(RB3LYP) = -920.3498788 a.u.&lt;br /&gt;
&lt;br /&gt;
Bond length: 2.0417 Å&lt;br /&gt;
===Vibrational Analysis===&lt;br /&gt;
&amp;lt;pre&amp;gt;&lt;br /&gt;
 Item               Value     Threshold  Converged?&lt;br /&gt;
 Maximum Force            0.000043     0.000450     YES&lt;br /&gt;
 RMS     Force            0.000043     0.000300     YES&lt;br /&gt;
 Maximum Displacement     0.000121     0.001800     YES&lt;br /&gt;
 RMS     Displacement     0.000172     0.001200     YES&lt;br /&gt;
&lt;br /&gt;
&amp;lt;/pre&amp;gt;&lt;br /&gt;
&amp;lt;pre&amp;gt;&lt;br /&gt;
Vibrational mode    Frequency    Infrared&lt;br /&gt;
#1             520.32       0.0000&lt;br /&gt;
&amp;lt;/pre&amp;gt;&lt;br /&gt;
There are no vibrational modes with negative frequencies&lt;br /&gt;
===Charge Analysis===&lt;br /&gt;
[[File:Adrian_Popescu_Cl2_Charges2.png|400px|center|thumb|Charge distribution of Cl&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;]]&lt;br /&gt;
As the Cl&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; molecule is made up of identical Cl atoms, the bond between them will be 100% covalent, the electrons that form the sigma bond are equally shared between the Cl atoms, so the charge on each Cl atom is zero.&lt;br /&gt;
&lt;br /&gt;
===Molecular orbitals Analysis===&lt;br /&gt;
[[File:orbital1_.png|400px|thumb|center|2σ&amp;lt;sub&amp;gt;g&amp;lt;/sub&amp;gt; bonding orbital]]&lt;br /&gt;
The 2σ&amp;lt;sub&amp;gt;g&amp;lt;/sub&amp;gt; bonding orbital is deep in energy, occupied, and corresponds to the bonding orbital formed by the 2s AOs of the Cl atoms.&lt;br /&gt;
[[File:Adrian_Popescu_orbital2.png|400px|thumb|center|2σ&amp;lt;sub&amp;gt;u*&amp;lt;/sub&amp;gt; antibonding orbital]]&lt;br /&gt;
The 2σ&amp;lt;sub&amp;gt;u*&amp;lt;/sub&amp;gt; orbital is higher in energy than the 2σ&amp;lt;sub&amp;gt;g&amp;lt;/sub&amp;gt; orbital, is occupied, and corresponds to the antibonding orbital formed by the 2s AOs of the Cl atoms.&lt;br /&gt;
[[File:Adrian_Popescu_orbital3.png|400px|thumb|center|3σ&amp;lt;sub&amp;gt;g&amp;lt;/sub&amp;gt; bonding orbital]]&lt;br /&gt;
The 3σ&amp;lt;sub&amp;gt;g&amp;lt;/sub&amp;gt; orbital is deep in energy, occupied, and corresponds to the bonding orbital formed by the 3p&amp;lt;sub&amp;gt;x&amp;lt;/sub&amp;gt; AOs of the Cl atoms.&lt;br /&gt;
[[File:Adrian_Popescu_homo.png|400px|thumb|center|1π&amp;lt;sub&amp;gt;g*&amp;lt;/sub&amp;gt; antibonding orbital]]&lt;br /&gt;
The 1π&amp;lt;sub&amp;gt;g*&amp;lt;/sub&amp;gt; orbital is high in energy, and is the HOMO (Highest Occupied Molecular Orbital). It corresponds to the antibonding orbital formed by the 3p&amp;lt;sub&amp;gt;y&amp;lt;/sub&amp;gt; (or 3p&amp;lt;sub&amp;gt;z&amp;lt;/sub&amp;gt;, as the orbitals are degenerate) AOs of the Cl atoms.&lt;br /&gt;
[[File:Adrian_Popescu_lumo.png|400px|thumb|center|3σ&amp;lt;sub&amp;gt;u*&amp;lt;/sub&amp;gt; antibonding orbital]]&lt;br /&gt;
The 3σ&amp;lt;sub&amp;gt;u*&amp;lt;/sub&amp;gt; orbital is high in energy, and is the LUMO (Lowest Unoccupied Molecular Orbital). It corresponds to the antibonding orbital formed by the 3p&amp;lt;sub&amp;gt;x&amp;lt;/sub&amp;gt; AOs of the Cl atoms.&lt;/div&gt;</summary>
		<author><name>Ap5817</name></author>
	</entry>
	<entry>
		<id>https://chemwiki.ch.ic.ac.uk/index.php?title=User:Ap5817&amp;diff=680658</id>
		<title>User:Ap5817</title>
		<link rel="alternate" type="text/html" href="https://chemwiki.ch.ic.ac.uk/index.php?title=User:Ap5817&amp;diff=680658"/>
		<updated>2018-03-08T16:23:25Z</updated>

		<summary type="html">&lt;p&gt;Ap5817: /* Charge Analysis */&lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;== NH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt; molecule ==&lt;br /&gt;
=== NH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt; calculations ===&lt;br /&gt;
Calculation method:RB3LYP&lt;br /&gt;
&lt;br /&gt;
Basis Set = 6-31G(d,p)&lt;br /&gt;
&lt;br /&gt;
Final Energy: E(RB3LYP) = -56.557768 a.u.&lt;br /&gt;
&lt;br /&gt;
Bond length:1.01789 Å&lt;br /&gt;
&lt;br /&gt;
Bond angle: 105.741 °C&lt;br /&gt;
&lt;br /&gt;
Point Group: C3v&amp;lt;pre&amp;gt;&lt;br /&gt;
Item               Value     Threshold  Converged?&lt;br /&gt;
 Maximum Force            0.000004     0.000450     YES&lt;br /&gt;
 RMS     Force            0.000004     0.000300     YES&lt;br /&gt;
 Maximum Displacement     0.000072     0.001800     YES&lt;br /&gt;
 RMS     Displacement     0.000035     0.001200     YES&lt;br /&gt;
&amp;lt;/pre&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&amp;lt;jmol&amp;gt;&amp;lt;jmolApplet&amp;gt;&lt;br /&gt;
&amp;lt;script&amp;gt;frame x.y&amp;lt;/script&amp;gt;&lt;br /&gt;
  &amp;lt;title&amp;gt;test molecule&amp;lt;/title&amp;gt;&lt;br /&gt;
  &amp;lt;color&amp;gt;black&amp;lt;/color&amp;gt;&lt;br /&gt;
  &amp;lt;size&amp;gt;200&amp;lt;/size&amp;gt;&lt;br /&gt;
  &amp;lt;uploadedFileContents&amp;gt;ADRIAN_POPESCU_PHUNT_NH3_OPTF_POP.LOG&amp;lt;/uploadedFileContents&amp;gt;&lt;br /&gt;
&amp;lt;/jmolApplet&amp;gt;&amp;lt;/jmol&amp;gt;&lt;br /&gt;
&lt;br /&gt;
[[Media:ADRIAN_POPESCU_PHUNT_NH3_OPTF_POP.LOG]]&lt;br /&gt;
&lt;br /&gt;
==Vibration analysis of NH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;==&lt;br /&gt;
[[File:Adrian_Popescu_Vibrations3.png|400px|thumb|Vibrational modes of NH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;|centre]]&lt;br /&gt;
===Vibrational modes===&lt;br /&gt;
Number of vibrational modes: 6&lt;br /&gt;
&lt;br /&gt;
Number of degenerate modes: 4 (2 pairs of degenerate vibrational modes )&lt;br /&gt;
&lt;br /&gt;
Number of bending motions: 3&lt;br /&gt;
&lt;br /&gt;
Number of stretching motions: 3&lt;br /&gt;
&lt;br /&gt;
The most symmetric vibrational mode: mode #4&lt;br /&gt;
&lt;br /&gt;
The &#039;&#039;umbrella mode&#039;&#039;: mode #1&lt;br /&gt;
&lt;br /&gt;
Number of bands expected to be seen in an experimental spectrum of gaseous ammonia: 5&lt;br /&gt;
===Charge Analysis===&lt;br /&gt;
[[File:Adrian_Popescu_Charges2.png|400px|center|thumb|Charges distribution of NH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;]]&lt;br /&gt;
&lt;br /&gt;
Charge on the N atom: -1.125&lt;br /&gt;
&lt;br /&gt;
Charge on the H atom: 0.375&lt;br /&gt;
&lt;br /&gt;
As Nitrogen has an electronegativity value of 3.04, which is significantly larger than the one of Hidrogen (2.2), it is expected that on the Nitrogen there will be a negative charge and on Hidrogen a possitive charge.&lt;br /&gt;
&lt;br /&gt;
==Reactivity of the Haber-Bosch process==&lt;br /&gt;
===Analysis of H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;===&lt;br /&gt;
Calculation method: RB3LYP&lt;br /&gt;
&lt;br /&gt;
Basis Set = 6-31G(d,p)&lt;br /&gt;
&lt;br /&gt;
Final Energy: E(RB3LYP) = -1.1785393 a.u.&lt;br /&gt;
&lt;br /&gt;
Bond length: 0.7428 Å&lt;br /&gt;
&amp;lt;pre&amp;gt;&lt;br /&gt;
Item               Value     Threshold  Converged?&lt;br /&gt;
 Maximum Force            0.000004     0.000450     YES&lt;br /&gt;
 RMS     Force            0.000004     0.000300     YES&lt;br /&gt;
 Maximum Displacement     0.000005     0.001800     YES&lt;br /&gt;
 RMS     Displacement     0.000007     0.001200     YES&amp;lt;/pre&amp;gt;&lt;br /&gt;
&amp;lt;pre&amp;gt;&lt;br /&gt;
Vibrational mode    Frequency    Infrared&lt;br /&gt;
#1             4465.6       0.0000&lt;br /&gt;
&amp;lt;/pre&amp;gt;&lt;br /&gt;
There are no vibrational modes with negative frequencies&lt;br /&gt;
&lt;br /&gt;
===Analysis of N&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;===&lt;br /&gt;
Calculation method: RB3LYP&lt;br /&gt;
&lt;br /&gt;
Basis Set = 6-31G(d,p)&lt;br /&gt;
&lt;br /&gt;
Final Energy: E(RB3LYP) = -109.5241268 a.u.&lt;br /&gt;
&lt;br /&gt;
Bond length: 1.1055 Å&lt;br /&gt;
&amp;lt;pre&amp;gt;&lt;br /&gt;
Item               Value     Threshold  Converged?&lt;br /&gt;
 Maximum Force            0.000001     0.000450     YES&lt;br /&gt;
 RMS     Force            0.000001     0.000300     YES&lt;br /&gt;
 Maximum Displacement     0.000000     0.001800     YES&lt;br /&gt;
 RMS     Displacement     0.000000     0.001200     YES&lt;br /&gt;
&amp;lt;/pre&amp;gt;&lt;br /&gt;
&amp;lt;pre&amp;gt;&lt;br /&gt;
Vibrational mode    Frequency    Infrared&lt;br /&gt;
#1             2457.33       0.0000&lt;br /&gt;
&amp;lt;/pre&amp;gt;&lt;br /&gt;
There are no vibrational modes with negative frequencies.&lt;br /&gt;
&lt;br /&gt;
===Calculation of the energy of the Haber-Bosch process===&lt;br /&gt;
N&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; + 3H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; -&amp;gt; 2NH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;&lt;br /&gt;
&lt;br /&gt;
E(NH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;)= -56.557768 a.u.&lt;br /&gt;
&lt;br /&gt;
2*E(NH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;)= -113.115536 a.u.&lt;br /&gt;
&lt;br /&gt;
E(N&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;)= -109.5251268 a.u.&lt;br /&gt;
&lt;br /&gt;
E(H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;)= -1.1785393 a.u.&lt;br /&gt;
&lt;br /&gt;
3*E(H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;)= -3.5359617 a.u.&lt;br /&gt;
&lt;br /&gt;
ΔE= 2*E(NH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;) - [E(N&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;) + 3*E(H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;)] = -145.57 kj/mol&lt;br /&gt;
&lt;br /&gt;
As the reaction is exothermic, the ammonia product is more stable than the gaseous reactants.&lt;br /&gt;
&lt;br /&gt;
==Analysis of Cl&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;==&lt;br /&gt;
===General Analysis===&lt;br /&gt;
Calculation method: RB3LYP&lt;br /&gt;
&lt;br /&gt;
Basis Set = 6-31G(d,p)&lt;br /&gt;
&lt;br /&gt;
Final Energy: E(RB3LYP) = -920.3498788 a.u.&lt;br /&gt;
&lt;br /&gt;
Bond length: 2.0417 Å&lt;br /&gt;
===Vibrational Analysis===&lt;br /&gt;
&amp;lt;pre&amp;gt;&lt;br /&gt;
 Item               Value     Threshold  Converged?&lt;br /&gt;
 Maximum Force            0.000043     0.000450     YES&lt;br /&gt;
 RMS     Force            0.000043     0.000300     YES&lt;br /&gt;
 Maximum Displacement     0.000121     0.001800     YES&lt;br /&gt;
 RMS     Displacement     0.000172     0.001200     YES&lt;br /&gt;
&lt;br /&gt;
&amp;lt;/pre&amp;gt;&lt;br /&gt;
&amp;lt;pre&amp;gt;&lt;br /&gt;
Vibrational mode    Frequency    Infrared&lt;br /&gt;
#1             520.32       0.0000&lt;br /&gt;
&amp;lt;/pre&amp;gt;&lt;br /&gt;
There are no vibrational modes with negative frequencies&lt;br /&gt;
===Charge Analysis===&lt;br /&gt;
[[File:Adrian_Popescu_Cl2_Charges2.png|400px|center|thumb|Charge distribution of Cl&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;]]&lt;br /&gt;
As the Cl&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; molecule is made up of identical Cl atoms, the bond between them will be 100% covalent, the electrons that form the sigma bond are equally shared between the Cl atoms, so the charge on each Cl atom is zero.&lt;br /&gt;
&lt;br /&gt;
===Molecular orbitals Analysis===&lt;br /&gt;
[[File:orbital1_.png|400px|thumb|center|2σ&amp;lt;sub&amp;gt;g&amp;lt;/sub&amp;gt; bonding orbital]]&lt;br /&gt;
The 2σ&amp;lt;sub&amp;gt;g&amp;lt;/sub&amp;gt; bonding orbital is deep in energy, occupied, and corresponds to the bonding orbital formed by the 2s AOs of the Cl atoms.&lt;br /&gt;
[[File:Adrian_Popescu_orbital2.png|400px|thumb|center|2σ&amp;lt;sub&amp;gt;u*&amp;lt;/sub&amp;gt; antibonding orbital]]&lt;br /&gt;
The 2σ&amp;lt;sub&amp;gt;u*&amp;lt;/sub&amp;gt; orbital is higher in energy than the 2σ&amp;lt;sub&amp;gt;g&amp;lt;/sub&amp;gt; orbital, is occupied, and corresponds to the antibonding orbital formed by the 2s AOs of the Cl atoms.&lt;br /&gt;
[[File:Adrian_Popescu_orbital3.png|400px|thumb|center|3σ&amp;lt;sub&amp;gt;g&amp;lt;/sub&amp;gt; bonding orbital]]&lt;br /&gt;
The 3σ&amp;lt;sub&amp;gt;g&amp;lt;/sub&amp;gt; orbital is deep in energy, occupied, and corresponds to the bonding orbital formed by the 3p&amp;lt;sub&amp;gt;x&amp;lt;/sub&amp;gt; AOs of the Cl atoms.&lt;br /&gt;
[[File:Adrian_Popescu_homo.png|400px|thumb|center|1π&amp;lt;sub&amp;gt;g*&amp;lt;/sub&amp;gt; antibonding orbital]]&lt;br /&gt;
The 1π&amp;lt;sub&amp;gt;g*&amp;lt;/sub&amp;gt; orbital is high in energy, and is the HOMO (Highest Occupied Molecular Orbital). It corresponds to the antibonding orbital formed by the 3p&amp;lt;sub&amp;gt;y&amp;lt;/sub&amp;gt; (or 3p&amp;lt;sub&amp;gt;z&amp;lt;/sub&amp;gt;, as the orbitals are degenerate) AOs of the Cl atoms.&lt;br /&gt;
[[File:Adrian_Popescu_lumo.png|400px|thumb|center|3σ&amp;lt;sub&amp;gt;u*&amp;lt;/sub&amp;gt; antibonding orbital]]&lt;br /&gt;
The 3σ&amp;lt;sub&amp;gt;u*&amp;lt;/sub&amp;gt; orbital is high in energy, and is the LUMO (Lowest Unoccupied Molecular Orbital). It corresponds to the antibonding orbital formed by the 3p&amp;lt;sub&amp;gt;x&amp;lt;/sub&amp;gt; AOs of the Cl atoms.&lt;/div&gt;</summary>
		<author><name>Ap5817</name></author>
	</entry>
	<entry>
		<id>https://chemwiki.ch.ic.ac.uk/index.php?title=User:Ap5817&amp;diff=680657</id>
		<title>User:Ap5817</title>
		<link rel="alternate" type="text/html" href="https://chemwiki.ch.ic.ac.uk/index.php?title=User:Ap5817&amp;diff=680657"/>
		<updated>2018-03-08T16:22:48Z</updated>

		<summary type="html">&lt;p&gt;Ap5817: /* Charge Analysis */&lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;== NH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt; molecule ==&lt;br /&gt;
=== NH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt; calculations ===&lt;br /&gt;
Calculation method:RB3LYP&lt;br /&gt;
&lt;br /&gt;
Basis Set = 6-31G(d,p)&lt;br /&gt;
&lt;br /&gt;
Final Energy: E(RB3LYP) = -56.557768 a.u.&lt;br /&gt;
&lt;br /&gt;
Bond length:1.01789 Å&lt;br /&gt;
&lt;br /&gt;
Bond angle: 105.741 °C&lt;br /&gt;
&lt;br /&gt;
Point Group: C3v&amp;lt;pre&amp;gt;&lt;br /&gt;
Item               Value     Threshold  Converged?&lt;br /&gt;
 Maximum Force            0.000004     0.000450     YES&lt;br /&gt;
 RMS     Force            0.000004     0.000300     YES&lt;br /&gt;
 Maximum Displacement     0.000072     0.001800     YES&lt;br /&gt;
 RMS     Displacement     0.000035     0.001200     YES&lt;br /&gt;
&amp;lt;/pre&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&amp;lt;jmol&amp;gt;&amp;lt;jmolApplet&amp;gt;&lt;br /&gt;
&amp;lt;script&amp;gt;frame x.y&amp;lt;/script&amp;gt;&lt;br /&gt;
  &amp;lt;title&amp;gt;test molecule&amp;lt;/title&amp;gt;&lt;br /&gt;
  &amp;lt;color&amp;gt;black&amp;lt;/color&amp;gt;&lt;br /&gt;
  &amp;lt;size&amp;gt;200&amp;lt;/size&amp;gt;&lt;br /&gt;
  &amp;lt;uploadedFileContents&amp;gt;ADRIAN_POPESCU_PHUNT_NH3_OPTF_POP.LOG&amp;lt;/uploadedFileContents&amp;gt;&lt;br /&gt;
&amp;lt;/jmolApplet&amp;gt;&amp;lt;/jmol&amp;gt;&lt;br /&gt;
&lt;br /&gt;
[[Media:ADRIAN_POPESCU_PHUNT_NH3_OPTF_POP.LOG]]&lt;br /&gt;
&lt;br /&gt;
==Vibration analysis of NH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;==&lt;br /&gt;
[[File:Adrian_Popescu_Vibrations3.png|400px|thumb|Vibrational modes of NH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;|centre]]&lt;br /&gt;
===Vibrational modes===&lt;br /&gt;
Number of vibrational modes: 6&lt;br /&gt;
&lt;br /&gt;
Number of degenerate modes: 4 (2 pairs of degenerate vibrational modes )&lt;br /&gt;
&lt;br /&gt;
Number of bending motions: 3&lt;br /&gt;
&lt;br /&gt;
Number of stretching motions: 3&lt;br /&gt;
&lt;br /&gt;
The most symmetric vibrational mode: mode #4&lt;br /&gt;
&lt;br /&gt;
The &#039;&#039;umbrella mode&#039;&#039;: mode #1&lt;br /&gt;
&lt;br /&gt;
Number of bands expected to be seen in an experimental spectrum of gaseous ammonia: 5&lt;br /&gt;
===Charge Analysis===&lt;br /&gt;
[[File:Adrian_Popescu_Charges2.png|400px|center|thumb|Charges distribution of NH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;]]&lt;br /&gt;
&lt;br /&gt;
Charge on the N atom: -1.125&lt;br /&gt;
&lt;br /&gt;
Charge on the H atom: 0.375&lt;br /&gt;
&lt;br /&gt;
As Nitrogen has an electronegativity value of 3.04, which is significantly larger than the one of Hidrogen (2.2), it is expected that on the Nitrogen there will be a negative charge and on Hidrogen a possitive charge.&lt;br /&gt;
&lt;br /&gt;
==Reactivity of the Haber-Bosch process==&lt;br /&gt;
===Analysis of H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;===&lt;br /&gt;
Calculation method: RB3LYP&lt;br /&gt;
&lt;br /&gt;
Basis Set = 6-31G(d,p)&lt;br /&gt;
&lt;br /&gt;
Final Energy: E(RB3LYP) = -1.1785393 a.u.&lt;br /&gt;
&lt;br /&gt;
Bond length: 0.7428 Å&lt;br /&gt;
&amp;lt;pre&amp;gt;&lt;br /&gt;
Item               Value     Threshold  Converged?&lt;br /&gt;
 Maximum Force            0.000004     0.000450     YES&lt;br /&gt;
 RMS     Force            0.000004     0.000300     YES&lt;br /&gt;
 Maximum Displacement     0.000005     0.001800     YES&lt;br /&gt;
 RMS     Displacement     0.000007     0.001200     YES&amp;lt;/pre&amp;gt;&lt;br /&gt;
&amp;lt;pre&amp;gt;&lt;br /&gt;
Vibrational mode    Frequency    Infrared&lt;br /&gt;
#1             4465.6       0.0000&lt;br /&gt;
&amp;lt;/pre&amp;gt;&lt;br /&gt;
There are no vibrational modes with negative frequencies&lt;br /&gt;
&lt;br /&gt;
===Analysis of N&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;===&lt;br /&gt;
Calculation method: RB3LYP&lt;br /&gt;
&lt;br /&gt;
Basis Set = 6-31G(d,p)&lt;br /&gt;
&lt;br /&gt;
Final Energy: E(RB3LYP) = -109.5241268 a.u.&lt;br /&gt;
&lt;br /&gt;
Bond length: 1.1055 Å&lt;br /&gt;
&amp;lt;pre&amp;gt;&lt;br /&gt;
Item               Value     Threshold  Converged?&lt;br /&gt;
 Maximum Force            0.000001     0.000450     YES&lt;br /&gt;
 RMS     Force            0.000001     0.000300     YES&lt;br /&gt;
 Maximum Displacement     0.000000     0.001800     YES&lt;br /&gt;
 RMS     Displacement     0.000000     0.001200     YES&lt;br /&gt;
&amp;lt;/pre&amp;gt;&lt;br /&gt;
&amp;lt;pre&amp;gt;&lt;br /&gt;
Vibrational mode    Frequency    Infrared&lt;br /&gt;
#1             2457.33       0.0000&lt;br /&gt;
&amp;lt;/pre&amp;gt;&lt;br /&gt;
There are no vibrational modes with negative frequencies.&lt;br /&gt;
&lt;br /&gt;
===Calculation of the energy of the Haber-Bosch process===&lt;br /&gt;
N&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; + 3H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; -&amp;gt; 2NH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;&lt;br /&gt;
&lt;br /&gt;
E(NH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;)= -56.557768 a.u.&lt;br /&gt;
&lt;br /&gt;
2*E(NH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;)= -113.115536 a.u.&lt;br /&gt;
&lt;br /&gt;
E(N&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;)= -109.5251268 a.u.&lt;br /&gt;
&lt;br /&gt;
E(H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;)= -1.1785393 a.u.&lt;br /&gt;
&lt;br /&gt;
3*E(H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;)= -3.5359617 a.u.&lt;br /&gt;
&lt;br /&gt;
ΔE= 2*E(NH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;) - [E(N&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;) + 3*E(H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;)] = -145.57 kj/mol&lt;br /&gt;
&lt;br /&gt;
As the reaction is exothermic, the ammonia product is more stable than the gaseous reactants.&lt;br /&gt;
&lt;br /&gt;
==Analysis of Cl&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;==&lt;br /&gt;
===General Analysis===&lt;br /&gt;
Calculation method: RB3LYP&lt;br /&gt;
&lt;br /&gt;
Basis Set = 6-31G(d,p)&lt;br /&gt;
&lt;br /&gt;
Final Energy: E(RB3LYP) = -920.3498788 a.u.&lt;br /&gt;
&lt;br /&gt;
Bond length: 2.0417 Å&lt;br /&gt;
===Vibrational Analysis===&lt;br /&gt;
&amp;lt;pre&amp;gt;&lt;br /&gt;
 Item               Value     Threshold  Converged?&lt;br /&gt;
 Maximum Force            0.000043     0.000450     YES&lt;br /&gt;
 RMS     Force            0.000043     0.000300     YES&lt;br /&gt;
 Maximum Displacement     0.000121     0.001800     YES&lt;br /&gt;
 RMS     Displacement     0.000172     0.001200     YES&lt;br /&gt;
&lt;br /&gt;
&amp;lt;/pre&amp;gt;&lt;br /&gt;
&amp;lt;pre&amp;gt;&lt;br /&gt;
Vibrational mode    Frequency    Infrared&lt;br /&gt;
#1             520.32       0.0000&lt;br /&gt;
&amp;lt;/pre&amp;gt;&lt;br /&gt;
There are no vibrational modes with negative frequencies&lt;br /&gt;
===Charge Analysis===&lt;br /&gt;
[[File:Adrian_Popescu_Cl2_Charges2.png|400px|center]]&lt;br /&gt;
As the Cl&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; molecule is made up of identical Cl atoms, the bond between them will be 100% covalent, the electrons that form the sigma bond are equally shared between the Cl atoms, so the charge on each Cl atom is zero.&lt;br /&gt;
&lt;br /&gt;
===Molecular orbitals Analysis===&lt;br /&gt;
[[File:orbital1_.png|400px|thumb|center|2σ&amp;lt;sub&amp;gt;g&amp;lt;/sub&amp;gt; bonding orbital]]&lt;br /&gt;
The 2σ&amp;lt;sub&amp;gt;g&amp;lt;/sub&amp;gt; bonding orbital is deep in energy, occupied, and corresponds to the bonding orbital formed by the 2s AOs of the Cl atoms.&lt;br /&gt;
[[File:Adrian_Popescu_orbital2.png|400px|thumb|center|2σ&amp;lt;sub&amp;gt;u*&amp;lt;/sub&amp;gt; antibonding orbital]]&lt;br /&gt;
The 2σ&amp;lt;sub&amp;gt;u*&amp;lt;/sub&amp;gt; orbital is higher in energy than the 2σ&amp;lt;sub&amp;gt;g&amp;lt;/sub&amp;gt; orbital, is occupied, and corresponds to the antibonding orbital formed by the 2s AOs of the Cl atoms.&lt;br /&gt;
[[File:Adrian_Popescu_orbital3.png|400px|thumb|center|3σ&amp;lt;sub&amp;gt;g&amp;lt;/sub&amp;gt; bonding orbital]]&lt;br /&gt;
The 3σ&amp;lt;sub&amp;gt;g&amp;lt;/sub&amp;gt; orbital is deep in energy, occupied, and corresponds to the bonding orbital formed by the 3p&amp;lt;sub&amp;gt;x&amp;lt;/sub&amp;gt; AOs of the Cl atoms.&lt;br /&gt;
[[File:Adrian_Popescu_homo.png|400px|thumb|center|1π&amp;lt;sub&amp;gt;g*&amp;lt;/sub&amp;gt; antibonding orbital]]&lt;br /&gt;
The 1π&amp;lt;sub&amp;gt;g*&amp;lt;/sub&amp;gt; orbital is high in energy, and is the HOMO (Highest Occupied Molecular Orbital). It corresponds to the antibonding orbital formed by the 3p&amp;lt;sub&amp;gt;y&amp;lt;/sub&amp;gt; (or 3p&amp;lt;sub&amp;gt;z&amp;lt;/sub&amp;gt;, as the orbitals are degenerate) AOs of the Cl atoms.&lt;br /&gt;
[[File:Adrian_Popescu_lumo.png|400px|thumb|center|3σ&amp;lt;sub&amp;gt;u*&amp;lt;/sub&amp;gt; antibonding orbital]]&lt;br /&gt;
The 3σ&amp;lt;sub&amp;gt;u*&amp;lt;/sub&amp;gt; orbital is high in energy, and is the LUMO (Lowest Unoccupied Molecular Orbital). It corresponds to the antibonding orbital formed by the 3p&amp;lt;sub&amp;gt;x&amp;lt;/sub&amp;gt; AOs of the Cl atoms.&lt;/div&gt;</summary>
		<author><name>Ap5817</name></author>
	</entry>
	<entry>
		<id>https://chemwiki.ch.ic.ac.uk/index.php?title=User:Ap5817&amp;diff=680655</id>
		<title>User:Ap5817</title>
		<link rel="alternate" type="text/html" href="https://chemwiki.ch.ic.ac.uk/index.php?title=User:Ap5817&amp;diff=680655"/>
		<updated>2018-03-08T16:21:56Z</updated>

		<summary type="html">&lt;p&gt;Ap5817: /* Vibration analysis of NH3 */&lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;== NH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt; molecule ==&lt;br /&gt;
=== NH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt; calculations ===&lt;br /&gt;
Calculation method:RB3LYP&lt;br /&gt;
&lt;br /&gt;
Basis Set = 6-31G(d,p)&lt;br /&gt;
&lt;br /&gt;
Final Energy: E(RB3LYP) = -56.557768 a.u.&lt;br /&gt;
&lt;br /&gt;
Bond length:1.01789 Å&lt;br /&gt;
&lt;br /&gt;
Bond angle: 105.741 °C&lt;br /&gt;
&lt;br /&gt;
Point Group: C3v&amp;lt;pre&amp;gt;&lt;br /&gt;
Item               Value     Threshold  Converged?&lt;br /&gt;
 Maximum Force            0.000004     0.000450     YES&lt;br /&gt;
 RMS     Force            0.000004     0.000300     YES&lt;br /&gt;
 Maximum Displacement     0.000072     0.001800     YES&lt;br /&gt;
 RMS     Displacement     0.000035     0.001200     YES&lt;br /&gt;
&amp;lt;/pre&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&amp;lt;jmol&amp;gt;&amp;lt;jmolApplet&amp;gt;&lt;br /&gt;
&amp;lt;script&amp;gt;frame x.y&amp;lt;/script&amp;gt;&lt;br /&gt;
  &amp;lt;title&amp;gt;test molecule&amp;lt;/title&amp;gt;&lt;br /&gt;
  &amp;lt;color&amp;gt;black&amp;lt;/color&amp;gt;&lt;br /&gt;
  &amp;lt;size&amp;gt;200&amp;lt;/size&amp;gt;&lt;br /&gt;
  &amp;lt;uploadedFileContents&amp;gt;ADRIAN_POPESCU_PHUNT_NH3_OPTF_POP.LOG&amp;lt;/uploadedFileContents&amp;gt;&lt;br /&gt;
&amp;lt;/jmolApplet&amp;gt;&amp;lt;/jmol&amp;gt;&lt;br /&gt;
&lt;br /&gt;
[[Media:ADRIAN_POPESCU_PHUNT_NH3_OPTF_POP.LOG]]&lt;br /&gt;
&lt;br /&gt;
==Vibration analysis of NH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;==&lt;br /&gt;
[[File:Adrian_Popescu_Vibrations3.png|400px|thumb|Vibrational modes of NH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;|centre]]&lt;br /&gt;
===Vibrational modes===&lt;br /&gt;
Number of vibrational modes: 6&lt;br /&gt;
&lt;br /&gt;
Number of degenerate modes: 4 (2 pairs of degenerate vibrational modes )&lt;br /&gt;
&lt;br /&gt;
Number of bending motions: 3&lt;br /&gt;
&lt;br /&gt;
Number of stretching motions: 3&lt;br /&gt;
&lt;br /&gt;
The most symmetric vibrational mode: mode #4&lt;br /&gt;
&lt;br /&gt;
The &#039;&#039;umbrella mode&#039;&#039;: mode #1&lt;br /&gt;
&lt;br /&gt;
Number of bands expected to be seen in an experimental spectrum of gaseous ammonia: 5&lt;br /&gt;
===Charge Analysis===&lt;br /&gt;
[[File:Adrian_Popescu_Charges2.png|400px|center]]&lt;br /&gt;
&lt;br /&gt;
Charge on the N atom: -1.125&lt;br /&gt;
&lt;br /&gt;
Charge on the H atom: 0.375&lt;br /&gt;
&lt;br /&gt;
As Nitrogen has an electronegativity value of 3.04, which is significantly larger than the one of Hidrogen (2.2), it is expected that on the Nitrogen there will be a negative charge and on Hidrogen a possitive charge.&lt;br /&gt;
&lt;br /&gt;
==Reactivity of the Haber-Bosch process==&lt;br /&gt;
===Analysis of H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;===&lt;br /&gt;
Calculation method: RB3LYP&lt;br /&gt;
&lt;br /&gt;
Basis Set = 6-31G(d,p)&lt;br /&gt;
&lt;br /&gt;
Final Energy: E(RB3LYP) = -1.1785393 a.u.&lt;br /&gt;
&lt;br /&gt;
Bond length: 0.7428 Å&lt;br /&gt;
&amp;lt;pre&amp;gt;&lt;br /&gt;
Item               Value     Threshold  Converged?&lt;br /&gt;
 Maximum Force            0.000004     0.000450     YES&lt;br /&gt;
 RMS     Force            0.000004     0.000300     YES&lt;br /&gt;
 Maximum Displacement     0.000005     0.001800     YES&lt;br /&gt;
 RMS     Displacement     0.000007     0.001200     YES&amp;lt;/pre&amp;gt;&lt;br /&gt;
&amp;lt;pre&amp;gt;&lt;br /&gt;
Vibrational mode    Frequency    Infrared&lt;br /&gt;
#1             4465.6       0.0000&lt;br /&gt;
&amp;lt;/pre&amp;gt;&lt;br /&gt;
There are no vibrational modes with negative frequencies&lt;br /&gt;
&lt;br /&gt;
===Analysis of N&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;===&lt;br /&gt;
Calculation method: RB3LYP&lt;br /&gt;
&lt;br /&gt;
Basis Set = 6-31G(d,p)&lt;br /&gt;
&lt;br /&gt;
Final Energy: E(RB3LYP) = -109.5241268 a.u.&lt;br /&gt;
&lt;br /&gt;
Bond length: 1.1055 Å&lt;br /&gt;
&amp;lt;pre&amp;gt;&lt;br /&gt;
Item               Value     Threshold  Converged?&lt;br /&gt;
 Maximum Force            0.000001     0.000450     YES&lt;br /&gt;
 RMS     Force            0.000001     0.000300     YES&lt;br /&gt;
 Maximum Displacement     0.000000     0.001800     YES&lt;br /&gt;
 RMS     Displacement     0.000000     0.001200     YES&lt;br /&gt;
&amp;lt;/pre&amp;gt;&lt;br /&gt;
&amp;lt;pre&amp;gt;&lt;br /&gt;
Vibrational mode    Frequency    Infrared&lt;br /&gt;
#1             2457.33       0.0000&lt;br /&gt;
&amp;lt;/pre&amp;gt;&lt;br /&gt;
There are no vibrational modes with negative frequencies.&lt;br /&gt;
&lt;br /&gt;
===Calculation of the energy of the Haber-Bosch process===&lt;br /&gt;
N&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; + 3H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; -&amp;gt; 2NH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;&lt;br /&gt;
&lt;br /&gt;
E(NH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;)= -56.557768 a.u.&lt;br /&gt;
&lt;br /&gt;
2*E(NH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;)= -113.115536 a.u.&lt;br /&gt;
&lt;br /&gt;
E(N&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;)= -109.5251268 a.u.&lt;br /&gt;
&lt;br /&gt;
E(H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;)= -1.1785393 a.u.&lt;br /&gt;
&lt;br /&gt;
3*E(H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;)= -3.5359617 a.u.&lt;br /&gt;
&lt;br /&gt;
ΔE= 2*E(NH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;) - [E(N&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;) + 3*E(H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;)] = -145.57 kj/mol&lt;br /&gt;
&lt;br /&gt;
As the reaction is exothermic, the ammonia product is more stable than the gaseous reactants.&lt;br /&gt;
&lt;br /&gt;
==Analysis of Cl&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;==&lt;br /&gt;
===General Analysis===&lt;br /&gt;
Calculation method: RB3LYP&lt;br /&gt;
&lt;br /&gt;
Basis Set = 6-31G(d,p)&lt;br /&gt;
&lt;br /&gt;
Final Energy: E(RB3LYP) = -920.3498788 a.u.&lt;br /&gt;
&lt;br /&gt;
Bond length: 2.0417 Å&lt;br /&gt;
===Vibrational Analysis===&lt;br /&gt;
&amp;lt;pre&amp;gt;&lt;br /&gt;
 Item               Value     Threshold  Converged?&lt;br /&gt;
 Maximum Force            0.000043     0.000450     YES&lt;br /&gt;
 RMS     Force            0.000043     0.000300     YES&lt;br /&gt;
 Maximum Displacement     0.000121     0.001800     YES&lt;br /&gt;
 RMS     Displacement     0.000172     0.001200     YES&lt;br /&gt;
&lt;br /&gt;
&amp;lt;/pre&amp;gt;&lt;br /&gt;
&amp;lt;pre&amp;gt;&lt;br /&gt;
Vibrational mode    Frequency    Infrared&lt;br /&gt;
#1             520.32       0.0000&lt;br /&gt;
&amp;lt;/pre&amp;gt;&lt;br /&gt;
There are no vibrational modes with negative frequencies&lt;br /&gt;
===Charge Analysis===&lt;br /&gt;
[[File:Adrian_Popescu_Cl2_Charges2.png|400px|center]]&lt;br /&gt;
As the Cl&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; molecule is made up of identical Cl atoms, the bond between them will be 100% covalent, the electrons that form the sigma bond are equally shared between the Cl atoms, so the charge on each Cl atom is zero.&lt;br /&gt;
&lt;br /&gt;
===Molecular orbitals Analysis===&lt;br /&gt;
[[File:orbital1_.png|400px|thumb|center|2σ&amp;lt;sub&amp;gt;g&amp;lt;/sub&amp;gt; bonding orbital]]&lt;br /&gt;
The 2σ&amp;lt;sub&amp;gt;g&amp;lt;/sub&amp;gt; bonding orbital is deep in energy, occupied, and corresponds to the bonding orbital formed by the 2s AOs of the Cl atoms.&lt;br /&gt;
[[File:Adrian_Popescu_orbital2.png|400px|thumb|center|2σ&amp;lt;sub&amp;gt;u*&amp;lt;/sub&amp;gt; antibonding orbital]]&lt;br /&gt;
The 2σ&amp;lt;sub&amp;gt;u*&amp;lt;/sub&amp;gt; orbital is higher in energy than the 2σ&amp;lt;sub&amp;gt;g&amp;lt;/sub&amp;gt; orbital, is occupied, and corresponds to the antibonding orbital formed by the 2s AOs of the Cl atoms.&lt;br /&gt;
[[File:Adrian_Popescu_orbital3.png|400px|thumb|center|3σ&amp;lt;sub&amp;gt;g&amp;lt;/sub&amp;gt; bonding orbital]]&lt;br /&gt;
The 3σ&amp;lt;sub&amp;gt;g&amp;lt;/sub&amp;gt; orbital is deep in energy, occupied, and corresponds to the bonding orbital formed by the 3p&amp;lt;sub&amp;gt;x&amp;lt;/sub&amp;gt; AOs of the Cl atoms.&lt;br /&gt;
[[File:Adrian_Popescu_homo.png|400px|thumb|center|1π&amp;lt;sub&amp;gt;g*&amp;lt;/sub&amp;gt; antibonding orbital]]&lt;br /&gt;
The 1π&amp;lt;sub&amp;gt;g*&amp;lt;/sub&amp;gt; orbital is high in energy, and is the HOMO (Highest Occupied Molecular Orbital). It corresponds to the antibonding orbital formed by the 3p&amp;lt;sub&amp;gt;y&amp;lt;/sub&amp;gt; (or 3p&amp;lt;sub&amp;gt;z&amp;lt;/sub&amp;gt;, as the orbitals are degenerate) AOs of the Cl atoms.&lt;br /&gt;
[[File:Adrian_Popescu_lumo.png|400px|thumb|center|3σ&amp;lt;sub&amp;gt;u*&amp;lt;/sub&amp;gt; antibonding orbital]]&lt;br /&gt;
The 3σ&amp;lt;sub&amp;gt;u*&amp;lt;/sub&amp;gt; orbital is high in energy, and is the LUMO (Lowest Unoccupied Molecular Orbital). It corresponds to the antibonding orbital formed by the 3p&amp;lt;sub&amp;gt;x&amp;lt;/sub&amp;gt; AOs of the Cl atoms.&lt;/div&gt;</summary>
		<author><name>Ap5817</name></author>
	</entry>
	<entry>
		<id>https://chemwiki.ch.ic.ac.uk/index.php?title=User:Ap5817&amp;diff=680652</id>
		<title>User:Ap5817</title>
		<link rel="alternate" type="text/html" href="https://chemwiki.ch.ic.ac.uk/index.php?title=User:Ap5817&amp;diff=680652"/>
		<updated>2018-03-08T16:19:56Z</updated>

		<summary type="html">&lt;p&gt;Ap5817: /* Vibration analysis of NH3 */&lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;== NH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt; molecule ==&lt;br /&gt;
=== NH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt; calculations ===&lt;br /&gt;
Calculation method:RB3LYP&lt;br /&gt;
&lt;br /&gt;
Basis Set = 6-31G(d,p)&lt;br /&gt;
&lt;br /&gt;
Final Energy: E(RB3LYP) = -56.557768 a.u.&lt;br /&gt;
&lt;br /&gt;
Bond length:1.01789 Å&lt;br /&gt;
&lt;br /&gt;
Bond angle: 105.741 °C&lt;br /&gt;
&lt;br /&gt;
Point Group: C3v&amp;lt;pre&amp;gt;&lt;br /&gt;
Item               Value     Threshold  Converged?&lt;br /&gt;
 Maximum Force            0.000004     0.000450     YES&lt;br /&gt;
 RMS     Force            0.000004     0.000300     YES&lt;br /&gt;
 Maximum Displacement     0.000072     0.001800     YES&lt;br /&gt;
 RMS     Displacement     0.000035     0.001200     YES&lt;br /&gt;
&amp;lt;/pre&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&amp;lt;jmol&amp;gt;&amp;lt;jmolApplet&amp;gt;&lt;br /&gt;
&amp;lt;script&amp;gt;frame x.y&amp;lt;/script&amp;gt;&lt;br /&gt;
  &amp;lt;title&amp;gt;test molecule&amp;lt;/title&amp;gt;&lt;br /&gt;
  &amp;lt;color&amp;gt;black&amp;lt;/color&amp;gt;&lt;br /&gt;
  &amp;lt;size&amp;gt;200&amp;lt;/size&amp;gt;&lt;br /&gt;
  &amp;lt;uploadedFileContents&amp;gt;ADRIAN_POPESCU_PHUNT_NH3_OPTF_POP.LOG&amp;lt;/uploadedFileContents&amp;gt;&lt;br /&gt;
&amp;lt;/jmolApplet&amp;gt;&amp;lt;/jmol&amp;gt;&lt;br /&gt;
&lt;br /&gt;
[[Media:ADRIAN_POPESCU_PHUNT_NH3_OPTF_POP.LOG]]&lt;br /&gt;
&lt;br /&gt;
==Vibration analysis of NH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;==&lt;br /&gt;
[[File:Adrian_Popescu_Vibrations3.png|400px]]&lt;br /&gt;
===Vibrational modes===&lt;br /&gt;
Number of vibrational modes: 6&lt;br /&gt;
&lt;br /&gt;
Number of degenerate modes: 4 (2 pairs of degenerate vibrational modes )&lt;br /&gt;
&lt;br /&gt;
Number of bending motions: 3&lt;br /&gt;
&lt;br /&gt;
Number of stretching motions: 3&lt;br /&gt;
&lt;br /&gt;
The most symmetric vibrational mode: mode #4&lt;br /&gt;
&lt;br /&gt;
The &#039;&#039;umbrella mode&#039;&#039;: mode #1&lt;br /&gt;
&lt;br /&gt;
Number of bands expected to be seen in an experimental spectrum of gaseous ammonia: 5&lt;br /&gt;
===Charge Analysis===&lt;br /&gt;
[[File:Adrian_Popescu_Charges2.png|400px|center]]&lt;br /&gt;
&lt;br /&gt;
Charge on the N atom: -1.125&lt;br /&gt;
&lt;br /&gt;
Charge on the H atom: 0.375&lt;br /&gt;
&lt;br /&gt;
As Nitrogen has an electronegativity value of 3.04, which is significantly larger than the one of Hidrogen (2.2), it is expected that on the Nitrogen there will be a negative charge and on Hidrogen a possitive charge.&lt;br /&gt;
&lt;br /&gt;
==Reactivity of the Haber-Bosch process==&lt;br /&gt;
===Analysis of H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;===&lt;br /&gt;
Calculation method: RB3LYP&lt;br /&gt;
&lt;br /&gt;
Basis Set = 6-31G(d,p)&lt;br /&gt;
&lt;br /&gt;
Final Energy: E(RB3LYP) = -1.1785393 a.u.&lt;br /&gt;
&lt;br /&gt;
Bond length: 0.7428 Å&lt;br /&gt;
&amp;lt;pre&amp;gt;&lt;br /&gt;
Item               Value     Threshold  Converged?&lt;br /&gt;
 Maximum Force            0.000004     0.000450     YES&lt;br /&gt;
 RMS     Force            0.000004     0.000300     YES&lt;br /&gt;
 Maximum Displacement     0.000005     0.001800     YES&lt;br /&gt;
 RMS     Displacement     0.000007     0.001200     YES&amp;lt;/pre&amp;gt;&lt;br /&gt;
&amp;lt;pre&amp;gt;&lt;br /&gt;
Vibrational mode    Frequency    Infrared&lt;br /&gt;
#1             4465.6       0.0000&lt;br /&gt;
&amp;lt;/pre&amp;gt;&lt;br /&gt;
There are no vibrational modes with negative frequencies&lt;br /&gt;
&lt;br /&gt;
===Analysis of N&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;===&lt;br /&gt;
Calculation method: RB3LYP&lt;br /&gt;
&lt;br /&gt;
Basis Set = 6-31G(d,p)&lt;br /&gt;
&lt;br /&gt;
Final Energy: E(RB3LYP) = -109.5241268 a.u.&lt;br /&gt;
&lt;br /&gt;
Bond length: 1.1055 Å&lt;br /&gt;
&amp;lt;pre&amp;gt;&lt;br /&gt;
Item               Value     Threshold  Converged?&lt;br /&gt;
 Maximum Force            0.000001     0.000450     YES&lt;br /&gt;
 RMS     Force            0.000001     0.000300     YES&lt;br /&gt;
 Maximum Displacement     0.000000     0.001800     YES&lt;br /&gt;
 RMS     Displacement     0.000000     0.001200     YES&lt;br /&gt;
&amp;lt;/pre&amp;gt;&lt;br /&gt;
&amp;lt;pre&amp;gt;&lt;br /&gt;
Vibrational mode    Frequency    Infrared&lt;br /&gt;
#1             2457.33       0.0000&lt;br /&gt;
&amp;lt;/pre&amp;gt;&lt;br /&gt;
There are no vibrational modes with negative frequencies.&lt;br /&gt;
&lt;br /&gt;
===Calculation of the energy of the Haber-Bosch process===&lt;br /&gt;
N&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; + 3H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; -&amp;gt; 2NH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;&lt;br /&gt;
&lt;br /&gt;
E(NH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;)= -56.557768 a.u.&lt;br /&gt;
&lt;br /&gt;
2*E(NH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;)= -113.115536 a.u.&lt;br /&gt;
&lt;br /&gt;
E(N&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;)= -109.5251268 a.u.&lt;br /&gt;
&lt;br /&gt;
E(H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;)= -1.1785393 a.u.&lt;br /&gt;
&lt;br /&gt;
3*E(H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;)= -3.5359617 a.u.&lt;br /&gt;
&lt;br /&gt;
ΔE= 2*E(NH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;) - [E(N&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;) + 3*E(H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;)] = -145.57 kj/mol&lt;br /&gt;
&lt;br /&gt;
As the reaction is exothermic, the ammonia product is more stable than the gaseous reactants.&lt;br /&gt;
&lt;br /&gt;
==Analysis of Cl&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;==&lt;br /&gt;
===General Analysis===&lt;br /&gt;
Calculation method: RB3LYP&lt;br /&gt;
&lt;br /&gt;
Basis Set = 6-31G(d,p)&lt;br /&gt;
&lt;br /&gt;
Final Energy: E(RB3LYP) = -920.3498788 a.u.&lt;br /&gt;
&lt;br /&gt;
Bond length: 2.0417 Å&lt;br /&gt;
===Vibrational Analysis===&lt;br /&gt;
&amp;lt;pre&amp;gt;&lt;br /&gt;
 Item               Value     Threshold  Converged?&lt;br /&gt;
 Maximum Force            0.000043     0.000450     YES&lt;br /&gt;
 RMS     Force            0.000043     0.000300     YES&lt;br /&gt;
 Maximum Displacement     0.000121     0.001800     YES&lt;br /&gt;
 RMS     Displacement     0.000172     0.001200     YES&lt;br /&gt;
&lt;br /&gt;
&amp;lt;/pre&amp;gt;&lt;br /&gt;
&amp;lt;pre&amp;gt;&lt;br /&gt;
Vibrational mode    Frequency    Infrared&lt;br /&gt;
#1             520.32       0.0000&lt;br /&gt;
&amp;lt;/pre&amp;gt;&lt;br /&gt;
There are no vibrational modes with negative frequencies&lt;br /&gt;
===Charge Analysis===&lt;br /&gt;
[[File:Adrian_Popescu_Cl2_Charges2.png|400px|center]]&lt;br /&gt;
As the Cl&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; molecule is made up of identical Cl atoms, the bond between them will be 100% covalent, the electrons that form the sigma bond are equally shared between the Cl atoms, so the charge on each Cl atom is zero.&lt;br /&gt;
&lt;br /&gt;
===Molecular orbitals Analysis===&lt;br /&gt;
[[File:orbital1_.png|400px|thumb|center|2σ&amp;lt;sub&amp;gt;g&amp;lt;/sub&amp;gt; bonding orbital]]&lt;br /&gt;
The 2σ&amp;lt;sub&amp;gt;g&amp;lt;/sub&amp;gt; bonding orbital is deep in energy, occupied, and corresponds to the bonding orbital formed by the 2s AOs of the Cl atoms.&lt;br /&gt;
[[File:Adrian_Popescu_orbital2.png|400px|thumb|center|2σ&amp;lt;sub&amp;gt;u*&amp;lt;/sub&amp;gt; antibonding orbital]]&lt;br /&gt;
The 2σ&amp;lt;sub&amp;gt;u*&amp;lt;/sub&amp;gt; orbital is higher in energy than the 2σ&amp;lt;sub&amp;gt;g&amp;lt;/sub&amp;gt; orbital, is occupied, and corresponds to the antibonding orbital formed by the 2s AOs of the Cl atoms.&lt;br /&gt;
[[File:Adrian_Popescu_orbital3.png|400px|thumb|center|3σ&amp;lt;sub&amp;gt;g&amp;lt;/sub&amp;gt; bonding orbital]]&lt;br /&gt;
The 3σ&amp;lt;sub&amp;gt;g&amp;lt;/sub&amp;gt; orbital is deep in energy, occupied, and corresponds to the bonding orbital formed by the 3p&amp;lt;sub&amp;gt;x&amp;lt;/sub&amp;gt; AOs of the Cl atoms.&lt;br /&gt;
[[File:Adrian_Popescu_homo.png|400px|thumb|center|1π&amp;lt;sub&amp;gt;g*&amp;lt;/sub&amp;gt; antibonding orbital]]&lt;br /&gt;
The 1π&amp;lt;sub&amp;gt;g*&amp;lt;/sub&amp;gt; orbital is high in energy, and is the HOMO (Highest Occupied Molecular Orbital). It corresponds to the antibonding orbital formed by the 3p&amp;lt;sub&amp;gt;y&amp;lt;/sub&amp;gt; (or 3p&amp;lt;sub&amp;gt;z&amp;lt;/sub&amp;gt;, as the orbitals are degenerate) AOs of the Cl atoms.&lt;br /&gt;
[[File:Adrian_Popescu_lumo.png|400px|thumb|center|3σ&amp;lt;sub&amp;gt;u*&amp;lt;/sub&amp;gt; antibonding orbital]]&lt;br /&gt;
The 3σ&amp;lt;sub&amp;gt;u*&amp;lt;/sub&amp;gt; orbital is high in energy, and is the LUMO (Lowest Unoccupied Molecular Orbital). It corresponds to the antibonding orbital formed by the 3p&amp;lt;sub&amp;gt;x&amp;lt;/sub&amp;gt; AOs of the Cl atoms.&lt;/div&gt;</summary>
		<author><name>Ap5817</name></author>
	</entry>
	<entry>
		<id>https://chemwiki.ch.ic.ac.uk/index.php?title=File:Adrian_Popescu_Vibrations3.png&amp;diff=680651</id>
		<title>File:Adrian Popescu Vibrations3.png</title>
		<link rel="alternate" type="text/html" href="https://chemwiki.ch.ic.ac.uk/index.php?title=File:Adrian_Popescu_Vibrations3.png&amp;diff=680651"/>
		<updated>2018-03-08T16:19:34Z</updated>

		<summary type="html">&lt;p&gt;Ap5817: &lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;&lt;/div&gt;</summary>
		<author><name>Ap5817</name></author>
	</entry>
	<entry>
		<id>https://chemwiki.ch.ic.ac.uk/index.php?title=File:Adrian_Popescu_Vibrations2.png&amp;diff=680650</id>
		<title>File:Adrian Popescu Vibrations2.png</title>
		<link rel="alternate" type="text/html" href="https://chemwiki.ch.ic.ac.uk/index.php?title=File:Adrian_Popescu_Vibrations2.png&amp;diff=680650"/>
		<updated>2018-03-08T16:17:55Z</updated>

		<summary type="html">&lt;p&gt;Ap5817: Ap5817 uploaded a new version of File:Adrian Popescu Vibrations2.png&lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;&lt;/div&gt;</summary>
		<author><name>Ap5817</name></author>
	</entry>
	<entry>
		<id>https://chemwiki.ch.ic.ac.uk/index.php?title=User:Ap5817&amp;diff=680640</id>
		<title>User:Ap5817</title>
		<link rel="alternate" type="text/html" href="https://chemwiki.ch.ic.ac.uk/index.php?title=User:Ap5817&amp;diff=680640"/>
		<updated>2018-03-08T16:10:43Z</updated>

		<summary type="html">&lt;p&gt;Ap5817: /* Calculation of the energy of the Haber-Bosch process */&lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;== NH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt; molecule ==&lt;br /&gt;
=== NH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt; calculations ===&lt;br /&gt;
Calculation method:RB3LYP&lt;br /&gt;
&lt;br /&gt;
Basis Set = 6-31G(d,p)&lt;br /&gt;
&lt;br /&gt;
Final Energy: E(RB3LYP) = -56.557768 a.u.&lt;br /&gt;
&lt;br /&gt;
Bond length:1.01789 Å&lt;br /&gt;
&lt;br /&gt;
Bond angle: 105.741 °C&lt;br /&gt;
&lt;br /&gt;
Point Group: C3v&amp;lt;pre&amp;gt;&lt;br /&gt;
Item               Value     Threshold  Converged?&lt;br /&gt;
 Maximum Force            0.000004     0.000450     YES&lt;br /&gt;
 RMS     Force            0.000004     0.000300     YES&lt;br /&gt;
 Maximum Displacement     0.000072     0.001800     YES&lt;br /&gt;
 RMS     Displacement     0.000035     0.001200     YES&lt;br /&gt;
&amp;lt;/pre&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&amp;lt;jmol&amp;gt;&amp;lt;jmolApplet&amp;gt;&lt;br /&gt;
&amp;lt;script&amp;gt;frame x.y&amp;lt;/script&amp;gt;&lt;br /&gt;
  &amp;lt;title&amp;gt;test molecule&amp;lt;/title&amp;gt;&lt;br /&gt;
  &amp;lt;color&amp;gt;black&amp;lt;/color&amp;gt;&lt;br /&gt;
  &amp;lt;size&amp;gt;200&amp;lt;/size&amp;gt;&lt;br /&gt;
  &amp;lt;uploadedFileContents&amp;gt;ADRIAN_POPESCU_PHUNT_NH3_OPTF_POP.LOG&amp;lt;/uploadedFileContents&amp;gt;&lt;br /&gt;
&amp;lt;/jmolApplet&amp;gt;&amp;lt;/jmol&amp;gt;&lt;br /&gt;
&lt;br /&gt;
[[Media:ADRIAN_POPESCU_PHUNT_NH3_OPTF_POP.LOG]]&lt;br /&gt;
&lt;br /&gt;
==Vibration analysis of NH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;==&lt;br /&gt;
[[File:Adrian_Popescu_Vibrations2.png|400px]]&lt;br /&gt;
===Vibrational modes===&lt;br /&gt;
Number of vibrational modes: 6&lt;br /&gt;
&lt;br /&gt;
Number of degenerate modes: 4 (2 pairs of degenerate vibrational modes )&lt;br /&gt;
&lt;br /&gt;
Number of bending motions: 3&lt;br /&gt;
&lt;br /&gt;
Number of stretching motions: 3&lt;br /&gt;
&lt;br /&gt;
The most symmetric vibrational mode: mode #4&lt;br /&gt;
&lt;br /&gt;
The &#039;&#039;umbrella mode&#039;&#039;: mode #1&lt;br /&gt;
&lt;br /&gt;
Number of bands expected to be seen in an experimental spectrum of gaseous ammonia: 5&lt;br /&gt;
===Charge Analysis===&lt;br /&gt;
[[File:Adrian_Popescu_Charges2.png|400px|center]]&lt;br /&gt;
&lt;br /&gt;
Charge on the N atom: -1.125&lt;br /&gt;
&lt;br /&gt;
Charge on the H atom: 0.375&lt;br /&gt;
&lt;br /&gt;
As Nitrogen has an electronegativity value of 3.04, which is significantly larger than the one of Hidrogen (2.2), it is expected that on the Nitrogen there will be a negative charge and on Hidrogen a possitive charge.&lt;br /&gt;
&lt;br /&gt;
==Reactivity of the Haber-Bosch process==&lt;br /&gt;
===Analysis of H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;===&lt;br /&gt;
Calculation method: RB3LYP&lt;br /&gt;
&lt;br /&gt;
Basis Set = 6-31G(d,p)&lt;br /&gt;
&lt;br /&gt;
Final Energy: E(RB3LYP) = -1.1785393 a.u.&lt;br /&gt;
&lt;br /&gt;
Bond length: 0.7428 Å&lt;br /&gt;
&amp;lt;pre&amp;gt;&lt;br /&gt;
Item               Value     Threshold  Converged?&lt;br /&gt;
 Maximum Force            0.000004     0.000450     YES&lt;br /&gt;
 RMS     Force            0.000004     0.000300     YES&lt;br /&gt;
 Maximum Displacement     0.000005     0.001800     YES&lt;br /&gt;
 RMS     Displacement     0.000007     0.001200     YES&amp;lt;/pre&amp;gt;&lt;br /&gt;
&amp;lt;pre&amp;gt;&lt;br /&gt;
Vibrational mode    Frequency    Infrared&lt;br /&gt;
#1             4465.6       0.0000&lt;br /&gt;
&amp;lt;/pre&amp;gt;&lt;br /&gt;
There are no vibrational modes with negative frequencies&lt;br /&gt;
&lt;br /&gt;
===Analysis of N&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;===&lt;br /&gt;
Calculation method: RB3LYP&lt;br /&gt;
&lt;br /&gt;
Basis Set = 6-31G(d,p)&lt;br /&gt;
&lt;br /&gt;
Final Energy: E(RB3LYP) = -109.5241268 a.u.&lt;br /&gt;
&lt;br /&gt;
Bond length: 1.1055 Å&lt;br /&gt;
&amp;lt;pre&amp;gt;&lt;br /&gt;
Item               Value     Threshold  Converged?&lt;br /&gt;
 Maximum Force            0.000001     0.000450     YES&lt;br /&gt;
 RMS     Force            0.000001     0.000300     YES&lt;br /&gt;
 Maximum Displacement     0.000000     0.001800     YES&lt;br /&gt;
 RMS     Displacement     0.000000     0.001200     YES&lt;br /&gt;
&amp;lt;/pre&amp;gt;&lt;br /&gt;
&amp;lt;pre&amp;gt;&lt;br /&gt;
Vibrational mode    Frequency    Infrared&lt;br /&gt;
#1             2457.33       0.0000&lt;br /&gt;
&amp;lt;/pre&amp;gt;&lt;br /&gt;
There are no vibrational modes with negative frequencies.&lt;br /&gt;
&lt;br /&gt;
===Calculation of the energy of the Haber-Bosch process===&lt;br /&gt;
N&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; + 3H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; -&amp;gt; 2NH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;&lt;br /&gt;
&lt;br /&gt;
E(NH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;)= -56.557768 a.u.&lt;br /&gt;
&lt;br /&gt;
2*E(NH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;)= -113.115536 a.u.&lt;br /&gt;
&lt;br /&gt;
E(N&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;)= -109.5251268 a.u.&lt;br /&gt;
&lt;br /&gt;
E(H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;)= -1.1785393 a.u.&lt;br /&gt;
&lt;br /&gt;
3*E(H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;)= -3.5359617 a.u.&lt;br /&gt;
&lt;br /&gt;
ΔE= 2*E(NH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;) - [E(N&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;) + 3*E(H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;)] = -145.57 kj/mol&lt;br /&gt;
&lt;br /&gt;
As the reaction is exothermic, the ammonia product is more stable than the gaseous reactants.&lt;br /&gt;
&lt;br /&gt;
==Analysis of Cl&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;==&lt;br /&gt;
===General Analysis===&lt;br /&gt;
Calculation method: RB3LYP&lt;br /&gt;
&lt;br /&gt;
Basis Set = 6-31G(d,p)&lt;br /&gt;
&lt;br /&gt;
Final Energy: E(RB3LYP) = -920.3498788 a.u.&lt;br /&gt;
&lt;br /&gt;
Bond length: 2.0417 Å&lt;br /&gt;
===Vibrational Analysis===&lt;br /&gt;
&amp;lt;pre&amp;gt;&lt;br /&gt;
 Item               Value     Threshold  Converged?&lt;br /&gt;
 Maximum Force            0.000043     0.000450     YES&lt;br /&gt;
 RMS     Force            0.000043     0.000300     YES&lt;br /&gt;
 Maximum Displacement     0.000121     0.001800     YES&lt;br /&gt;
 RMS     Displacement     0.000172     0.001200     YES&lt;br /&gt;
&lt;br /&gt;
&amp;lt;/pre&amp;gt;&lt;br /&gt;
&amp;lt;pre&amp;gt;&lt;br /&gt;
Vibrational mode    Frequency    Infrared&lt;br /&gt;
#1             520.32       0.0000&lt;br /&gt;
&amp;lt;/pre&amp;gt;&lt;br /&gt;
There are no vibrational modes with negative frequencies&lt;br /&gt;
===Charge Analysis===&lt;br /&gt;
[[File:Adrian_Popescu_Cl2_Charges2.png|400px|center]]&lt;br /&gt;
As the Cl&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; molecule is made up of identical Cl atoms, the bond between them will be 100% covalent, the electrons that form the sigma bond are equally shared between the Cl atoms, so the charge on each Cl atom is zero.&lt;br /&gt;
&lt;br /&gt;
===Molecular orbitals Analysis===&lt;br /&gt;
[[File:orbital1_.png|400px|thumb|center|2σ&amp;lt;sub&amp;gt;g&amp;lt;/sub&amp;gt; bonding orbital]]&lt;br /&gt;
The 2σ&amp;lt;sub&amp;gt;g&amp;lt;/sub&amp;gt; bonding orbital is deep in energy, occupied, and corresponds to the bonding orbital formed by the 2s AOs of the Cl atoms.&lt;br /&gt;
[[File:Adrian_Popescu_orbital2.png|400px|thumb|center|2σ&amp;lt;sub&amp;gt;u*&amp;lt;/sub&amp;gt; antibonding orbital]]&lt;br /&gt;
The 2σ&amp;lt;sub&amp;gt;u*&amp;lt;/sub&amp;gt; orbital is higher in energy than the 2σ&amp;lt;sub&amp;gt;g&amp;lt;/sub&amp;gt; orbital, is occupied, and corresponds to the antibonding orbital formed by the 2s AOs of the Cl atoms.&lt;br /&gt;
[[File:Adrian_Popescu_orbital3.png|400px|thumb|center|3σ&amp;lt;sub&amp;gt;g&amp;lt;/sub&amp;gt; bonding orbital]]&lt;br /&gt;
The 3σ&amp;lt;sub&amp;gt;g&amp;lt;/sub&amp;gt; orbital is deep in energy, occupied, and corresponds to the bonding orbital formed by the 3p&amp;lt;sub&amp;gt;x&amp;lt;/sub&amp;gt; AOs of the Cl atoms.&lt;br /&gt;
[[File:Adrian_Popescu_homo.png|400px|thumb|center|1π&amp;lt;sub&amp;gt;g*&amp;lt;/sub&amp;gt; antibonding orbital]]&lt;br /&gt;
The 1π&amp;lt;sub&amp;gt;g*&amp;lt;/sub&amp;gt; orbital is high in energy, and is the HOMO (Highest Occupied Molecular Orbital). It corresponds to the antibonding orbital formed by the 3p&amp;lt;sub&amp;gt;y&amp;lt;/sub&amp;gt; (or 3p&amp;lt;sub&amp;gt;z&amp;lt;/sub&amp;gt;, as the orbitals are degenerate) AOs of the Cl atoms.&lt;br /&gt;
[[File:Adrian_Popescu_lumo.png|400px|thumb|center|3σ&amp;lt;sub&amp;gt;u*&amp;lt;/sub&amp;gt; antibonding orbital]]&lt;br /&gt;
The 3σ&amp;lt;sub&amp;gt;u*&amp;lt;/sub&amp;gt; orbital is high in energy, and is the LUMO (Lowest Unoccupied Molecular Orbital). It corresponds to the antibonding orbital formed by the 3p&amp;lt;sub&amp;gt;x&amp;lt;/sub&amp;gt; AOs of the Cl atoms.&lt;/div&gt;</summary>
		<author><name>Ap5817</name></author>
	</entry>
	<entry>
		<id>https://chemwiki.ch.ic.ac.uk/index.php?title=User:Ap5817&amp;diff=680637</id>
		<title>User:Ap5817</title>
		<link rel="alternate" type="text/html" href="https://chemwiki.ch.ic.ac.uk/index.php?title=User:Ap5817&amp;diff=680637"/>
		<updated>2018-03-08T16:10:02Z</updated>

		<summary type="html">&lt;p&gt;Ap5817: /* Calculation of the energy of the Haber-Bosch process */&lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;== NH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt; molecule ==&lt;br /&gt;
=== NH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt; calculations ===&lt;br /&gt;
Calculation method:RB3LYP&lt;br /&gt;
&lt;br /&gt;
Basis Set = 6-31G(d,p)&lt;br /&gt;
&lt;br /&gt;
Final Energy: E(RB3LYP) = -56.557768 a.u.&lt;br /&gt;
&lt;br /&gt;
Bond length:1.01789 Å&lt;br /&gt;
&lt;br /&gt;
Bond angle: 105.741 °C&lt;br /&gt;
&lt;br /&gt;
Point Group: C3v&amp;lt;pre&amp;gt;&lt;br /&gt;
Item               Value     Threshold  Converged?&lt;br /&gt;
 Maximum Force            0.000004     0.000450     YES&lt;br /&gt;
 RMS     Force            0.000004     0.000300     YES&lt;br /&gt;
 Maximum Displacement     0.000072     0.001800     YES&lt;br /&gt;
 RMS     Displacement     0.000035     0.001200     YES&lt;br /&gt;
&amp;lt;/pre&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&amp;lt;jmol&amp;gt;&amp;lt;jmolApplet&amp;gt;&lt;br /&gt;
&amp;lt;script&amp;gt;frame x.y&amp;lt;/script&amp;gt;&lt;br /&gt;
  &amp;lt;title&amp;gt;test molecule&amp;lt;/title&amp;gt;&lt;br /&gt;
  &amp;lt;color&amp;gt;black&amp;lt;/color&amp;gt;&lt;br /&gt;
  &amp;lt;size&amp;gt;200&amp;lt;/size&amp;gt;&lt;br /&gt;
  &amp;lt;uploadedFileContents&amp;gt;ADRIAN_POPESCU_PHUNT_NH3_OPTF_POP.LOG&amp;lt;/uploadedFileContents&amp;gt;&lt;br /&gt;
&amp;lt;/jmolApplet&amp;gt;&amp;lt;/jmol&amp;gt;&lt;br /&gt;
&lt;br /&gt;
[[Media:ADRIAN_POPESCU_PHUNT_NH3_OPTF_POP.LOG]]&lt;br /&gt;
&lt;br /&gt;
==Vibration analysis of NH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;==&lt;br /&gt;
[[File:Adrian_Popescu_Vibrations2.png|400px]]&lt;br /&gt;
===Vibrational modes===&lt;br /&gt;
Number of vibrational modes: 6&lt;br /&gt;
&lt;br /&gt;
Number of degenerate modes: 4 (2 pairs of degenerate vibrational modes )&lt;br /&gt;
&lt;br /&gt;
Number of bending motions: 3&lt;br /&gt;
&lt;br /&gt;
Number of stretching motions: 3&lt;br /&gt;
&lt;br /&gt;
The most symmetric vibrational mode: mode #4&lt;br /&gt;
&lt;br /&gt;
The &#039;&#039;umbrella mode&#039;&#039;: mode #1&lt;br /&gt;
&lt;br /&gt;
Number of bands expected to be seen in an experimental spectrum of gaseous ammonia: 5&lt;br /&gt;
===Charge Analysis===&lt;br /&gt;
[[File:Adrian_Popescu_Charges2.png|400px|center]]&lt;br /&gt;
&lt;br /&gt;
Charge on the N atom: -1.125&lt;br /&gt;
&lt;br /&gt;
Charge on the H atom: 0.375&lt;br /&gt;
&lt;br /&gt;
As Nitrogen has an electronegativity value of 3.04, which is significantly larger than the one of Hidrogen (2.2), it is expected that on the Nitrogen there will be a negative charge and on Hidrogen a possitive charge.&lt;br /&gt;
&lt;br /&gt;
==Reactivity of the Haber-Bosch process==&lt;br /&gt;
===Analysis of H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;===&lt;br /&gt;
Calculation method: RB3LYP&lt;br /&gt;
&lt;br /&gt;
Basis Set = 6-31G(d,p)&lt;br /&gt;
&lt;br /&gt;
Final Energy: E(RB3LYP) = -1.1785393 a.u.&lt;br /&gt;
&lt;br /&gt;
Bond length: 0.7428 Å&lt;br /&gt;
&amp;lt;pre&amp;gt;&lt;br /&gt;
Item               Value     Threshold  Converged?&lt;br /&gt;
 Maximum Force            0.000004     0.000450     YES&lt;br /&gt;
 RMS     Force            0.000004     0.000300     YES&lt;br /&gt;
 Maximum Displacement     0.000005     0.001800     YES&lt;br /&gt;
 RMS     Displacement     0.000007     0.001200     YES&amp;lt;/pre&amp;gt;&lt;br /&gt;
&amp;lt;pre&amp;gt;&lt;br /&gt;
Vibrational mode    Frequency    Infrared&lt;br /&gt;
#1             4465.6       0.0000&lt;br /&gt;
&amp;lt;/pre&amp;gt;&lt;br /&gt;
There are no vibrational modes with negative frequencies&lt;br /&gt;
&lt;br /&gt;
===Analysis of N&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;===&lt;br /&gt;
Calculation method: RB3LYP&lt;br /&gt;
&lt;br /&gt;
Basis Set = 6-31G(d,p)&lt;br /&gt;
&lt;br /&gt;
Final Energy: E(RB3LYP) = -109.5241268 a.u.&lt;br /&gt;
&lt;br /&gt;
Bond length: 1.1055 Å&lt;br /&gt;
&amp;lt;pre&amp;gt;&lt;br /&gt;
Item               Value     Threshold  Converged?&lt;br /&gt;
 Maximum Force            0.000001     0.000450     YES&lt;br /&gt;
 RMS     Force            0.000001     0.000300     YES&lt;br /&gt;
 Maximum Displacement     0.000000     0.001800     YES&lt;br /&gt;
 RMS     Displacement     0.000000     0.001200     YES&lt;br /&gt;
&amp;lt;/pre&amp;gt;&lt;br /&gt;
&amp;lt;pre&amp;gt;&lt;br /&gt;
Vibrational mode    Frequency    Infrared&lt;br /&gt;
#1             2457.33       0.0000&lt;br /&gt;
&amp;lt;/pre&amp;gt;&lt;br /&gt;
There are no vibrational modes with negative frequencies.&lt;br /&gt;
&lt;br /&gt;
===Calculation of the energy of the Haber-Bosch process===&lt;br /&gt;
N&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; + 3H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; -&amp;gt; 2NH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;&lt;br /&gt;
&lt;br /&gt;
E(NH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;)= -56.557768 a u&lt;br /&gt;
&lt;br /&gt;
2*E(NH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;)= -113.115536 a u&lt;br /&gt;
&lt;br /&gt;
E(N&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;)= -109.5251268 a u&lt;br /&gt;
&lt;br /&gt;
E(H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;)= -1.1785393 a u&lt;br /&gt;
&lt;br /&gt;
3*E(H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;)= -3.5359617 a u&lt;br /&gt;
&lt;br /&gt;
ΔE= 2*E(NH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;) - [E(N&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;) + 3*E(H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;)] = -145.57 kj/mol&lt;br /&gt;
&lt;br /&gt;
As the reaction is exothermic, the ammonia product is more stable than the gaseous reactants.&lt;br /&gt;
&lt;br /&gt;
==Analysis of Cl&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;==&lt;br /&gt;
===General Analysis===&lt;br /&gt;
Calculation method: RB3LYP&lt;br /&gt;
&lt;br /&gt;
Basis Set = 6-31G(d,p)&lt;br /&gt;
&lt;br /&gt;
Final Energy: E(RB3LYP) = -920.3498788 a.u.&lt;br /&gt;
&lt;br /&gt;
Bond length: 2.0417 Å&lt;br /&gt;
===Vibrational Analysis===&lt;br /&gt;
&amp;lt;pre&amp;gt;&lt;br /&gt;
 Item               Value     Threshold  Converged?&lt;br /&gt;
 Maximum Force            0.000043     0.000450     YES&lt;br /&gt;
 RMS     Force            0.000043     0.000300     YES&lt;br /&gt;
 Maximum Displacement     0.000121     0.001800     YES&lt;br /&gt;
 RMS     Displacement     0.000172     0.001200     YES&lt;br /&gt;
&lt;br /&gt;
&amp;lt;/pre&amp;gt;&lt;br /&gt;
&amp;lt;pre&amp;gt;&lt;br /&gt;
Vibrational mode    Frequency    Infrared&lt;br /&gt;
#1             520.32       0.0000&lt;br /&gt;
&amp;lt;/pre&amp;gt;&lt;br /&gt;
There are no vibrational modes with negative frequencies&lt;br /&gt;
===Charge Analysis===&lt;br /&gt;
[[File:Adrian_Popescu_Cl2_Charges2.png|400px|center]]&lt;br /&gt;
As the Cl&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; molecule is made up of identical Cl atoms, the bond between them will be 100% covalent, the electrons that form the sigma bond are equally shared between the Cl atoms, so the charge on each Cl atom is zero.&lt;br /&gt;
&lt;br /&gt;
===Molecular orbitals Analysis===&lt;br /&gt;
[[File:orbital1_.png|400px|thumb|center|2σ&amp;lt;sub&amp;gt;g&amp;lt;/sub&amp;gt; bonding orbital]]&lt;br /&gt;
The 2σ&amp;lt;sub&amp;gt;g&amp;lt;/sub&amp;gt; bonding orbital is deep in energy, occupied, and corresponds to the bonding orbital formed by the 2s AOs of the Cl atoms.&lt;br /&gt;
[[File:Adrian_Popescu_orbital2.png|400px|thumb|center|2σ&amp;lt;sub&amp;gt;u*&amp;lt;/sub&amp;gt; antibonding orbital]]&lt;br /&gt;
The 2σ&amp;lt;sub&amp;gt;u*&amp;lt;/sub&amp;gt; orbital is higher in energy than the 2σ&amp;lt;sub&amp;gt;g&amp;lt;/sub&amp;gt; orbital, is occupied, and corresponds to the antibonding orbital formed by the 2s AOs of the Cl atoms.&lt;br /&gt;
[[File:Adrian_Popescu_orbital3.png|400px|thumb|center|3σ&amp;lt;sub&amp;gt;g&amp;lt;/sub&amp;gt; bonding orbital]]&lt;br /&gt;
The 3σ&amp;lt;sub&amp;gt;g&amp;lt;/sub&amp;gt; orbital is deep in energy, occupied, and corresponds to the bonding orbital formed by the 3p&amp;lt;sub&amp;gt;x&amp;lt;/sub&amp;gt; AOs of the Cl atoms.&lt;br /&gt;
[[File:Adrian_Popescu_homo.png|400px|thumb|center|1π&amp;lt;sub&amp;gt;g*&amp;lt;/sub&amp;gt; antibonding orbital]]&lt;br /&gt;
The 1π&amp;lt;sub&amp;gt;g*&amp;lt;/sub&amp;gt; orbital is high in energy, and is the HOMO (Highest Occupied Molecular Orbital). It corresponds to the antibonding orbital formed by the 3p&amp;lt;sub&amp;gt;y&amp;lt;/sub&amp;gt; (or 3p&amp;lt;sub&amp;gt;z&amp;lt;/sub&amp;gt;, as the orbitals are degenerate) AOs of the Cl atoms.&lt;br /&gt;
[[File:Adrian_Popescu_lumo.png|400px|thumb|center|3σ&amp;lt;sub&amp;gt;u*&amp;lt;/sub&amp;gt; antibonding orbital]]&lt;br /&gt;
The 3σ&amp;lt;sub&amp;gt;u*&amp;lt;/sub&amp;gt; orbital is high in energy, and is the LUMO (Lowest Unoccupied Molecular Orbital). It corresponds to the antibonding orbital formed by the 3p&amp;lt;sub&amp;gt;x&amp;lt;/sub&amp;gt; AOs of the Cl atoms.&lt;/div&gt;</summary>
		<author><name>Ap5817</name></author>
	</entry>
	<entry>
		<id>https://chemwiki.ch.ic.ac.uk/index.php?title=User:Ap5817&amp;diff=680635</id>
		<title>User:Ap5817</title>
		<link rel="alternate" type="text/html" href="https://chemwiki.ch.ic.ac.uk/index.php?title=User:Ap5817&amp;diff=680635"/>
		<updated>2018-03-08T16:09:38Z</updated>

		<summary type="html">&lt;p&gt;Ap5817: /* Analysis of H2 */&lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;== NH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt; molecule ==&lt;br /&gt;
=== NH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt; calculations ===&lt;br /&gt;
Calculation method:RB3LYP&lt;br /&gt;
&lt;br /&gt;
Basis Set = 6-31G(d,p)&lt;br /&gt;
&lt;br /&gt;
Final Energy: E(RB3LYP) = -56.557768 a.u.&lt;br /&gt;
&lt;br /&gt;
Bond length:1.01789 Å&lt;br /&gt;
&lt;br /&gt;
Bond angle: 105.741 °C&lt;br /&gt;
&lt;br /&gt;
Point Group: C3v&amp;lt;pre&amp;gt;&lt;br /&gt;
Item               Value     Threshold  Converged?&lt;br /&gt;
 Maximum Force            0.000004     0.000450     YES&lt;br /&gt;
 RMS     Force            0.000004     0.000300     YES&lt;br /&gt;
 Maximum Displacement     0.000072     0.001800     YES&lt;br /&gt;
 RMS     Displacement     0.000035     0.001200     YES&lt;br /&gt;
&amp;lt;/pre&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&amp;lt;jmol&amp;gt;&amp;lt;jmolApplet&amp;gt;&lt;br /&gt;
&amp;lt;script&amp;gt;frame x.y&amp;lt;/script&amp;gt;&lt;br /&gt;
  &amp;lt;title&amp;gt;test molecule&amp;lt;/title&amp;gt;&lt;br /&gt;
  &amp;lt;color&amp;gt;black&amp;lt;/color&amp;gt;&lt;br /&gt;
  &amp;lt;size&amp;gt;200&amp;lt;/size&amp;gt;&lt;br /&gt;
  &amp;lt;uploadedFileContents&amp;gt;ADRIAN_POPESCU_PHUNT_NH3_OPTF_POP.LOG&amp;lt;/uploadedFileContents&amp;gt;&lt;br /&gt;
&amp;lt;/jmolApplet&amp;gt;&amp;lt;/jmol&amp;gt;&lt;br /&gt;
&lt;br /&gt;
[[Media:ADRIAN_POPESCU_PHUNT_NH3_OPTF_POP.LOG]]&lt;br /&gt;
&lt;br /&gt;
==Vibration analysis of NH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;==&lt;br /&gt;
[[File:Adrian_Popescu_Vibrations2.png|400px]]&lt;br /&gt;
===Vibrational modes===&lt;br /&gt;
Number of vibrational modes: 6&lt;br /&gt;
&lt;br /&gt;
Number of degenerate modes: 4 (2 pairs of degenerate vibrational modes )&lt;br /&gt;
&lt;br /&gt;
Number of bending motions: 3&lt;br /&gt;
&lt;br /&gt;
Number of stretching motions: 3&lt;br /&gt;
&lt;br /&gt;
The most symmetric vibrational mode: mode #4&lt;br /&gt;
&lt;br /&gt;
The &#039;&#039;umbrella mode&#039;&#039;: mode #1&lt;br /&gt;
&lt;br /&gt;
Number of bands expected to be seen in an experimental spectrum of gaseous ammonia: 5&lt;br /&gt;
===Charge Analysis===&lt;br /&gt;
[[File:Adrian_Popescu_Charges2.png|400px|center]]&lt;br /&gt;
&lt;br /&gt;
Charge on the N atom: -1.125&lt;br /&gt;
&lt;br /&gt;
Charge on the H atom: 0.375&lt;br /&gt;
&lt;br /&gt;
As Nitrogen has an electronegativity value of 3.04, which is significantly larger than the one of Hidrogen (2.2), it is expected that on the Nitrogen there will be a negative charge and on Hidrogen a possitive charge.&lt;br /&gt;
&lt;br /&gt;
==Reactivity of the Haber-Bosch process==&lt;br /&gt;
===Analysis of H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;===&lt;br /&gt;
Calculation method: RB3LYP&lt;br /&gt;
&lt;br /&gt;
Basis Set = 6-31G(d,p)&lt;br /&gt;
&lt;br /&gt;
Final Energy: E(RB3LYP) = -1.1785393 a.u.&lt;br /&gt;
&lt;br /&gt;
Bond length: 0.7428 Å&lt;br /&gt;
&amp;lt;pre&amp;gt;&lt;br /&gt;
Item               Value     Threshold  Converged?&lt;br /&gt;
 Maximum Force            0.000004     0.000450     YES&lt;br /&gt;
 RMS     Force            0.000004     0.000300     YES&lt;br /&gt;
 Maximum Displacement     0.000005     0.001800     YES&lt;br /&gt;
 RMS     Displacement     0.000007     0.001200     YES&amp;lt;/pre&amp;gt;&lt;br /&gt;
&amp;lt;pre&amp;gt;&lt;br /&gt;
Vibrational mode    Frequency    Infrared&lt;br /&gt;
#1             4465.6       0.0000&lt;br /&gt;
&amp;lt;/pre&amp;gt;&lt;br /&gt;
There are no vibrational modes with negative frequencies&lt;br /&gt;
&lt;br /&gt;
===Analysis of N&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;===&lt;br /&gt;
Calculation method: RB3LYP&lt;br /&gt;
&lt;br /&gt;
Basis Set = 6-31G(d,p)&lt;br /&gt;
&lt;br /&gt;
Final Energy: E(RB3LYP) = -109.5241268 a.u.&lt;br /&gt;
&lt;br /&gt;
Bond length: 1.1055 Å&lt;br /&gt;
&amp;lt;pre&amp;gt;&lt;br /&gt;
Item               Value     Threshold  Converged?&lt;br /&gt;
 Maximum Force            0.000001     0.000450     YES&lt;br /&gt;
 RMS     Force            0.000001     0.000300     YES&lt;br /&gt;
 Maximum Displacement     0.000000     0.001800     YES&lt;br /&gt;
 RMS     Displacement     0.000000     0.001200     YES&lt;br /&gt;
&amp;lt;/pre&amp;gt;&lt;br /&gt;
&amp;lt;pre&amp;gt;&lt;br /&gt;
Vibrational mode    Frequency    Infrared&lt;br /&gt;
#1             2457.33       0.0000&lt;br /&gt;
&amp;lt;/pre&amp;gt;&lt;br /&gt;
There are no vibrational modes with negative frequencies.&lt;br /&gt;
&lt;br /&gt;
===Calculation of the energy of the Haber-Bosch process===&lt;br /&gt;
N&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; + 3H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; -&amp;gt; 2NH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;&lt;br /&gt;
&lt;br /&gt;
E(NH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;)= -56.557768 a u&lt;br /&gt;
&lt;br /&gt;
2*E(NH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;)= -113.115536 a u&lt;br /&gt;
&lt;br /&gt;
E(N&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;)= -109.5251268 a u&lt;br /&gt;
&lt;br /&gt;
E(H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;)= -1.1785393 a u&lt;br /&gt;
&lt;br /&gt;
3*E(H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;)= -3.5359617 a u&lt;br /&gt;
&lt;br /&gt;
ΔE=2*E(NH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;) - [E(N&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;) + 3*E(H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;)] = -145.57 kj/mol&lt;br /&gt;
&lt;br /&gt;
As the reaction is exothermic, the ammonia product is more stable than the gaseous reactants.&lt;br /&gt;
==Analysis of Cl&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;==&lt;br /&gt;
===General Analysis===&lt;br /&gt;
Calculation method: RB3LYP&lt;br /&gt;
&lt;br /&gt;
Basis Set = 6-31G(d,p)&lt;br /&gt;
&lt;br /&gt;
Final Energy: E(RB3LYP) = -920.3498788 a.u.&lt;br /&gt;
&lt;br /&gt;
Bond length: 2.0417 Å&lt;br /&gt;
===Vibrational Analysis===&lt;br /&gt;
&amp;lt;pre&amp;gt;&lt;br /&gt;
 Item               Value     Threshold  Converged?&lt;br /&gt;
 Maximum Force            0.000043     0.000450     YES&lt;br /&gt;
 RMS     Force            0.000043     0.000300     YES&lt;br /&gt;
 Maximum Displacement     0.000121     0.001800     YES&lt;br /&gt;
 RMS     Displacement     0.000172     0.001200     YES&lt;br /&gt;
&lt;br /&gt;
&amp;lt;/pre&amp;gt;&lt;br /&gt;
&amp;lt;pre&amp;gt;&lt;br /&gt;
Vibrational mode    Frequency    Infrared&lt;br /&gt;
#1             520.32       0.0000&lt;br /&gt;
&amp;lt;/pre&amp;gt;&lt;br /&gt;
There are no vibrational modes with negative frequencies&lt;br /&gt;
===Charge Analysis===&lt;br /&gt;
[[File:Adrian_Popescu_Cl2_Charges2.png|400px|center]]&lt;br /&gt;
As the Cl&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; molecule is made up of identical Cl atoms, the bond between them will be 100% covalent, the electrons that form the sigma bond are equally shared between the Cl atoms, so the charge on each Cl atom is zero.&lt;br /&gt;
&lt;br /&gt;
===Molecular orbitals Analysis===&lt;br /&gt;
[[File:orbital1_.png|400px|thumb|center|2σ&amp;lt;sub&amp;gt;g&amp;lt;/sub&amp;gt; bonding orbital]]&lt;br /&gt;
The 2σ&amp;lt;sub&amp;gt;g&amp;lt;/sub&amp;gt; bonding orbital is deep in energy, occupied, and corresponds to the bonding orbital formed by the 2s AOs of the Cl atoms.&lt;br /&gt;
[[File:Adrian_Popescu_orbital2.png|400px|thumb|center|2σ&amp;lt;sub&amp;gt;u*&amp;lt;/sub&amp;gt; antibonding orbital]]&lt;br /&gt;
The 2σ&amp;lt;sub&amp;gt;u*&amp;lt;/sub&amp;gt; orbital is higher in energy than the 2σ&amp;lt;sub&amp;gt;g&amp;lt;/sub&amp;gt; orbital, is occupied, and corresponds to the antibonding orbital formed by the 2s AOs of the Cl atoms.&lt;br /&gt;
[[File:Adrian_Popescu_orbital3.png|400px|thumb|center|3σ&amp;lt;sub&amp;gt;g&amp;lt;/sub&amp;gt; bonding orbital]]&lt;br /&gt;
The 3σ&amp;lt;sub&amp;gt;g&amp;lt;/sub&amp;gt; orbital is deep in energy, occupied, and corresponds to the bonding orbital formed by the 3p&amp;lt;sub&amp;gt;x&amp;lt;/sub&amp;gt; AOs of the Cl atoms.&lt;br /&gt;
[[File:Adrian_Popescu_homo.png|400px|thumb|center|1π&amp;lt;sub&amp;gt;g*&amp;lt;/sub&amp;gt; antibonding orbital]]&lt;br /&gt;
The 1π&amp;lt;sub&amp;gt;g*&amp;lt;/sub&amp;gt; orbital is high in energy, and is the HOMO (Highest Occupied Molecular Orbital). It corresponds to the antibonding orbital formed by the 3p&amp;lt;sub&amp;gt;y&amp;lt;/sub&amp;gt; (or 3p&amp;lt;sub&amp;gt;z&amp;lt;/sub&amp;gt;, as the orbitals are degenerate) AOs of the Cl atoms.&lt;br /&gt;
[[File:Adrian_Popescu_lumo.png|400px|thumb|center|3σ&amp;lt;sub&amp;gt;u*&amp;lt;/sub&amp;gt; antibonding orbital]]&lt;br /&gt;
The 3σ&amp;lt;sub&amp;gt;u*&amp;lt;/sub&amp;gt; orbital is high in energy, and is the LUMO (Lowest Unoccupied Molecular Orbital). It corresponds to the antibonding orbital formed by the 3p&amp;lt;sub&amp;gt;x&amp;lt;/sub&amp;gt; AOs of the Cl atoms.&lt;/div&gt;</summary>
		<author><name>Ap5817</name></author>
	</entry>
	<entry>
		<id>https://chemwiki.ch.ic.ac.uk/index.php?title=User:Ap5817&amp;diff=680633</id>
		<title>User:Ap5817</title>
		<link rel="alternate" type="text/html" href="https://chemwiki.ch.ic.ac.uk/index.php?title=User:Ap5817&amp;diff=680633"/>
		<updated>2018-03-08T16:09:05Z</updated>

		<summary type="html">&lt;p&gt;Ap5817: /* Vibration analysis of NH3 */&lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;== NH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt; molecule ==&lt;br /&gt;
=== NH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt; calculations ===&lt;br /&gt;
Calculation method:RB3LYP&lt;br /&gt;
&lt;br /&gt;
Basis Set = 6-31G(d,p)&lt;br /&gt;
&lt;br /&gt;
Final Energy: E(RB3LYP) = -56.557768 a.u.&lt;br /&gt;
&lt;br /&gt;
Bond length:1.01789 Å&lt;br /&gt;
&lt;br /&gt;
Bond angle: 105.741 °C&lt;br /&gt;
&lt;br /&gt;
Point Group: C3v&amp;lt;pre&amp;gt;&lt;br /&gt;
Item               Value     Threshold  Converged?&lt;br /&gt;
 Maximum Force            0.000004     0.000450     YES&lt;br /&gt;
 RMS     Force            0.000004     0.000300     YES&lt;br /&gt;
 Maximum Displacement     0.000072     0.001800     YES&lt;br /&gt;
 RMS     Displacement     0.000035     0.001200     YES&lt;br /&gt;
&amp;lt;/pre&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&amp;lt;jmol&amp;gt;&amp;lt;jmolApplet&amp;gt;&lt;br /&gt;
&amp;lt;script&amp;gt;frame x.y&amp;lt;/script&amp;gt;&lt;br /&gt;
  &amp;lt;title&amp;gt;test molecule&amp;lt;/title&amp;gt;&lt;br /&gt;
  &amp;lt;color&amp;gt;black&amp;lt;/color&amp;gt;&lt;br /&gt;
  &amp;lt;size&amp;gt;200&amp;lt;/size&amp;gt;&lt;br /&gt;
  &amp;lt;uploadedFileContents&amp;gt;ADRIAN_POPESCU_PHUNT_NH3_OPTF_POP.LOG&amp;lt;/uploadedFileContents&amp;gt;&lt;br /&gt;
&amp;lt;/jmolApplet&amp;gt;&amp;lt;/jmol&amp;gt;&lt;br /&gt;
&lt;br /&gt;
[[Media:ADRIAN_POPESCU_PHUNT_NH3_OPTF_POP.LOG]]&lt;br /&gt;
&lt;br /&gt;
==Vibration analysis of NH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;==&lt;br /&gt;
[[File:Adrian_Popescu_Vibrations2.png|400px]]&lt;br /&gt;
===Vibrational modes===&lt;br /&gt;
Number of vibrational modes: 6&lt;br /&gt;
&lt;br /&gt;
Number of degenerate modes: 4 (2 pairs of degenerate vibrational modes )&lt;br /&gt;
&lt;br /&gt;
Number of bending motions: 3&lt;br /&gt;
&lt;br /&gt;
Number of stretching motions: 3&lt;br /&gt;
&lt;br /&gt;
The most symmetric vibrational mode: mode #4&lt;br /&gt;
&lt;br /&gt;
The &#039;&#039;umbrella mode&#039;&#039;: mode #1&lt;br /&gt;
&lt;br /&gt;
Number of bands expected to be seen in an experimental spectrum of gaseous ammonia: 5&lt;br /&gt;
===Charge Analysis===&lt;br /&gt;
[[File:Adrian_Popescu_Charges2.png|400px|center]]&lt;br /&gt;
&lt;br /&gt;
Charge on the N atom: -1.125&lt;br /&gt;
&lt;br /&gt;
Charge on the H atom: 0.375&lt;br /&gt;
&lt;br /&gt;
As Nitrogen has an electronegativity value of 3.04, which is significantly larger than the one of Hidrogen (2.2), it is expected that on the Nitrogen there will be a negative charge and on Hidrogen a possitive charge.&lt;br /&gt;
&lt;br /&gt;
==Reactivity of the Haber-Bosch process==&lt;br /&gt;
===Analysis of H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;===&lt;br /&gt;
Calculation method:RB3LYP&lt;br /&gt;
&lt;br /&gt;
Basis Set = 6-31G(d,p)&lt;br /&gt;
&lt;br /&gt;
Final Energy: E(RB3LYP) = -1.1785393 a.u.&lt;br /&gt;
&lt;br /&gt;
Bond length:0.7428 Å&lt;br /&gt;
&amp;lt;pre&amp;gt;&lt;br /&gt;
Item               Value     Threshold  Converged?&lt;br /&gt;
 Maximum Force            0.000004     0.000450     YES&lt;br /&gt;
 RMS     Force            0.000004     0.000300     YES&lt;br /&gt;
 Maximum Displacement     0.000005     0.001800     YES&lt;br /&gt;
 RMS     Displacement     0.000007     0.001200     YES&amp;lt;/pre&amp;gt;&lt;br /&gt;
&amp;lt;pre&amp;gt;&lt;br /&gt;
Vibrational mode    Frequency    Infrared&lt;br /&gt;
#1             4465.6       0.0000&lt;br /&gt;
&amp;lt;/pre&amp;gt;&lt;br /&gt;
There are no vibrational modes with negative frequencies&lt;br /&gt;
===Analysis of N&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;===&lt;br /&gt;
Calculation method: RB3LYP&lt;br /&gt;
&lt;br /&gt;
Basis Set = 6-31G(d,p)&lt;br /&gt;
&lt;br /&gt;
Final Energy: E(RB3LYP) = -109.5241268 a.u.&lt;br /&gt;
&lt;br /&gt;
Bond length: 1.1055 Å&lt;br /&gt;
&amp;lt;pre&amp;gt;&lt;br /&gt;
Item               Value     Threshold  Converged?&lt;br /&gt;
 Maximum Force            0.000001     0.000450     YES&lt;br /&gt;
 RMS     Force            0.000001     0.000300     YES&lt;br /&gt;
 Maximum Displacement     0.000000     0.001800     YES&lt;br /&gt;
 RMS     Displacement     0.000000     0.001200     YES&lt;br /&gt;
&amp;lt;/pre&amp;gt;&lt;br /&gt;
&amp;lt;pre&amp;gt;&lt;br /&gt;
Vibrational mode    Frequency    Infrared&lt;br /&gt;
#1             2457.33       0.0000&lt;br /&gt;
&amp;lt;/pre&amp;gt;&lt;br /&gt;
There are no vibrational modes with negative frequencies.&lt;br /&gt;
&lt;br /&gt;
===Calculation of the energy of the Haber-Bosch process===&lt;br /&gt;
N&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; + 3H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; -&amp;gt; 2NH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;&lt;br /&gt;
&lt;br /&gt;
E(NH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;)= -56.557768 a u&lt;br /&gt;
&lt;br /&gt;
2*E(NH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;)= -113.115536 a u&lt;br /&gt;
&lt;br /&gt;
E(N&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;)= -109.5251268 a u&lt;br /&gt;
&lt;br /&gt;
E(H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;)= -1.1785393 a u&lt;br /&gt;
&lt;br /&gt;
3*E(H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;)= -3.5359617 a u&lt;br /&gt;
&lt;br /&gt;
ΔE=2*E(NH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;) - [E(N&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;) + 3*E(H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;)] = -145.57 kj/mol&lt;br /&gt;
&lt;br /&gt;
As the reaction is exothermic, the ammonia product is more stable than the gaseous reactants.&lt;br /&gt;
==Analysis of Cl&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;==&lt;br /&gt;
===General Analysis===&lt;br /&gt;
Calculation method: RB3LYP&lt;br /&gt;
&lt;br /&gt;
Basis Set = 6-31G(d,p)&lt;br /&gt;
&lt;br /&gt;
Final Energy: E(RB3LYP) = -920.3498788 a.u.&lt;br /&gt;
&lt;br /&gt;
Bond length: 2.0417 Å&lt;br /&gt;
===Vibrational Analysis===&lt;br /&gt;
&amp;lt;pre&amp;gt;&lt;br /&gt;
 Item               Value     Threshold  Converged?&lt;br /&gt;
 Maximum Force            0.000043     0.000450     YES&lt;br /&gt;
 RMS     Force            0.000043     0.000300     YES&lt;br /&gt;
 Maximum Displacement     0.000121     0.001800     YES&lt;br /&gt;
 RMS     Displacement     0.000172     0.001200     YES&lt;br /&gt;
&lt;br /&gt;
&amp;lt;/pre&amp;gt;&lt;br /&gt;
&amp;lt;pre&amp;gt;&lt;br /&gt;
Vibrational mode    Frequency    Infrared&lt;br /&gt;
#1             520.32       0.0000&lt;br /&gt;
&amp;lt;/pre&amp;gt;&lt;br /&gt;
There are no vibrational modes with negative frequencies&lt;br /&gt;
===Charge Analysis===&lt;br /&gt;
[[File:Adrian_Popescu_Cl2_Charges2.png|400px|center]]&lt;br /&gt;
As the Cl&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; molecule is made up of identical Cl atoms, the bond between them will be 100% covalent, the electrons that form the sigma bond are equally shared between the Cl atoms, so the charge on each Cl atom is zero.&lt;br /&gt;
&lt;br /&gt;
===Molecular orbitals Analysis===&lt;br /&gt;
[[File:orbital1_.png|400px|thumb|center|2σ&amp;lt;sub&amp;gt;g&amp;lt;/sub&amp;gt; bonding orbital]]&lt;br /&gt;
The 2σ&amp;lt;sub&amp;gt;g&amp;lt;/sub&amp;gt; bonding orbital is deep in energy, occupied, and corresponds to the bonding orbital formed by the 2s AOs of the Cl atoms.&lt;br /&gt;
[[File:Adrian_Popescu_orbital2.png|400px|thumb|center|2σ&amp;lt;sub&amp;gt;u*&amp;lt;/sub&amp;gt; antibonding orbital]]&lt;br /&gt;
The 2σ&amp;lt;sub&amp;gt;u*&amp;lt;/sub&amp;gt; orbital is higher in energy than the 2σ&amp;lt;sub&amp;gt;g&amp;lt;/sub&amp;gt; orbital, is occupied, and corresponds to the antibonding orbital formed by the 2s AOs of the Cl atoms.&lt;br /&gt;
[[File:Adrian_Popescu_orbital3.png|400px|thumb|center|3σ&amp;lt;sub&amp;gt;g&amp;lt;/sub&amp;gt; bonding orbital]]&lt;br /&gt;
The 3σ&amp;lt;sub&amp;gt;g&amp;lt;/sub&amp;gt; orbital is deep in energy, occupied, and corresponds to the bonding orbital formed by the 3p&amp;lt;sub&amp;gt;x&amp;lt;/sub&amp;gt; AOs of the Cl atoms.&lt;br /&gt;
[[File:Adrian_Popescu_homo.png|400px|thumb|center|1π&amp;lt;sub&amp;gt;g*&amp;lt;/sub&amp;gt; antibonding orbital]]&lt;br /&gt;
The 1π&amp;lt;sub&amp;gt;g*&amp;lt;/sub&amp;gt; orbital is high in energy, and is the HOMO (Highest Occupied Molecular Orbital). It corresponds to the antibonding orbital formed by the 3p&amp;lt;sub&amp;gt;y&amp;lt;/sub&amp;gt; (or 3p&amp;lt;sub&amp;gt;z&amp;lt;/sub&amp;gt;, as the orbitals are degenerate) AOs of the Cl atoms.&lt;br /&gt;
[[File:Adrian_Popescu_lumo.png|400px|thumb|center|3σ&amp;lt;sub&amp;gt;u*&amp;lt;/sub&amp;gt; antibonding orbital]]&lt;br /&gt;
The 3σ&amp;lt;sub&amp;gt;u*&amp;lt;/sub&amp;gt; orbital is high in energy, and is the LUMO (Lowest Unoccupied Molecular Orbital). It corresponds to the antibonding orbital formed by the 3p&amp;lt;sub&amp;gt;x&amp;lt;/sub&amp;gt; AOs of the Cl atoms.&lt;/div&gt;</summary>
		<author><name>Ap5817</name></author>
	</entry>
	<entry>
		<id>https://chemwiki.ch.ic.ac.uk/index.php?title=User:Ap5817&amp;diff=680632</id>
		<title>User:Ap5817</title>
		<link rel="alternate" type="text/html" href="https://chemwiki.ch.ic.ac.uk/index.php?title=User:Ap5817&amp;diff=680632"/>
		<updated>2018-03-08T16:08:41Z</updated>

		<summary type="html">&lt;p&gt;Ap5817: &lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;== NH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt; molecule ==&lt;br /&gt;
=== NH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt; calculations ===&lt;br /&gt;
Calculation method:RB3LYP&lt;br /&gt;
&lt;br /&gt;
Basis Set = 6-31G(d,p)&lt;br /&gt;
&lt;br /&gt;
Final Energy: E(RB3LYP) = -56.557768 a.u.&lt;br /&gt;
&lt;br /&gt;
Bond length:1.01789 Å&lt;br /&gt;
&lt;br /&gt;
Bond angle: 105.741 °C&lt;br /&gt;
&lt;br /&gt;
Point Group: C3v&amp;lt;pre&amp;gt;&lt;br /&gt;
Item               Value     Threshold  Converged?&lt;br /&gt;
 Maximum Force            0.000004     0.000450     YES&lt;br /&gt;
 RMS     Force            0.000004     0.000300     YES&lt;br /&gt;
 Maximum Displacement     0.000072     0.001800     YES&lt;br /&gt;
 RMS     Displacement     0.000035     0.001200     YES&lt;br /&gt;
&amp;lt;/pre&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&amp;lt;jmol&amp;gt;&amp;lt;jmolApplet&amp;gt;&lt;br /&gt;
&amp;lt;script&amp;gt;frame x.y&amp;lt;/script&amp;gt;&lt;br /&gt;
  &amp;lt;title&amp;gt;test molecule&amp;lt;/title&amp;gt;&lt;br /&gt;
  &amp;lt;color&amp;gt;black&amp;lt;/color&amp;gt;&lt;br /&gt;
  &amp;lt;size&amp;gt;200&amp;lt;/size&amp;gt;&lt;br /&gt;
  &amp;lt;uploadedFileContents&amp;gt;ADRIAN_POPESCU_PHUNT_NH3_OPTF_POP.LOG&amp;lt;/uploadedFileContents&amp;gt;&lt;br /&gt;
&amp;lt;/jmolApplet&amp;gt;&amp;lt;/jmol&amp;gt;&lt;br /&gt;
&lt;br /&gt;
[[Media:ADRIAN_POPESCU_PHUNT_NH3_OPTF_POP.LOG]]&lt;br /&gt;
&lt;br /&gt;
==Vibration analysis of NH3==&lt;br /&gt;
[[File:Adrian_Popescu_Vibrations2.png|400px]]&lt;br /&gt;
===Vibrational modes===&lt;br /&gt;
Number of vibrational modes: 6&lt;br /&gt;
&lt;br /&gt;
Number of degenerate modes: 4 (2 pairs of degenerate vibrational modes )&lt;br /&gt;
&lt;br /&gt;
Number of bending motions: 3&lt;br /&gt;
&lt;br /&gt;
Number of stretching motions: 3&lt;br /&gt;
&lt;br /&gt;
The most symmetric vibrational mode: mode #4&lt;br /&gt;
&lt;br /&gt;
The &#039;&#039;umbrella mode&#039;&#039;: mode #1&lt;br /&gt;
&lt;br /&gt;
Number of bands expected to be seen in an experimental spectrum of gaseous ammonia: 5&lt;br /&gt;
===Charge Analysis===&lt;br /&gt;
[[File:Adrian_Popescu_Charges2.png|400px|center]]&lt;br /&gt;
&lt;br /&gt;
Charge on the N atom: -1.125&lt;br /&gt;
&lt;br /&gt;
Charge on the H atom: 0.375&lt;br /&gt;
&lt;br /&gt;
As Nitrogen has an electronegativity value of 3.04, which is significantly larger than the one of Hidrogen (2.2), it is expected that on the Nitrogen there will be a negative charge and on Hidrogen a possitive charge.&lt;br /&gt;
&lt;br /&gt;
==Reactivity of the Haber-Bosch process==&lt;br /&gt;
===Analysis of H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;===&lt;br /&gt;
Calculation method:RB3LYP&lt;br /&gt;
&lt;br /&gt;
Basis Set = 6-31G(d,p)&lt;br /&gt;
&lt;br /&gt;
Final Energy: E(RB3LYP) = -1.1785393 a.u.&lt;br /&gt;
&lt;br /&gt;
Bond length:0.7428 Å&lt;br /&gt;
&amp;lt;pre&amp;gt;&lt;br /&gt;
Item               Value     Threshold  Converged?&lt;br /&gt;
 Maximum Force            0.000004     0.000450     YES&lt;br /&gt;
 RMS     Force            0.000004     0.000300     YES&lt;br /&gt;
 Maximum Displacement     0.000005     0.001800     YES&lt;br /&gt;
 RMS     Displacement     0.000007     0.001200     YES&amp;lt;/pre&amp;gt;&lt;br /&gt;
&amp;lt;pre&amp;gt;&lt;br /&gt;
Vibrational mode    Frequency    Infrared&lt;br /&gt;
#1             4465.6       0.0000&lt;br /&gt;
&amp;lt;/pre&amp;gt;&lt;br /&gt;
There are no vibrational modes with negative frequencies&lt;br /&gt;
===Analysis of N&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;===&lt;br /&gt;
Calculation method: RB3LYP&lt;br /&gt;
&lt;br /&gt;
Basis Set = 6-31G(d,p)&lt;br /&gt;
&lt;br /&gt;
Final Energy: E(RB3LYP) = -109.5241268 a.u.&lt;br /&gt;
&lt;br /&gt;
Bond length: 1.1055 Å&lt;br /&gt;
&amp;lt;pre&amp;gt;&lt;br /&gt;
Item               Value     Threshold  Converged?&lt;br /&gt;
 Maximum Force            0.000001     0.000450     YES&lt;br /&gt;
 RMS     Force            0.000001     0.000300     YES&lt;br /&gt;
 Maximum Displacement     0.000000     0.001800     YES&lt;br /&gt;
 RMS     Displacement     0.000000     0.001200     YES&lt;br /&gt;
&amp;lt;/pre&amp;gt;&lt;br /&gt;
&amp;lt;pre&amp;gt;&lt;br /&gt;
Vibrational mode    Frequency    Infrared&lt;br /&gt;
#1             2457.33       0.0000&lt;br /&gt;
&amp;lt;/pre&amp;gt;&lt;br /&gt;
There are no vibrational modes with negative frequencies.&lt;br /&gt;
&lt;br /&gt;
===Calculation of the energy of the Haber-Bosch process===&lt;br /&gt;
N&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; + 3H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; -&amp;gt; 2NH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;&lt;br /&gt;
&lt;br /&gt;
E(NH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;)= -56.557768 a u&lt;br /&gt;
&lt;br /&gt;
2*E(NH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;)= -113.115536 a u&lt;br /&gt;
&lt;br /&gt;
E(N&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;)= -109.5251268 a u&lt;br /&gt;
&lt;br /&gt;
E(H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;)= -1.1785393 a u&lt;br /&gt;
&lt;br /&gt;
3*E(H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;)= -3.5359617 a u&lt;br /&gt;
&lt;br /&gt;
ΔE=2*E(NH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;) - [E(N&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;) + 3*E(H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;)] = -145.57 kj/mol&lt;br /&gt;
&lt;br /&gt;
As the reaction is exothermic, the ammonia product is more stable than the gaseous reactants.&lt;br /&gt;
==Analysis of Cl&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;==&lt;br /&gt;
===General Analysis===&lt;br /&gt;
Calculation method: RB3LYP&lt;br /&gt;
&lt;br /&gt;
Basis Set = 6-31G(d,p)&lt;br /&gt;
&lt;br /&gt;
Final Energy: E(RB3LYP) = -920.3498788 a.u.&lt;br /&gt;
&lt;br /&gt;
Bond length: 2.0417 Å&lt;br /&gt;
===Vibrational Analysis===&lt;br /&gt;
&amp;lt;pre&amp;gt;&lt;br /&gt;
 Item               Value     Threshold  Converged?&lt;br /&gt;
 Maximum Force            0.000043     0.000450     YES&lt;br /&gt;
 RMS     Force            0.000043     0.000300     YES&lt;br /&gt;
 Maximum Displacement     0.000121     0.001800     YES&lt;br /&gt;
 RMS     Displacement     0.000172     0.001200     YES&lt;br /&gt;
&lt;br /&gt;
&amp;lt;/pre&amp;gt;&lt;br /&gt;
&amp;lt;pre&amp;gt;&lt;br /&gt;
Vibrational mode    Frequency    Infrared&lt;br /&gt;
#1             520.32       0.0000&lt;br /&gt;
&amp;lt;/pre&amp;gt;&lt;br /&gt;
There are no vibrational modes with negative frequencies&lt;br /&gt;
===Charge Analysis===&lt;br /&gt;
[[File:Adrian_Popescu_Cl2_Charges2.png|400px|center]]&lt;br /&gt;
As the Cl&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; molecule is made up of identical Cl atoms, the bond between them will be 100% covalent, the electrons that form the sigma bond are equally shared between the Cl atoms, so the charge on each Cl atom is zero.&lt;br /&gt;
&lt;br /&gt;
===Molecular orbitals Analysis===&lt;br /&gt;
[[File:orbital1_.png|400px|thumb|center|2σ&amp;lt;sub&amp;gt;g&amp;lt;/sub&amp;gt; bonding orbital]]&lt;br /&gt;
The 2σ&amp;lt;sub&amp;gt;g&amp;lt;/sub&amp;gt; bonding orbital is deep in energy, occupied, and corresponds to the bonding orbital formed by the 2s AOs of the Cl atoms.&lt;br /&gt;
[[File:Adrian_Popescu_orbital2.png|400px|thumb|center|2σ&amp;lt;sub&amp;gt;u*&amp;lt;/sub&amp;gt; antibonding orbital]]&lt;br /&gt;
The 2σ&amp;lt;sub&amp;gt;u*&amp;lt;/sub&amp;gt; orbital is higher in energy than the 2σ&amp;lt;sub&amp;gt;g&amp;lt;/sub&amp;gt; orbital, is occupied, and corresponds to the antibonding orbital formed by the 2s AOs of the Cl atoms.&lt;br /&gt;
[[File:Adrian_Popescu_orbital3.png|400px|thumb|center|3σ&amp;lt;sub&amp;gt;g&amp;lt;/sub&amp;gt; bonding orbital]]&lt;br /&gt;
The 3σ&amp;lt;sub&amp;gt;g&amp;lt;/sub&amp;gt; orbital is deep in energy, occupied, and corresponds to the bonding orbital formed by the 3p&amp;lt;sub&amp;gt;x&amp;lt;/sub&amp;gt; AOs of the Cl atoms.&lt;br /&gt;
[[File:Adrian_Popescu_homo.png|400px|thumb|center|1π&amp;lt;sub&amp;gt;g*&amp;lt;/sub&amp;gt; antibonding orbital]]&lt;br /&gt;
The 1π&amp;lt;sub&amp;gt;g*&amp;lt;/sub&amp;gt; orbital is high in energy, and is the HOMO (Highest Occupied Molecular Orbital). It corresponds to the antibonding orbital formed by the 3p&amp;lt;sub&amp;gt;y&amp;lt;/sub&amp;gt; (or 3p&amp;lt;sub&amp;gt;z&amp;lt;/sub&amp;gt;, as the orbitals are degenerate) AOs of the Cl atoms.&lt;br /&gt;
[[File:Adrian_Popescu_lumo.png|400px|thumb|center|3σ&amp;lt;sub&amp;gt;u*&amp;lt;/sub&amp;gt; antibonding orbital]]&lt;br /&gt;
The 3σ&amp;lt;sub&amp;gt;u*&amp;lt;/sub&amp;gt; orbital is high in energy, and is the LUMO (Lowest Unoccupied Molecular Orbital). It corresponds to the antibonding orbital formed by the 3p&amp;lt;sub&amp;gt;x&amp;lt;/sub&amp;gt; AOs of the Cl atoms.&lt;/div&gt;</summary>
		<author><name>Ap5817</name></author>
	</entry>
	<entry>
		<id>https://chemwiki.ch.ic.ac.uk/index.php?title=User:Ap5817&amp;diff=680631</id>
		<title>User:Ap5817</title>
		<link rel="alternate" type="text/html" href="https://chemwiki.ch.ic.ac.uk/index.php?title=User:Ap5817&amp;diff=680631"/>
		<updated>2018-03-08T16:08:08Z</updated>

		<summary type="html">&lt;p&gt;Ap5817: &lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;== NH3 molecule ==&lt;br /&gt;
=== NH3 calculations ===&lt;br /&gt;
Calculation method:RB3LYP&lt;br /&gt;
&lt;br /&gt;
Basis Set = 6-31G(d,p)&lt;br /&gt;
&lt;br /&gt;
Final Energy: E(RB3LYP) = -56.557768 a.u.&lt;br /&gt;
&lt;br /&gt;
Bond length:1.01789 Å&lt;br /&gt;
&lt;br /&gt;
Bond angle: 105.741 °C&lt;br /&gt;
&lt;br /&gt;
Point Group: C3v&amp;lt;pre&amp;gt;&lt;br /&gt;
Item               Value     Threshold  Converged?&lt;br /&gt;
 Maximum Force            0.000004     0.000450     YES&lt;br /&gt;
 RMS     Force            0.000004     0.000300     YES&lt;br /&gt;
 Maximum Displacement     0.000072     0.001800     YES&lt;br /&gt;
 RMS     Displacement     0.000035     0.001200     YES&lt;br /&gt;
&amp;lt;/pre&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&amp;lt;jmol&amp;gt;&amp;lt;jmolApplet&amp;gt;&lt;br /&gt;
&amp;lt;script&amp;gt;frame x.y&amp;lt;/script&amp;gt;&lt;br /&gt;
  &amp;lt;title&amp;gt;test molecule&amp;lt;/title&amp;gt;&lt;br /&gt;
  &amp;lt;color&amp;gt;black&amp;lt;/color&amp;gt;&lt;br /&gt;
  &amp;lt;size&amp;gt;200&amp;lt;/size&amp;gt;&lt;br /&gt;
  &amp;lt;uploadedFileContents&amp;gt;ADRIAN_POPESCU_PHUNT_NH3_OPTF_POP.LOG&amp;lt;/uploadedFileContents&amp;gt;&lt;br /&gt;
&amp;lt;/jmolApplet&amp;gt;&amp;lt;/jmol&amp;gt;&lt;br /&gt;
&lt;br /&gt;
[[Media:ADRIAN_POPESCU_PHUNT_NH3_OPTF_POP.LOG]]&lt;br /&gt;
&lt;br /&gt;
==Vibration analysis of NH3==&lt;br /&gt;
[[File:Adrian_Popescu_Vibrations2.png|400px]]&lt;br /&gt;
===Vibrational modes===&lt;br /&gt;
Number of vibrational modes: 6&lt;br /&gt;
&lt;br /&gt;
Number of degenerate modes: 4 (2 pairs of degenerate vibrational modes )&lt;br /&gt;
&lt;br /&gt;
Number of bending motions: 3&lt;br /&gt;
&lt;br /&gt;
Number of stretching motions: 3&lt;br /&gt;
&lt;br /&gt;
The most symmetric vibrational mode: mode #4&lt;br /&gt;
&lt;br /&gt;
The &#039;&#039;umbrella mode&#039;&#039;: mode #1&lt;br /&gt;
&lt;br /&gt;
Number of bands expected to be seen in an experimental spectrum of gaseous ammonia: 5&lt;br /&gt;
===Charge Analysis===&lt;br /&gt;
[[File:Adrian_Popescu_Charges2.png|400px|center]]&lt;br /&gt;
&lt;br /&gt;
Charge on the N atom: -1.125&lt;br /&gt;
&lt;br /&gt;
Charge on the H atom: 0.375&lt;br /&gt;
&lt;br /&gt;
As Nitrogen has an electronegativity value of 3.04, which is significantly larger than the one of Hidrogen (2.2), it is expected that on the Nitrogen there will be a negative charge and on Hidrogen a possitive charge.&lt;br /&gt;
&lt;br /&gt;
==Reactivity of the Haber-Bosch process==&lt;br /&gt;
===Analysis of H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;===&lt;br /&gt;
Calculation method:RB3LYP&lt;br /&gt;
&lt;br /&gt;
Basis Set = 6-31G(d,p)&lt;br /&gt;
&lt;br /&gt;
Final Energy: E(RB3LYP) = -1.1785393 a.u.&lt;br /&gt;
&lt;br /&gt;
Bond length:0.7428 Å&lt;br /&gt;
&amp;lt;pre&amp;gt;&lt;br /&gt;
Item               Value     Threshold  Converged?&lt;br /&gt;
 Maximum Force            0.000004     0.000450     YES&lt;br /&gt;
 RMS     Force            0.000004     0.000300     YES&lt;br /&gt;
 Maximum Displacement     0.000005     0.001800     YES&lt;br /&gt;
 RMS     Displacement     0.000007     0.001200     YES&amp;lt;/pre&amp;gt;&lt;br /&gt;
&amp;lt;pre&amp;gt;&lt;br /&gt;
Vibrational mode    Frequency    Infrared&lt;br /&gt;
#1             4465.6       0.0000&lt;br /&gt;
&amp;lt;/pre&amp;gt;&lt;br /&gt;
There are no vibrational modes with negative frequencies&lt;br /&gt;
===Analysis of N&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;===&lt;br /&gt;
Calculation method: RB3LYP&lt;br /&gt;
&lt;br /&gt;
Basis Set = 6-31G(d,p)&lt;br /&gt;
&lt;br /&gt;
Final Energy: E(RB3LYP) = -109.5241268 a.u.&lt;br /&gt;
&lt;br /&gt;
Bond length: 1.1055 Å&lt;br /&gt;
&amp;lt;pre&amp;gt;&lt;br /&gt;
Item               Value     Threshold  Converged?&lt;br /&gt;
 Maximum Force            0.000001     0.000450     YES&lt;br /&gt;
 RMS     Force            0.000001     0.000300     YES&lt;br /&gt;
 Maximum Displacement     0.000000     0.001800     YES&lt;br /&gt;
 RMS     Displacement     0.000000     0.001200     YES&lt;br /&gt;
&amp;lt;/pre&amp;gt;&lt;br /&gt;
&amp;lt;pre&amp;gt;&lt;br /&gt;
Vibrational mode    Frequency    Infrared&lt;br /&gt;
#1             2457.33       0.0000&lt;br /&gt;
&amp;lt;/pre&amp;gt;&lt;br /&gt;
There are no vibrational modes with negative frequencies.&lt;br /&gt;
&lt;br /&gt;
===Calculation of the energy of the Haber-Bosch process===&lt;br /&gt;
N&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; + 3H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; -&amp;gt; 2NH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;&lt;br /&gt;
&lt;br /&gt;
E(NH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;)= -56.557768 a u&lt;br /&gt;
&lt;br /&gt;
2*E(NH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;)= -113.115536 a u&lt;br /&gt;
&lt;br /&gt;
E(N&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;)= -109.5251268 a u&lt;br /&gt;
&lt;br /&gt;
E(H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;)= -1.1785393 a u&lt;br /&gt;
&lt;br /&gt;
3*E(H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;)= -3.5359617 a u&lt;br /&gt;
&lt;br /&gt;
ΔE=2*E(NH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;) - [E(N&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;) + 3*E(H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;)] = -145.57 kj/mol&lt;br /&gt;
&lt;br /&gt;
As the reaction is exothermic, the ammonia product is more stable than the gaseous reactants.&lt;br /&gt;
==Analysis of Cl&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;==&lt;br /&gt;
===General Analysis===&lt;br /&gt;
Calculation method: RB3LYP&lt;br /&gt;
&lt;br /&gt;
Basis Set = 6-31G(d,p)&lt;br /&gt;
&lt;br /&gt;
Final Energy: E(RB3LYP) = -920.3498788 a.u.&lt;br /&gt;
&lt;br /&gt;
Bond length: 2.0417 Å&lt;br /&gt;
===Vibrational Analysis===&lt;br /&gt;
&amp;lt;pre&amp;gt;&lt;br /&gt;
 Item               Value     Threshold  Converged?&lt;br /&gt;
 Maximum Force            0.000043     0.000450     YES&lt;br /&gt;
 RMS     Force            0.000043     0.000300     YES&lt;br /&gt;
 Maximum Displacement     0.000121     0.001800     YES&lt;br /&gt;
 RMS     Displacement     0.000172     0.001200     YES&lt;br /&gt;
&lt;br /&gt;
&amp;lt;/pre&amp;gt;&lt;br /&gt;
&amp;lt;pre&amp;gt;&lt;br /&gt;
Vibrational mode    Frequency    Infrared&lt;br /&gt;
#1             520.32       0.0000&lt;br /&gt;
&amp;lt;/pre&amp;gt;&lt;br /&gt;
There are no vibrational modes with negative frequencies&lt;br /&gt;
===Charge Analysis===&lt;br /&gt;
[[File:Adrian_Popescu_Cl2_Charges2.png|400px|center]]&lt;br /&gt;
As the Cl&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; molecule is made up of identical Cl atoms, the bond between them will be 100% covalent, the electrons that form the sigma bond are equally shared between the Cl atoms, so the charge on each Cl atom is zero.&lt;br /&gt;
&lt;br /&gt;
===Molecular orbitals Analysis===&lt;br /&gt;
[[File:orbital1_.png|400px|thumb|center|2σ&amp;lt;sub&amp;gt;g&amp;lt;/sub&amp;gt; bonding orbital]]&lt;br /&gt;
The 2σ&amp;lt;sub&amp;gt;g&amp;lt;/sub&amp;gt; bonding orbital is deep in energy, occupied, and corresponds to the bonding orbital formed by the 2s AOs of the Cl atoms.&lt;br /&gt;
[[File:Adrian_Popescu_orbital2.png|400px|thumb|center|2σ&amp;lt;sub&amp;gt;u*&amp;lt;/sub&amp;gt; antibonding orbital]]&lt;br /&gt;
The 2σ&amp;lt;sub&amp;gt;u*&amp;lt;/sub&amp;gt; orbital is higher in energy than the 2σ&amp;lt;sub&amp;gt;g&amp;lt;/sub&amp;gt; orbital, is occupied, and corresponds to the antibonding orbital formed by the 2s AOs of the Cl atoms.&lt;br /&gt;
[[File:Adrian_Popescu_orbital3.png|400px|thumb|center|3σ&amp;lt;sub&amp;gt;g&amp;lt;/sub&amp;gt; bonding orbital]]&lt;br /&gt;
The 3σ&amp;lt;sub&amp;gt;g&amp;lt;/sub&amp;gt; orbital is deep in energy, occupied, and corresponds to the bonding orbital formed by the 3p&amp;lt;sub&amp;gt;x&amp;lt;/sub&amp;gt; AOs of the Cl atoms.&lt;br /&gt;
[[File:Adrian_Popescu_homo.png|400px|thumb|center|1π&amp;lt;sub&amp;gt;g*&amp;lt;/sub&amp;gt; antibonding orbital]]&lt;br /&gt;
The 1π&amp;lt;sub&amp;gt;g*&amp;lt;/sub&amp;gt; orbital is high in energy, and is the HOMO (Highest Occupied Molecular Orbital). It corresponds to the antibonding orbital formed by the 3p&amp;lt;sub&amp;gt;y&amp;lt;/sub&amp;gt; (or 3p&amp;lt;sub&amp;gt;z&amp;lt;/sub&amp;gt;, as the orbitals are degenerate) AOs of the Cl atoms.&lt;br /&gt;
[[File:Adrian_Popescu_lumo.png|400px|thumb|center|3σ&amp;lt;sub&amp;gt;u*&amp;lt;/sub&amp;gt; antibonding orbital]]&lt;br /&gt;
The 3σ&amp;lt;sub&amp;gt;u*&amp;lt;/sub&amp;gt; orbital is high in energy, and is the LUMO (Lowest Unoccupied Molecular Orbital). It corresponds to the antibonding orbital formed by the 3p&amp;lt;sub&amp;gt;x&amp;lt;/sub&amp;gt; AOs of the Cl atoms.&lt;/div&gt;</summary>
		<author><name>Ap5817</name></author>
	</entry>
	<entry>
		<id>https://chemwiki.ch.ic.ac.uk/index.php?title=User:Ap5817&amp;diff=680372</id>
		<title>User:Ap5817</title>
		<link rel="alternate" type="text/html" href="https://chemwiki.ch.ic.ac.uk/index.php?title=User:Ap5817&amp;diff=680372"/>
		<updated>2018-03-08T12:21:37Z</updated>

		<summary type="html">&lt;p&gt;Ap5817: &lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;== NH3 molecule ==&lt;br /&gt;
=== NH3 calculations ===&lt;br /&gt;
Calculation method:RB3LYP&lt;br /&gt;
&lt;br /&gt;
Basis Set = 6-31G(d,p)&lt;br /&gt;
&lt;br /&gt;
Final Energy: E(RB3LYP) = -56.557768 a.u.&lt;br /&gt;
&lt;br /&gt;
Bond length:1.01789 Å&lt;br /&gt;
&lt;br /&gt;
Bond angle: 105.741 °C&lt;br /&gt;
&lt;br /&gt;
Point Group: C3v&amp;lt;pre&amp;gt;&lt;br /&gt;
Item               Value     Threshold  Converged?&lt;br /&gt;
 Maximum Force            0.000004     0.000450     YES&lt;br /&gt;
 RMS     Force            0.000004     0.000300     YES&lt;br /&gt;
 Maximum Displacement     0.000072     0.001800     YES&lt;br /&gt;
 RMS     Displacement     0.000035     0.001200     YES&lt;br /&gt;
&amp;lt;/pre&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&amp;lt;jmol&amp;gt;&amp;lt;jmolApplet&amp;gt;&lt;br /&gt;
&amp;lt;script&amp;gt;frame x.y&amp;lt;/script&amp;gt;&lt;br /&gt;
  &amp;lt;title&amp;gt;test molecule&amp;lt;/title&amp;gt;&lt;br /&gt;
  &amp;lt;color&amp;gt;black&amp;lt;/color&amp;gt;&lt;br /&gt;
  &amp;lt;size&amp;gt;200&amp;lt;/size&amp;gt;&lt;br /&gt;
  &amp;lt;uploadedFileContents&amp;gt;ADRIAN_POPESCU_PHUNT_NH3_OPTF_POP.LOG&amp;lt;/uploadedFileContents&amp;gt;&lt;br /&gt;
&amp;lt;/jmolApplet&amp;gt;&amp;lt;/jmol&amp;gt;&lt;br /&gt;
&lt;br /&gt;
[[Media:ADRIAN_POPESCU_PHUNT_NH3_OPTF_POP.LOG]]&lt;br /&gt;
&lt;br /&gt;
==Vibration analysis of NH3==&lt;br /&gt;
[[File:Adrian_Popescu_Vibrations2.png|400px]]&lt;br /&gt;
===Vibrational modes===&lt;br /&gt;
Number of vibrational modes: 6&lt;br /&gt;
&lt;br /&gt;
Number of degenerate modes: 4 (2 pairs of degenerate vibrational modes )&lt;br /&gt;
&lt;br /&gt;
Number of bending motions: 3&lt;br /&gt;
&lt;br /&gt;
Number of stretching motions: 3&lt;br /&gt;
&lt;br /&gt;
The most symmetric vibrational mode: mode #4&lt;br /&gt;
&lt;br /&gt;
The &#039;&#039;umbrella mode&#039;&#039;: mode #1&lt;br /&gt;
&lt;br /&gt;
Number of bands expected to be seen in an experimental spectrum of gaseous ammonia: 5&lt;br /&gt;
===Charge Analysis===&lt;br /&gt;
[[File:Adrian_Popescu_Charges2.png|400px|center]]&lt;br /&gt;
&lt;br /&gt;
Charge on the N atom: -1.125&lt;br /&gt;
&lt;br /&gt;
Charge on the H atom: 0.375&lt;br /&gt;
&lt;br /&gt;
As Nitrogen has an electronegativity value of 3.04, which is significantly larger than the one of Hidrogen (2.2), it is expected that on the Nitrogen there will be a negative charge and on Hidrogen a possitive charge.&lt;br /&gt;
&lt;br /&gt;
==Reactivity of the Haber-Bosch process==&lt;br /&gt;
===Analysis of H&amp;lt;sup&amp;gt;2&amp;lt;/sup&amp;gt;===&lt;br /&gt;
Calculation method:RB3LYP&lt;br /&gt;
&lt;br /&gt;
Basis Set = 6-31G(d,p)&lt;br /&gt;
&lt;br /&gt;
Final Energy: E(RB3LYP) = -1.1785393 a.u.&lt;br /&gt;
&lt;br /&gt;
Bond length:0.7428 Å&lt;br /&gt;
&amp;lt;pre&amp;gt;&lt;br /&gt;
Item               Value     Threshold  Converged?&lt;br /&gt;
 Maximum Force            0.000004     0.000450     YES&lt;br /&gt;
 RMS     Force            0.000004     0.000300     YES&lt;br /&gt;
 Maximum Displacement     0.000005     0.001800     YES&lt;br /&gt;
 RMS     Displacement     0.000007     0.001200     YES&amp;lt;/pre&amp;gt;&lt;br /&gt;
&amp;lt;pre&amp;gt;&lt;br /&gt;
Vibrational mode    Frequency    Infrared&lt;br /&gt;
#1             4465.6       0.0000&lt;br /&gt;
&amp;lt;/pre&amp;gt;&lt;br /&gt;
There are no vibrational modes with negative frequencies&lt;br /&gt;
===Analysis of N&amp;lt;sup&amp;gt;2&amp;lt;/sup&amp;gt;===&lt;br /&gt;
Calculation method: RB3LYP&lt;br /&gt;
&lt;br /&gt;
Basis Set = 6-31G(d,p)&lt;br /&gt;
&lt;br /&gt;
Final Energy: E(RB3LYP) = -109.5241268 a.u.&lt;br /&gt;
&lt;br /&gt;
Bond length: 1.1055 Å&lt;br /&gt;
&amp;lt;pre&amp;gt;&lt;br /&gt;
Item               Value     Threshold  Converged?&lt;br /&gt;
 Maximum Force            0.000001     0.000450     YES&lt;br /&gt;
 RMS     Force            0.000001     0.000300     YES&lt;br /&gt;
 Maximum Displacement     0.000000     0.001800     YES&lt;br /&gt;
 RMS     Displacement     0.000000     0.001200     YES&lt;br /&gt;
&amp;lt;/pre&amp;gt;&lt;br /&gt;
&amp;lt;pre&amp;gt;&lt;br /&gt;
Vibrational mode    Frequency    Infrared&lt;br /&gt;
#1             2457.33       0.0000&lt;br /&gt;
&amp;lt;/pre&amp;gt;&lt;br /&gt;
There are no vibrational modes with negative frequencies&lt;br /&gt;
&lt;br /&gt;
===Calculation of the energy of the Haber-Bosch process===&lt;br /&gt;
N&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; + 3H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; -&amp;gt; 2NH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;&lt;br /&gt;
&lt;br /&gt;
E(NH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;)= -56.557768 a u&lt;br /&gt;
&lt;br /&gt;
2*E(NH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;)= -113.115536 a u&lt;br /&gt;
&lt;br /&gt;
E(N&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;)= -109.5251268 a u&lt;br /&gt;
&lt;br /&gt;
E(H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;)= -1.1785393 a u&lt;br /&gt;
&lt;br /&gt;
3*E(H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;)= -3.5359617 a u&lt;br /&gt;
&lt;br /&gt;
ΔE=2*E(NH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;) - [E(N&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;) + 3*E(H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;)] = -145.57 kj/mol&lt;br /&gt;
&lt;br /&gt;
As the reaction is exothermic, the ammonia product is more stable than the gaseous reactants.&lt;br /&gt;
==Analysis of Cl&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;==&lt;br /&gt;
===General Analysis===&lt;br /&gt;
Calculation method: RB3LYP&lt;br /&gt;
&lt;br /&gt;
Basis Set = 6-31G(d,p)&lt;br /&gt;
&lt;br /&gt;
Final Energy: E(RB3LYP) = -920.3498788 a.u.&lt;br /&gt;
&lt;br /&gt;
Bond length: 2.0417 Å&lt;br /&gt;
===Vibrational Analysis===&lt;br /&gt;
&amp;lt;pre&amp;gt;&lt;br /&gt;
 Item               Value     Threshold  Converged?&lt;br /&gt;
 Maximum Force            0.000043     0.000450     YES&lt;br /&gt;
 RMS     Force            0.000043     0.000300     YES&lt;br /&gt;
 Maximum Displacement     0.000121     0.001800     YES&lt;br /&gt;
 RMS     Displacement     0.000172     0.001200     YES&lt;br /&gt;
&lt;br /&gt;
&amp;lt;/pre&amp;gt;&lt;br /&gt;
&amp;lt;pre&amp;gt;&lt;br /&gt;
Vibrational mode    Frequency    Infrared&lt;br /&gt;
#1             520.32       0.0000&lt;br /&gt;
&amp;lt;/pre&amp;gt;&lt;br /&gt;
There are no vibrational modes with negative frequencies&lt;br /&gt;
===Charge Analysis===&lt;br /&gt;
[[File:Adrian_Popescu_Cl2_Charges2.png|400px|center]]&lt;br /&gt;
As the Cl&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; molecule is made up of identical Cl atoms, the bond between them will be 100% covalent, the electrons that form the sigma bond are equally shared between the cl atoms, so the charge on each Cl atom is zero.&lt;br /&gt;
&lt;br /&gt;
===Molecular orbitals Analysis===&lt;br /&gt;
[[File:orbital1_.png|400px|thumb|center|2σ&amp;lt;sup&amp;gt;g&amp;lt;/sup&amp;gt; bonding orbital]]&lt;br /&gt;
The 2σ&amp;lt;sup&amp;gt;g&amp;lt;/sup&amp;gt; bonding orbital is deep in energy, occupied, and corresponds to the bonding orbital formed by the 2s AOs of the Cl atoms.&lt;br /&gt;
[[File:Adrian_Popescu_orbital2.png|400px|thumb|center|2σ&amp;lt;sup&amp;gt;u*&amp;lt;/sup&amp;gt; antibonding orbital]]&lt;br /&gt;
The 2σ&amp;lt;sup&amp;gt;u*&amp;lt;/sup&amp;gt; orbital is higher in energy than the 2σ&amp;lt;sup&amp;gt;g&amp;lt;/sup&amp;gt; orbital, is occupied, and corresponds to the antibonding orbital formed by the 2s AOs of the Cl atoms.&lt;br /&gt;
[[File:Adrian_Popescu_orbital3.png|400px|thumb|center|3σ&amp;lt;sup&amp;gt;g&amp;lt;/sup&amp;gt; bonding orbital]]&lt;br /&gt;
The 3σ&amp;lt;sup&amp;gt;g&amp;lt;/sup&amp;gt; orbital is deep in energy, occupied, and corresponds to the bonding orbital formed by the 3p&amp;lt;sup&amp;gt;x&amp;lt;/sup&amp;gt; AOs of the Cl atoms.&lt;br /&gt;
[[File:Adrian_Popescu_homo.png|400px|thumb|center|1π&amp;lt;sup&amp;gt;g*&amp;lt;/sup&amp;gt; antibonding orbital]]&lt;br /&gt;
The 1π&amp;lt;sup&amp;gt;g*&amp;lt;/sup&amp;gt; orbital is high in energy, and is the HOMO (Highest Occupied Molecular Orbital). It corresponds to the antibonding orbital formed by the 3p&amp;lt;sup&amp;gt;y&amp;lt;/sup&amp;gt; (or 3p&amp;lt;sup&amp;gt;z&amp;lt;/sup&amp;gt;, as the orbitals are degenerate) AOs of the Cl atoms.&lt;br /&gt;
[[File:Adrian_Popescu_lumo.png|400px|thumb|center|3σ&amp;lt;sup&amp;gt;u*&amp;lt;/sup&amp;gt; antibonding orbital]]&lt;br /&gt;
The 3σ&amp;lt;sup&amp;gt;u*&amp;lt;/sup&amp;gt; orbital is high in energy, and is the LUMO (Lowest Unoccupied Molecular Orbital). It corresponds to the antibonding orbital formed by the 3p&amp;lt;sup&amp;gt;x&amp;lt;/sup&amp;gt; AOs of the Cl atoms.&lt;/div&gt;</summary>
		<author><name>Ap5817</name></author>
	</entry>
	<entry>
		<id>https://chemwiki.ch.ic.ac.uk/index.php?title=User:Ap5817&amp;diff=680339</id>
		<title>User:Ap5817</title>
		<link rel="alternate" type="text/html" href="https://chemwiki.ch.ic.ac.uk/index.php?title=User:Ap5817&amp;diff=680339"/>
		<updated>2018-03-08T12:05:14Z</updated>

		<summary type="html">&lt;p&gt;Ap5817: /* Vibration analysis of NH3 */&lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;== NH3 molecule ==&lt;br /&gt;
=== NH3 calculations ===&lt;br /&gt;
Calculation method:RB3LYP&lt;br /&gt;
&lt;br /&gt;
Basis Set = 6-31G(d,p)&lt;br /&gt;
&lt;br /&gt;
Final Energy: E(RB3LYP) = -56.557768 a.u.&lt;br /&gt;
&lt;br /&gt;
Bond length:1.01789 Å&lt;br /&gt;
&lt;br /&gt;
Bond angle: 105.741 °C&lt;br /&gt;
&lt;br /&gt;
Point Group: C3v&amp;lt;pre&amp;gt;&lt;br /&gt;
Item               Value     Threshold  Converged?&lt;br /&gt;
 Maximum Force            0.000004     0.000450     YES&lt;br /&gt;
 RMS     Force            0.000004     0.000300     YES&lt;br /&gt;
 Maximum Displacement     0.000072     0.001800     YES&lt;br /&gt;
 RMS     Displacement     0.000035     0.001200     YES&lt;br /&gt;
&amp;lt;/pre&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&amp;lt;jmol&amp;gt;&amp;lt;jmolApplet&amp;gt;&lt;br /&gt;
&amp;lt;script&amp;gt;frame x.y&amp;lt;/script&amp;gt;&lt;br /&gt;
  &amp;lt;title&amp;gt;test molecule&amp;lt;/title&amp;gt;&lt;br /&gt;
  &amp;lt;color&amp;gt;black&amp;lt;/color&amp;gt;&lt;br /&gt;
  &amp;lt;size&amp;gt;200&amp;lt;/size&amp;gt;&lt;br /&gt;
  &amp;lt;uploadedFileContents&amp;gt;ADRIAN_POPESCU_PHUNT_NH3_OPTF_POP.LOG&amp;lt;/uploadedFileContents&amp;gt;&lt;br /&gt;
&amp;lt;/jmolApplet&amp;gt;&amp;lt;/jmol&amp;gt;&lt;br /&gt;
&lt;br /&gt;
[[Media:ADRIAN_POPESCU_PHUNT_NH3_OPTF_POP.LOG]]&lt;br /&gt;
&lt;br /&gt;
==Vibration analysis of NH3==&lt;br /&gt;
[[File:Adrian_Popescu_Vibrations2.png|400px]]&lt;br /&gt;
===Vibrational modes===&lt;br /&gt;
Number of vibrational modes: 6&lt;br /&gt;
&lt;br /&gt;
Number of degenerate modes: 4 (2 pairs of degenerate vibrational modes &lt;br /&gt;
&lt;br /&gt;
Number of bending motions: 3&lt;br /&gt;
&lt;br /&gt;
Number of stretching motions: 3&lt;br /&gt;
&lt;br /&gt;
The most symmetric vibrational mode: mode #4&lt;br /&gt;
&lt;br /&gt;
The &#039;&#039;umbrella mode&#039;&#039;: mode #1&lt;br /&gt;
&lt;br /&gt;
Number of bands expected to be seen in an experimental spectrum of gaseous ammonia: 5&lt;br /&gt;
===Charge Analysis===&lt;br /&gt;
[[File:Adrian_Popescu_Charges2.png|400px|center]]&lt;br /&gt;
&lt;br /&gt;
Charge on the N atom: -1.125&lt;br /&gt;
&lt;br /&gt;
Charge on the H atom: 0.375&lt;br /&gt;
&lt;br /&gt;
As Nitrogen has an electronegativity value of 3.04, which is significantly larger than the one of Hidrogen (2.2), it is expected that on the Nitrogen there will be a negative charge and on Hidrogen a possitive charge.&lt;br /&gt;
&lt;br /&gt;
==Reactivity of the Haber-Bosch process==&lt;br /&gt;
===Analysis of H2===&lt;br /&gt;
Calculation method:RB3LYP&lt;br /&gt;
&lt;br /&gt;
Basis Set = 6-31G(d,p)&lt;br /&gt;
&lt;br /&gt;
Final Energy: E(RB3LYP) = -1.1785393 a.u.&lt;br /&gt;
&lt;br /&gt;
Bond length:0.7428 Å&lt;br /&gt;
&amp;lt;pre&amp;gt;&lt;br /&gt;
Item               Value     Threshold  Converged?&lt;br /&gt;
 Maximum Force            0.000004     0.000450     YES&lt;br /&gt;
 RMS     Force            0.000004     0.000300     YES&lt;br /&gt;
 Maximum Displacement     0.000005     0.001800     YES&lt;br /&gt;
 RMS     Displacement     0.000007     0.001200     YES&amp;lt;/pre&amp;gt;&lt;br /&gt;
&amp;lt;pre&amp;gt;&lt;br /&gt;
Vibrational mode    Frequency    Infrared&lt;br /&gt;
#1             4465.6       0.0000&lt;br /&gt;
&amp;lt;/pre&amp;gt;&lt;br /&gt;
There are no vibrational modes with negative frequencies&lt;br /&gt;
===Analysis of N2===&lt;br /&gt;
Calculation method:RB3LYP&lt;br /&gt;
&lt;br /&gt;
Basis Set = 6-31G(d,p)&lt;br /&gt;
&lt;br /&gt;
Final Energy: E(RB3LYP) = -109.5241268 a.u.&lt;br /&gt;
&lt;br /&gt;
Bond length: 1.1055 Å&lt;br /&gt;
&amp;lt;pre&amp;gt;&lt;br /&gt;
Item               Value     Threshold  Converged?&lt;br /&gt;
 Maximum Force            0.000001     0.000450     YES&lt;br /&gt;
 RMS     Force            0.000001     0.000300     YES&lt;br /&gt;
 Maximum Displacement     0.000000     0.001800     YES&lt;br /&gt;
 RMS     Displacement     0.000000     0.001200     YES&lt;br /&gt;
&amp;lt;/pre&amp;gt;&lt;br /&gt;
&amp;lt;pre&amp;gt;&lt;br /&gt;
Vibrational mode    Frequency    Infrared&lt;br /&gt;
#1             2457.33       0.0000&lt;br /&gt;
&amp;lt;/pre&amp;gt;&lt;br /&gt;
There are no vibrational modes with negative frequencies&lt;br /&gt;
&lt;br /&gt;
===Calculation of the energy of the Haber-Bosch process===&lt;br /&gt;
N&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; + 3H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; -&amp;gt; 2NH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;&lt;br /&gt;
&lt;br /&gt;
E(NH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;)= -56.557768 a u&lt;br /&gt;
&lt;br /&gt;
2*E(NH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;)= -113.115536 a u&lt;br /&gt;
&lt;br /&gt;
E(N&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;)= -109.5251268 a u&lt;br /&gt;
&lt;br /&gt;
E(H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;)= -1.1785393 a u&lt;br /&gt;
&lt;br /&gt;
3*E(H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;)= -3.5359617 a u&lt;br /&gt;
&lt;br /&gt;
ΔE=2*E(NH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;) - [E(N&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;) + 3*E(H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;)] = -145.57 kj/mol&lt;br /&gt;
&lt;br /&gt;
As the reaction is exothermic, the ammonia product is more stable than the gaseous reactants.&lt;br /&gt;
==Analysis of Cl&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;==&lt;br /&gt;
===General Analysis===&lt;br /&gt;
Calculation method:RB3LYP&lt;br /&gt;
&lt;br /&gt;
Basis Set = 6-31G(d,p)&lt;br /&gt;
&lt;br /&gt;
Final Energy: E(RB3LYP) = -920.3498788 a.u.&lt;br /&gt;
&lt;br /&gt;
Bond length: 2.0417 Å&lt;br /&gt;
===Vibrational Analysis===&lt;br /&gt;
&amp;lt;pre&amp;gt;&lt;br /&gt;
 Item               Value     Threshold  Converged?&lt;br /&gt;
 Maximum Force            0.000043     0.000450     YES&lt;br /&gt;
 RMS     Force            0.000043     0.000300     YES&lt;br /&gt;
 Maximum Displacement     0.000121     0.001800     YES&lt;br /&gt;
 RMS     Displacement     0.000172     0.001200     YES&lt;br /&gt;
&lt;br /&gt;
&amp;lt;/pre&amp;gt;&lt;br /&gt;
&amp;lt;pre&amp;gt;&lt;br /&gt;
Vibrational mode    Frequency    Infrared&lt;br /&gt;
#1             520.32       0.0000&lt;br /&gt;
&amp;lt;/pre&amp;gt;&lt;br /&gt;
There are no vibrational modes with negative frequencies&lt;br /&gt;
===Charge Analysis===&lt;br /&gt;
[[File:Adrian_Popescu_Cl2_Charges2.png|400px|center]]&lt;br /&gt;
As the Cl&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; molecule is made up of identical Cl atoms, the bond between them will be 100% covalent, the electrons that form the sigma bond are equally shared between the cl atoms, so the charge on each Cl atom is zero.&lt;br /&gt;
&lt;br /&gt;
===Molecular orbitals Analysis===&lt;br /&gt;
[[File:orbital1_.png|400px|thumb|center|2σg bonding orbital]]&lt;br /&gt;
The 2σg bonding orbital is deep in energy, occupied, and corresponds to the bonding orbital formed by the 2s AOs of the Cl atoms.&lt;br /&gt;
[[File:Adrian_Popescu_orbital2.png|400px|thumb|center|2σu* antibonding orbital]]&lt;br /&gt;
The 2σu* orbital is higher in energy than the 2σg orbital, is occupied, and corresponds to the antibonding orbital formed by the 2s AOs of the Cl atoms.&lt;br /&gt;
[[File:Adrian_Popescu_orbital3.png|400px|thumb|center|3σg bonding orbital]]&lt;br /&gt;
The 3σg orbital is deep in energy, occupied, and corresponds to the bonding orbital formed by the 3px AOs of the Cl atoms.&lt;br /&gt;
[[File:Adrian_Popescu_homo.png|400px|thumb|center|1πg* antibonding orbital]]&lt;br /&gt;
The 1πg* orbital is high in energy, and is the HOMO (Highest Occupied Molecular Orbital). It corresponds to the antibonding orbital formed by the 3py (or 3pz, as the orbitals are degenerate) AOs of the Cl atoms.&lt;br /&gt;
[[File:Adrian_Popescu_lumo.png|400px|thumb|center|3σu* antibonding orbital]]&lt;br /&gt;
The 3σu* orbital is high in energy, and is the LUMO (Lowest Unoccupied Molecular Orbital). It corresponds to the antibonding orbital formed by the 3px AOs of the Cl atoms.&lt;/div&gt;</summary>
		<author><name>Ap5817</name></author>
	</entry>
	<entry>
		<id>https://chemwiki.ch.ic.ac.uk/index.php?title=File:Adrian_Popescu_Vibrations2.png&amp;diff=680337</id>
		<title>File:Adrian Popescu Vibrations2.png</title>
		<link rel="alternate" type="text/html" href="https://chemwiki.ch.ic.ac.uk/index.php?title=File:Adrian_Popescu_Vibrations2.png&amp;diff=680337"/>
		<updated>2018-03-08T12:03:50Z</updated>

		<summary type="html">&lt;p&gt;Ap5817: &lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;&lt;/div&gt;</summary>
		<author><name>Ap5817</name></author>
	</entry>
	<entry>
		<id>https://chemwiki.ch.ic.ac.uk/index.php?title=File:Adrian_Popescu_lumo.png&amp;diff=679470</id>
		<title>File:Adrian Popescu lumo.png</title>
		<link rel="alternate" type="text/html" href="https://chemwiki.ch.ic.ac.uk/index.php?title=File:Adrian_Popescu_lumo.png&amp;diff=679470"/>
		<updated>2018-03-07T20:38:08Z</updated>

		<summary type="html">&lt;p&gt;Ap5817: &lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;&lt;/div&gt;</summary>
		<author><name>Ap5817</name></author>
	</entry>
	<entry>
		<id>https://chemwiki.ch.ic.ac.uk/index.php?title=User:Ap5817&amp;diff=679469</id>
		<title>User:Ap5817</title>
		<link rel="alternate" type="text/html" href="https://chemwiki.ch.ic.ac.uk/index.php?title=User:Ap5817&amp;diff=679469"/>
		<updated>2018-03-07T20:37:13Z</updated>

		<summary type="html">&lt;p&gt;Ap5817: /* Molecular orbitals Analysis */&lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;== NH3 molecule ==&lt;br /&gt;
=== NH3 calculations ===&lt;br /&gt;
Calculation method:RB3LYP&lt;br /&gt;
&lt;br /&gt;
Basis Set = 6-31G(d,p)&lt;br /&gt;
&lt;br /&gt;
Final Energy: E(RB3LYP) = -56.557768 a.u.&lt;br /&gt;
&lt;br /&gt;
Bond length:1.01789 Å&lt;br /&gt;
&lt;br /&gt;
Bond angle: 105.741 °C&lt;br /&gt;
&lt;br /&gt;
Point Group: C3v&amp;lt;pre&amp;gt;&lt;br /&gt;
Item               Value     Threshold  Converged?&lt;br /&gt;
 Maximum Force            0.000004     0.000450     YES&lt;br /&gt;
 RMS     Force            0.000004     0.000300     YES&lt;br /&gt;
 Maximum Displacement     0.000072     0.001800     YES&lt;br /&gt;
 RMS     Displacement     0.000035     0.001200     YES&lt;br /&gt;
&amp;lt;/pre&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&amp;lt;jmol&amp;gt;&amp;lt;jmolApplet&amp;gt;&lt;br /&gt;
&amp;lt;script&amp;gt;frame x.y&amp;lt;/script&amp;gt;&lt;br /&gt;
  &amp;lt;title&amp;gt;test molecule&amp;lt;/title&amp;gt;&lt;br /&gt;
  &amp;lt;color&amp;gt;black&amp;lt;/color&amp;gt;&lt;br /&gt;
  &amp;lt;size&amp;gt;200&amp;lt;/size&amp;gt;&lt;br /&gt;
  &amp;lt;uploadedFileContents&amp;gt;ADRIAN_POPESCU_PHUNT_NH3_OPTF_POP.LOG&amp;lt;/uploadedFileContents&amp;gt;&lt;br /&gt;
&amp;lt;/jmolApplet&amp;gt;&amp;lt;/jmol&amp;gt;&lt;br /&gt;
&lt;br /&gt;
[[Media:ADRIAN_POPESCU_PHUNT_NH3_OPTF_POP.LOG]]&lt;br /&gt;
&lt;br /&gt;
==Vibration analysis of NH3==&lt;br /&gt;
[[File:Adrian_Popescu_Display_Vibrations.png|1000px]]&lt;br /&gt;
===Vibrational modes===&lt;br /&gt;
Number of vibrational modes: 6&lt;br /&gt;
&lt;br /&gt;
Number of degenerate modes: 4 (2 pairs of degenerate vibrational modes &lt;br /&gt;
&lt;br /&gt;
Number of bending motions: 3&lt;br /&gt;
&lt;br /&gt;
Number of stretching motions: 3&lt;br /&gt;
&lt;br /&gt;
The most symmetric vibrational mode: mode #4&lt;br /&gt;
&lt;br /&gt;
The &#039;&#039;umbrella mode&#039;&#039;: mode #1&lt;br /&gt;
&lt;br /&gt;
Number of bands expected to be seen in an experimental spectrum of gaseous ammonia: 5&lt;br /&gt;
===Charge Analysis===&lt;br /&gt;
[[File:Adrian_Popescu_Charges2.png|400px|center]]&lt;br /&gt;
&lt;br /&gt;
Charge on the N atom: -1.125&lt;br /&gt;
&lt;br /&gt;
Charge on the H atom: 0.375&lt;br /&gt;
&lt;br /&gt;
As Nitrogen has an electronegativity value of 3.04, which is significantly larger than the one of Hidrogen (2.2), it is expected that on the Nitrogen there will be a negative charge and on Hidrogen a possitive charge.&lt;br /&gt;
&lt;br /&gt;
==Reactivity of the Haber-Bosch process==&lt;br /&gt;
===Analysis of H2===&lt;br /&gt;
Calculation method:RB3LYP&lt;br /&gt;
&lt;br /&gt;
Basis Set = 6-31G(d,p)&lt;br /&gt;
&lt;br /&gt;
Final Energy: E(RB3LYP) = -1.1785393 a.u.&lt;br /&gt;
&lt;br /&gt;
Bond length:0.7428 Å&lt;br /&gt;
&amp;lt;pre&amp;gt;&lt;br /&gt;
Item               Value     Threshold  Converged?&lt;br /&gt;
 Maximum Force            0.000004     0.000450     YES&lt;br /&gt;
 RMS     Force            0.000004     0.000300     YES&lt;br /&gt;
 Maximum Displacement     0.000005     0.001800     YES&lt;br /&gt;
 RMS     Displacement     0.000007     0.001200     YES&amp;lt;/pre&amp;gt;&lt;br /&gt;
&amp;lt;pre&amp;gt;&lt;br /&gt;
Vibrational mode    Frequency    Infrared&lt;br /&gt;
#1             4465.6       0.0000&lt;br /&gt;
&amp;lt;/pre&amp;gt;&lt;br /&gt;
There are no vibrational modes with negative frequencies&lt;br /&gt;
===Analysis of N2===&lt;br /&gt;
Calculation method:RB3LYP&lt;br /&gt;
&lt;br /&gt;
Basis Set = 6-31G(d,p)&lt;br /&gt;
&lt;br /&gt;
Final Energy: E(RB3LYP) = -109.5241268 a.u.&lt;br /&gt;
&lt;br /&gt;
Bond length: 1.1055 Å&lt;br /&gt;
&amp;lt;pre&amp;gt;&lt;br /&gt;
Item               Value     Threshold  Converged?&lt;br /&gt;
 Maximum Force            0.000001     0.000450     YES&lt;br /&gt;
 RMS     Force            0.000001     0.000300     YES&lt;br /&gt;
 Maximum Displacement     0.000000     0.001800     YES&lt;br /&gt;
 RMS     Displacement     0.000000     0.001200     YES&lt;br /&gt;
&amp;lt;/pre&amp;gt;&lt;br /&gt;
&amp;lt;pre&amp;gt;&lt;br /&gt;
Vibrational mode    Frequency    Infrared&lt;br /&gt;
#1             2457.33       0.0000&lt;br /&gt;
&amp;lt;/pre&amp;gt;&lt;br /&gt;
There are no vibrational modes with negative frequencies&lt;br /&gt;
&lt;br /&gt;
===Calculation of the energy of the Haber-Bosch process===&lt;br /&gt;
N&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; + 3H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; -&amp;gt; 2NH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;&lt;br /&gt;
&lt;br /&gt;
E(NH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;)= -56.557768 a u&lt;br /&gt;
&lt;br /&gt;
2*E(NH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;)= -113.115536 a u&lt;br /&gt;
&lt;br /&gt;
E(N&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;)= -109.5251268 a u&lt;br /&gt;
&lt;br /&gt;
E(H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;)= -1.1785393 a u&lt;br /&gt;
&lt;br /&gt;
3*E(H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;)= -3.5359617 a u&lt;br /&gt;
&lt;br /&gt;
ΔE=2*E(NH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;) - [E(N&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;) + 3*E(H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;)] = -145.57 kj/mol&lt;br /&gt;
&lt;br /&gt;
As the reaction is exothermic, the ammonia product is more stable than the gaseous reactants.&lt;br /&gt;
==Analysis of Cl&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;==&lt;br /&gt;
===General Analysis===&lt;br /&gt;
Calculation method:RB3LYP&lt;br /&gt;
&lt;br /&gt;
Basis Set = 6-31G(d,p)&lt;br /&gt;
&lt;br /&gt;
Final Energy: E(RB3LYP) = -920.3498788 a.u.&lt;br /&gt;
&lt;br /&gt;
Bond length: 2.0417 Å&lt;br /&gt;
===Vibrational Analysis===&lt;br /&gt;
&amp;lt;pre&amp;gt;&lt;br /&gt;
 Item               Value     Threshold  Converged?&lt;br /&gt;
 Maximum Force            0.000043     0.000450     YES&lt;br /&gt;
 RMS     Force            0.000043     0.000300     YES&lt;br /&gt;
 Maximum Displacement     0.000121     0.001800     YES&lt;br /&gt;
 RMS     Displacement     0.000172     0.001200     YES&lt;br /&gt;
&lt;br /&gt;
&amp;lt;/pre&amp;gt;&lt;br /&gt;
&amp;lt;pre&amp;gt;&lt;br /&gt;
Vibrational mode    Frequency    Infrared&lt;br /&gt;
#1             520.32       0.0000&lt;br /&gt;
&amp;lt;/pre&amp;gt;&lt;br /&gt;
There are no vibrational modes with negative frequencies&lt;br /&gt;
===Charge Analysis===&lt;br /&gt;
[[File:Adrian_Popescu_Cl2_Charges2.png|400px|center]]&lt;br /&gt;
As the Cl&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; molecule is made up of identical Cl atoms, the bond between them will be 100% covalent, the electrons that form the sigma bond are equally shared between the cl atoms, so the charge on each Cl atom is zero.&lt;br /&gt;
&lt;br /&gt;
===Molecular orbitals Analysis===&lt;br /&gt;
[[File:orbital1_.png|400px|thumb|center|2σg bonding orbital]]&lt;br /&gt;
The 2σg bonding orbital is deep in energy, occupied, and corresponds to the bonding orbital formed by the 2s AOs of the Cl atoms.&lt;br /&gt;
[[File:Adrian_Popescu_orbital2.png|400px|thumb|center|2σu* antibonding orbital]]&lt;br /&gt;
The 2σu* orbital is higher in energy than the 2σg orbital, is occupied, and corresponds to the antibonding orbital formed by the 2s AOs of the Cl atoms.&lt;br /&gt;
[[File:Adrian_Popescu_orbital3.png|400px|thumb|center|3σg bonding orbital]]&lt;br /&gt;
The 3σg orbital is deep in energy, occupied, and corresponds to the bonding orbital formed by the 3px AOs of the Cl atoms.&lt;br /&gt;
[[File:Adrian_Popescu_homo.png|400px|thumb|center|1πg* antibonding orbital]]&lt;br /&gt;
The 1πg* orbital is high in energy, and is the HOMO (Highest Occupied Molecular Orbital). It corresponds to the antibonding orbital formed by the 3py (or 3pz, as the orbitals are degenerate) AOs of the Cl atoms.&lt;br /&gt;
[[File:Adrian_Popescu_lumo.png|400px|thumb|center|3σu* antibonding orbital]]&lt;br /&gt;
The 3σu* orbital is high in energy, and is the LUMO (Lowest Unoccupied Molecular Orbital). It corresponds to the antibonding orbital formed by the 3px AOs of the Cl atoms.&lt;/div&gt;</summary>
		<author><name>Ap5817</name></author>
	</entry>
	<entry>
		<id>https://chemwiki.ch.ic.ac.uk/index.php?title=File:Adrian_Popescu_homo.png&amp;diff=679467</id>
		<title>File:Adrian Popescu homo.png</title>
		<link rel="alternate" type="text/html" href="https://chemwiki.ch.ic.ac.uk/index.php?title=File:Adrian_Popescu_homo.png&amp;diff=679467"/>
		<updated>2018-03-07T20:30:34Z</updated>

		<summary type="html">&lt;p&gt;Ap5817: &lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;&lt;/div&gt;</summary>
		<author><name>Ap5817</name></author>
	</entry>
	<entry>
		<id>https://chemwiki.ch.ic.ac.uk/index.php?title=User:Ap5817&amp;diff=679465</id>
		<title>User:Ap5817</title>
		<link rel="alternate" type="text/html" href="https://chemwiki.ch.ic.ac.uk/index.php?title=User:Ap5817&amp;diff=679465"/>
		<updated>2018-03-07T20:27:53Z</updated>

		<summary type="html">&lt;p&gt;Ap5817: /* Molecular orbitals Analysis */&lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;== NH3 molecule ==&lt;br /&gt;
=== NH3 calculations ===&lt;br /&gt;
Calculation method:RB3LYP&lt;br /&gt;
&lt;br /&gt;
Basis Set = 6-31G(d,p)&lt;br /&gt;
&lt;br /&gt;
Final Energy: E(RB3LYP) = -56.557768 a.u.&lt;br /&gt;
&lt;br /&gt;
Bond length:1.01789 Å&lt;br /&gt;
&lt;br /&gt;
Bond angle: 105.741 °C&lt;br /&gt;
&lt;br /&gt;
Point Group: C3v&amp;lt;pre&amp;gt;&lt;br /&gt;
Item               Value     Threshold  Converged?&lt;br /&gt;
 Maximum Force            0.000004     0.000450     YES&lt;br /&gt;
 RMS     Force            0.000004     0.000300     YES&lt;br /&gt;
 Maximum Displacement     0.000072     0.001800     YES&lt;br /&gt;
 RMS     Displacement     0.000035     0.001200     YES&lt;br /&gt;
&amp;lt;/pre&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&amp;lt;jmol&amp;gt;&amp;lt;jmolApplet&amp;gt;&lt;br /&gt;
&amp;lt;script&amp;gt;frame x.y&amp;lt;/script&amp;gt;&lt;br /&gt;
  &amp;lt;title&amp;gt;test molecule&amp;lt;/title&amp;gt;&lt;br /&gt;
  &amp;lt;color&amp;gt;black&amp;lt;/color&amp;gt;&lt;br /&gt;
  &amp;lt;size&amp;gt;200&amp;lt;/size&amp;gt;&lt;br /&gt;
  &amp;lt;uploadedFileContents&amp;gt;ADRIAN_POPESCU_PHUNT_NH3_OPTF_POP.LOG&amp;lt;/uploadedFileContents&amp;gt;&lt;br /&gt;
&amp;lt;/jmolApplet&amp;gt;&amp;lt;/jmol&amp;gt;&lt;br /&gt;
&lt;br /&gt;
[[Media:ADRIAN_POPESCU_PHUNT_NH3_OPTF_POP.LOG]]&lt;br /&gt;
&lt;br /&gt;
==Vibration analysis of NH3==&lt;br /&gt;
[[File:Adrian_Popescu_Display_Vibrations.png|1000px]]&lt;br /&gt;
===Vibrational modes===&lt;br /&gt;
Number of vibrational modes: 6&lt;br /&gt;
&lt;br /&gt;
Number of degenerate modes: 4 (2 pairs of degenerate vibrational modes &lt;br /&gt;
&lt;br /&gt;
Number of bending motions: 3&lt;br /&gt;
&lt;br /&gt;
Number of stretching motions: 3&lt;br /&gt;
&lt;br /&gt;
The most symmetric vibrational mode: mode #4&lt;br /&gt;
&lt;br /&gt;
The &#039;&#039;umbrella mode&#039;&#039;: mode #1&lt;br /&gt;
&lt;br /&gt;
Number of bands expected to be seen in an experimental spectrum of gaseous ammonia: 5&lt;br /&gt;
===Charge Analysis===&lt;br /&gt;
[[File:Adrian_Popescu_Charges2.png|400px|center]]&lt;br /&gt;
&lt;br /&gt;
Charge on the N atom: -1.125&lt;br /&gt;
&lt;br /&gt;
Charge on the H atom: 0.375&lt;br /&gt;
&lt;br /&gt;
As Nitrogen has an electronegativity value of 3.04, which is significantly larger than the one of Hidrogen (2.2), it is expected that on the Nitrogen there will be a negative charge and on Hidrogen a possitive charge.&lt;br /&gt;
&lt;br /&gt;
==Reactivity of the Haber-Bosch process==&lt;br /&gt;
===Analysis of H2===&lt;br /&gt;
Calculation method:RB3LYP&lt;br /&gt;
&lt;br /&gt;
Basis Set = 6-31G(d,p)&lt;br /&gt;
&lt;br /&gt;
Final Energy: E(RB3LYP) = -1.1785393 a.u.&lt;br /&gt;
&lt;br /&gt;
Bond length:0.7428 Å&lt;br /&gt;
&amp;lt;pre&amp;gt;&lt;br /&gt;
Item               Value     Threshold  Converged?&lt;br /&gt;
 Maximum Force            0.000004     0.000450     YES&lt;br /&gt;
 RMS     Force            0.000004     0.000300     YES&lt;br /&gt;
 Maximum Displacement     0.000005     0.001800     YES&lt;br /&gt;
 RMS     Displacement     0.000007     0.001200     YES&amp;lt;/pre&amp;gt;&lt;br /&gt;
&amp;lt;pre&amp;gt;&lt;br /&gt;
Vibrational mode    Frequency    Infrared&lt;br /&gt;
#1             4465.6       0.0000&lt;br /&gt;
&amp;lt;/pre&amp;gt;&lt;br /&gt;
There are no vibrational modes with negative frequencies&lt;br /&gt;
===Analysis of N2===&lt;br /&gt;
Calculation method:RB3LYP&lt;br /&gt;
&lt;br /&gt;
Basis Set = 6-31G(d,p)&lt;br /&gt;
&lt;br /&gt;
Final Energy: E(RB3LYP) = -109.5241268 a.u.&lt;br /&gt;
&lt;br /&gt;
Bond length: 1.1055 Å&lt;br /&gt;
&amp;lt;pre&amp;gt;&lt;br /&gt;
Item               Value     Threshold  Converged?&lt;br /&gt;
 Maximum Force            0.000001     0.000450     YES&lt;br /&gt;
 RMS     Force            0.000001     0.000300     YES&lt;br /&gt;
 Maximum Displacement     0.000000     0.001800     YES&lt;br /&gt;
 RMS     Displacement     0.000000     0.001200     YES&lt;br /&gt;
&amp;lt;/pre&amp;gt;&lt;br /&gt;
&amp;lt;pre&amp;gt;&lt;br /&gt;
Vibrational mode    Frequency    Infrared&lt;br /&gt;
#1             2457.33       0.0000&lt;br /&gt;
&amp;lt;/pre&amp;gt;&lt;br /&gt;
There are no vibrational modes with negative frequencies&lt;br /&gt;
&lt;br /&gt;
===Calculation of the energy of the Haber-Bosch process===&lt;br /&gt;
N&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; + 3H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; -&amp;gt; 2NH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;&lt;br /&gt;
&lt;br /&gt;
E(NH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;)= -56.557768 a u&lt;br /&gt;
&lt;br /&gt;
2*E(NH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;)= -113.115536 a u&lt;br /&gt;
&lt;br /&gt;
E(N&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;)= -109.5251268 a u&lt;br /&gt;
&lt;br /&gt;
E(H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;)= -1.1785393 a u&lt;br /&gt;
&lt;br /&gt;
3*E(H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;)= -3.5359617 a u&lt;br /&gt;
&lt;br /&gt;
ΔE=2*E(NH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;) - [E(N&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;) + 3*E(H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;)] = -145.57 kj/mol&lt;br /&gt;
&lt;br /&gt;
As the reaction is exothermic, the ammonia product is more stable than the gaseous reactants.&lt;br /&gt;
==Analysis of Cl&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;==&lt;br /&gt;
===General Analysis===&lt;br /&gt;
Calculation method:RB3LYP&lt;br /&gt;
&lt;br /&gt;
Basis Set = 6-31G(d,p)&lt;br /&gt;
&lt;br /&gt;
Final Energy: E(RB3LYP) = -920.3498788 a.u.&lt;br /&gt;
&lt;br /&gt;
Bond length: 2.0417 Å&lt;br /&gt;
===Vibrational Analysis===&lt;br /&gt;
&amp;lt;pre&amp;gt;&lt;br /&gt;
 Item               Value     Threshold  Converged?&lt;br /&gt;
 Maximum Force            0.000043     0.000450     YES&lt;br /&gt;
 RMS     Force            0.000043     0.000300     YES&lt;br /&gt;
 Maximum Displacement     0.000121     0.001800     YES&lt;br /&gt;
 RMS     Displacement     0.000172     0.001200     YES&lt;br /&gt;
&lt;br /&gt;
&amp;lt;/pre&amp;gt;&lt;br /&gt;
&amp;lt;pre&amp;gt;&lt;br /&gt;
Vibrational mode    Frequency    Infrared&lt;br /&gt;
#1             520.32       0.0000&lt;br /&gt;
&amp;lt;/pre&amp;gt;&lt;br /&gt;
There are no vibrational modes with negative frequencies&lt;br /&gt;
===Charge Analysis===&lt;br /&gt;
[[File:Adrian_Popescu_Cl2_Charges2.png|400px|center]]&lt;br /&gt;
As the Cl&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; molecule is made up of identical Cl atoms, the bond between them will be 100% covalent, the electrons that form the sigma bond are equally shared between the cl atoms, so the charge on each Cl atom is zero.&lt;br /&gt;
&lt;br /&gt;
===Molecular orbitals Analysis===&lt;br /&gt;
[[File:orbital1_.png|400px|thumb|center|2σg bonding orbital]]&lt;br /&gt;
The 2σg bonding orbital is deep in energy, occupied, and corresponds to the bonding orbital formed by the 2s AOs of the Cl atoms.&lt;br /&gt;
[[File:Adrian_Popescu_orbital2.png|400px|thumb|center|2σu* antibonding orbital]]&lt;br /&gt;
The 2σu* orbital is higher in energy than the 2σg orbital, is occupied, and corresponds to the antibonding orbital formed by the 2s AOs of the Cl atoms.&lt;br /&gt;
[[File:Adrian_Popescu_orbital3.png|400px|thumb|center|3σg bonding orbital]]&lt;br /&gt;
The 3σg orbital is deep in energy, occupied, and corresponds to the bonding orbital formed by the 3px AOs of the Cl atoms.&lt;/div&gt;</summary>
		<author><name>Ap5817</name></author>
	</entry>
	<entry>
		<id>https://chemwiki.ch.ic.ac.uk/index.php?title=File:Adrian_Popescu_orbital3.png&amp;diff=679456</id>
		<title>File:Adrian Popescu orbital3.png</title>
		<link rel="alternate" type="text/html" href="https://chemwiki.ch.ic.ac.uk/index.php?title=File:Adrian_Popescu_orbital3.png&amp;diff=679456"/>
		<updated>2018-03-07T20:21:34Z</updated>

		<summary type="html">&lt;p&gt;Ap5817: &lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;&lt;/div&gt;</summary>
		<author><name>Ap5817</name></author>
	</entry>
	<entry>
		<id>https://chemwiki.ch.ic.ac.uk/index.php?title=User:Ap5817&amp;diff=679455</id>
		<title>User:Ap5817</title>
		<link rel="alternate" type="text/html" href="https://chemwiki.ch.ic.ac.uk/index.php?title=User:Ap5817&amp;diff=679455"/>
		<updated>2018-03-07T20:19:32Z</updated>

		<summary type="html">&lt;p&gt;Ap5817: /* Molecular orbitals Analysis */&lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;== NH3 molecule ==&lt;br /&gt;
=== NH3 calculations ===&lt;br /&gt;
Calculation method:RB3LYP&lt;br /&gt;
&lt;br /&gt;
Basis Set = 6-31G(d,p)&lt;br /&gt;
&lt;br /&gt;
Final Energy: E(RB3LYP) = -56.557768 a.u.&lt;br /&gt;
&lt;br /&gt;
Bond length:1.01789 Å&lt;br /&gt;
&lt;br /&gt;
Bond angle: 105.741 °C&lt;br /&gt;
&lt;br /&gt;
Point Group: C3v&amp;lt;pre&amp;gt;&lt;br /&gt;
Item               Value     Threshold  Converged?&lt;br /&gt;
 Maximum Force            0.000004     0.000450     YES&lt;br /&gt;
 RMS     Force            0.000004     0.000300     YES&lt;br /&gt;
 Maximum Displacement     0.000072     0.001800     YES&lt;br /&gt;
 RMS     Displacement     0.000035     0.001200     YES&lt;br /&gt;
&amp;lt;/pre&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&amp;lt;jmol&amp;gt;&amp;lt;jmolApplet&amp;gt;&lt;br /&gt;
&amp;lt;script&amp;gt;frame x.y&amp;lt;/script&amp;gt;&lt;br /&gt;
  &amp;lt;title&amp;gt;test molecule&amp;lt;/title&amp;gt;&lt;br /&gt;
  &amp;lt;color&amp;gt;black&amp;lt;/color&amp;gt;&lt;br /&gt;
  &amp;lt;size&amp;gt;200&amp;lt;/size&amp;gt;&lt;br /&gt;
  &amp;lt;uploadedFileContents&amp;gt;ADRIAN_POPESCU_PHUNT_NH3_OPTF_POP.LOG&amp;lt;/uploadedFileContents&amp;gt;&lt;br /&gt;
&amp;lt;/jmolApplet&amp;gt;&amp;lt;/jmol&amp;gt;&lt;br /&gt;
&lt;br /&gt;
[[Media:ADRIAN_POPESCU_PHUNT_NH3_OPTF_POP.LOG]]&lt;br /&gt;
&lt;br /&gt;
==Vibration analysis of NH3==&lt;br /&gt;
[[File:Adrian_Popescu_Display_Vibrations.png|1000px]]&lt;br /&gt;
===Vibrational modes===&lt;br /&gt;
Number of vibrational modes: 6&lt;br /&gt;
&lt;br /&gt;
Number of degenerate modes: 4 (2 pairs of degenerate vibrational modes &lt;br /&gt;
&lt;br /&gt;
Number of bending motions: 3&lt;br /&gt;
&lt;br /&gt;
Number of stretching motions: 3&lt;br /&gt;
&lt;br /&gt;
The most symmetric vibrational mode: mode #4&lt;br /&gt;
&lt;br /&gt;
The &#039;&#039;umbrella mode&#039;&#039;: mode #1&lt;br /&gt;
&lt;br /&gt;
Number of bands expected to be seen in an experimental spectrum of gaseous ammonia: 5&lt;br /&gt;
===Charge Analysis===&lt;br /&gt;
[[File:Adrian_Popescu_Charges2.png|400px|center]]&lt;br /&gt;
&lt;br /&gt;
Charge on the N atom: -1.125&lt;br /&gt;
&lt;br /&gt;
Charge on the H atom: 0.375&lt;br /&gt;
&lt;br /&gt;
As Nitrogen has an electronegativity value of 3.04, which is significantly larger than the one of Hidrogen (2.2), it is expected that on the Nitrogen there will be a negative charge and on Hidrogen a possitive charge.&lt;br /&gt;
&lt;br /&gt;
==Reactivity of the Haber-Bosch process==&lt;br /&gt;
===Analysis of H2===&lt;br /&gt;
Calculation method:RB3LYP&lt;br /&gt;
&lt;br /&gt;
Basis Set = 6-31G(d,p)&lt;br /&gt;
&lt;br /&gt;
Final Energy: E(RB3LYP) = -1.1785393 a.u.&lt;br /&gt;
&lt;br /&gt;
Bond length:0.7428 Å&lt;br /&gt;
&amp;lt;pre&amp;gt;&lt;br /&gt;
Item               Value     Threshold  Converged?&lt;br /&gt;
 Maximum Force            0.000004     0.000450     YES&lt;br /&gt;
 RMS     Force            0.000004     0.000300     YES&lt;br /&gt;
 Maximum Displacement     0.000005     0.001800     YES&lt;br /&gt;
 RMS     Displacement     0.000007     0.001200     YES&amp;lt;/pre&amp;gt;&lt;br /&gt;
&amp;lt;pre&amp;gt;&lt;br /&gt;
Vibrational mode    Frequency    Infrared&lt;br /&gt;
#1             4465.6       0.0000&lt;br /&gt;
&amp;lt;/pre&amp;gt;&lt;br /&gt;
There are no vibrational modes with negative frequencies&lt;br /&gt;
===Analysis of N2===&lt;br /&gt;
Calculation method:RB3LYP&lt;br /&gt;
&lt;br /&gt;
Basis Set = 6-31G(d,p)&lt;br /&gt;
&lt;br /&gt;
Final Energy: E(RB3LYP) = -109.5241268 a.u.&lt;br /&gt;
&lt;br /&gt;
Bond length: 1.1055 Å&lt;br /&gt;
&amp;lt;pre&amp;gt;&lt;br /&gt;
Item               Value     Threshold  Converged?&lt;br /&gt;
 Maximum Force            0.000001     0.000450     YES&lt;br /&gt;
 RMS     Force            0.000001     0.000300     YES&lt;br /&gt;
 Maximum Displacement     0.000000     0.001800     YES&lt;br /&gt;
 RMS     Displacement     0.000000     0.001200     YES&lt;br /&gt;
&amp;lt;/pre&amp;gt;&lt;br /&gt;
&amp;lt;pre&amp;gt;&lt;br /&gt;
Vibrational mode    Frequency    Infrared&lt;br /&gt;
#1             2457.33       0.0000&lt;br /&gt;
&amp;lt;/pre&amp;gt;&lt;br /&gt;
There are no vibrational modes with negative frequencies&lt;br /&gt;
&lt;br /&gt;
===Calculation of the energy of the Haber-Bosch process===&lt;br /&gt;
N&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; + 3H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; -&amp;gt; 2NH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;&lt;br /&gt;
&lt;br /&gt;
E(NH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;)= -56.557768 a u&lt;br /&gt;
&lt;br /&gt;
2*E(NH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;)= -113.115536 a u&lt;br /&gt;
&lt;br /&gt;
E(N&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;)= -109.5251268 a u&lt;br /&gt;
&lt;br /&gt;
E(H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;)= -1.1785393 a u&lt;br /&gt;
&lt;br /&gt;
3*E(H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;)= -3.5359617 a u&lt;br /&gt;
&lt;br /&gt;
ΔE=2*E(NH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;) - [E(N&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;) + 3*E(H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;)] = -145.57 kj/mol&lt;br /&gt;
&lt;br /&gt;
As the reaction is exothermic, the ammonia product is more stable than the gaseous reactants.&lt;br /&gt;
==Analysis of Cl&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;==&lt;br /&gt;
===General Analysis===&lt;br /&gt;
Calculation method:RB3LYP&lt;br /&gt;
&lt;br /&gt;
Basis Set = 6-31G(d,p)&lt;br /&gt;
&lt;br /&gt;
Final Energy: E(RB3LYP) = -920.3498788 a.u.&lt;br /&gt;
&lt;br /&gt;
Bond length: 2.0417 Å&lt;br /&gt;
===Vibrational Analysis===&lt;br /&gt;
&amp;lt;pre&amp;gt;&lt;br /&gt;
 Item               Value     Threshold  Converged?&lt;br /&gt;
 Maximum Force            0.000043     0.000450     YES&lt;br /&gt;
 RMS     Force            0.000043     0.000300     YES&lt;br /&gt;
 Maximum Displacement     0.000121     0.001800     YES&lt;br /&gt;
 RMS     Displacement     0.000172     0.001200     YES&lt;br /&gt;
&lt;br /&gt;
&amp;lt;/pre&amp;gt;&lt;br /&gt;
&amp;lt;pre&amp;gt;&lt;br /&gt;
Vibrational mode    Frequency    Infrared&lt;br /&gt;
#1             520.32       0.0000&lt;br /&gt;
&amp;lt;/pre&amp;gt;&lt;br /&gt;
There are no vibrational modes with negative frequencies&lt;br /&gt;
===Charge Analysis===&lt;br /&gt;
[[File:Adrian_Popescu_Cl2_Charges2.png|400px|center]]&lt;br /&gt;
As the Cl&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; molecule is made up of identical Cl atoms, the bond between them will be 100% covalent, the electrons that form the sigma bond are equally shared between the cl atoms, so the charge on each Cl atom is zero.&lt;br /&gt;
&lt;br /&gt;
===Molecular orbitals Analysis===&lt;br /&gt;
[[File:orbital1_.png|400px|thumb|center|2σg bonding orbital]]&lt;br /&gt;
The 2σg bonding orbital is deep in energy, occupied, and corresponds to the bonding orbital formed by the 2s AOs of the Cl atoms.&lt;br /&gt;
[[File:Adrian_Popescu_orbital2.png|400px|thumb|center|2σu* antibonding orbital]]&lt;br /&gt;
The 2σu* orbital is higher in energy than the 2σg orbital, is occupied, and corresponds to the antibonding orbital formed by the 2s AOs of the Cl atoms.&lt;/div&gt;</summary>
		<author><name>Ap5817</name></author>
	</entry>
	<entry>
		<id>https://chemwiki.ch.ic.ac.uk/index.php?title=File:Adrian_Popescu_orbital2.png&amp;diff=679453</id>
		<title>File:Adrian Popescu orbital2.png</title>
		<link rel="alternate" type="text/html" href="https://chemwiki.ch.ic.ac.uk/index.php?title=File:Adrian_Popescu_orbital2.png&amp;diff=679453"/>
		<updated>2018-03-07T20:16:21Z</updated>

		<summary type="html">&lt;p&gt;Ap5817: &lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;&lt;/div&gt;</summary>
		<author><name>Ap5817</name></author>
	</entry>
	<entry>
		<id>https://chemwiki.ch.ic.ac.uk/index.php?title=User:Ap5817&amp;diff=679440</id>
		<title>User:Ap5817</title>
		<link rel="alternate" type="text/html" href="https://chemwiki.ch.ic.ac.uk/index.php?title=User:Ap5817&amp;diff=679440"/>
		<updated>2018-03-07T19:53:02Z</updated>

		<summary type="html">&lt;p&gt;Ap5817: /* Molecular orbitals Analysis */&lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;== NH3 molecule ==&lt;br /&gt;
=== NH3 calculations ===&lt;br /&gt;
Calculation method:RB3LYP&lt;br /&gt;
&lt;br /&gt;
Basis Set = 6-31G(d,p)&lt;br /&gt;
&lt;br /&gt;
Final Energy: E(RB3LYP) = -56.557768 a.u.&lt;br /&gt;
&lt;br /&gt;
Bond length:1.01789 Å&lt;br /&gt;
&lt;br /&gt;
Bond angle: 105.741 °C&lt;br /&gt;
&lt;br /&gt;
Point Group: C3v&amp;lt;pre&amp;gt;&lt;br /&gt;
Item               Value     Threshold  Converged?&lt;br /&gt;
 Maximum Force            0.000004     0.000450     YES&lt;br /&gt;
 RMS     Force            0.000004     0.000300     YES&lt;br /&gt;
 Maximum Displacement     0.000072     0.001800     YES&lt;br /&gt;
 RMS     Displacement     0.000035     0.001200     YES&lt;br /&gt;
&amp;lt;/pre&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&amp;lt;jmol&amp;gt;&amp;lt;jmolApplet&amp;gt;&lt;br /&gt;
&amp;lt;script&amp;gt;frame x.y&amp;lt;/script&amp;gt;&lt;br /&gt;
  &amp;lt;title&amp;gt;test molecule&amp;lt;/title&amp;gt;&lt;br /&gt;
  &amp;lt;color&amp;gt;black&amp;lt;/color&amp;gt;&lt;br /&gt;
  &amp;lt;size&amp;gt;200&amp;lt;/size&amp;gt;&lt;br /&gt;
  &amp;lt;uploadedFileContents&amp;gt;ADRIAN_POPESCU_PHUNT_NH3_OPTF_POP.LOG&amp;lt;/uploadedFileContents&amp;gt;&lt;br /&gt;
&amp;lt;/jmolApplet&amp;gt;&amp;lt;/jmol&amp;gt;&lt;br /&gt;
&lt;br /&gt;
[[Media:ADRIAN_POPESCU_PHUNT_NH3_OPTF_POP.LOG]]&lt;br /&gt;
&lt;br /&gt;
==Vibration analysis of NH3==&lt;br /&gt;
[[File:Adrian_Popescu_Display_Vibrations.png|1000px]]&lt;br /&gt;
===Vibrational modes===&lt;br /&gt;
Number of vibrational modes: 6&lt;br /&gt;
&lt;br /&gt;
Number of degenerate modes: 4 (2 pairs of degenerate vibrational modes &lt;br /&gt;
&lt;br /&gt;
Number of bending motions: 3&lt;br /&gt;
&lt;br /&gt;
Number of stretching motions: 3&lt;br /&gt;
&lt;br /&gt;
The most symmetric vibrational mode: mode #4&lt;br /&gt;
&lt;br /&gt;
The &#039;&#039;umbrella mode&#039;&#039;: mode #1&lt;br /&gt;
&lt;br /&gt;
Number of bands expected to be seen in an experimental spectrum of gaseous ammonia: 5&lt;br /&gt;
===Charge Analysis===&lt;br /&gt;
[[File:Adrian_Popescu_Charges2.png|400px|center]]&lt;br /&gt;
&lt;br /&gt;
Charge on the N atom: -1.125&lt;br /&gt;
&lt;br /&gt;
Charge on the H atom: 0.375&lt;br /&gt;
&lt;br /&gt;
As Nitrogen has an electronegativity value of 3.04, which is significantly larger than the one of Hidrogen (2.2), it is expected that on the Nitrogen there will be a negative charge and on Hidrogen a possitive charge.&lt;br /&gt;
&lt;br /&gt;
==Reactivity of the Haber-Bosch process==&lt;br /&gt;
===Analysis of H2===&lt;br /&gt;
Calculation method:RB3LYP&lt;br /&gt;
&lt;br /&gt;
Basis Set = 6-31G(d,p)&lt;br /&gt;
&lt;br /&gt;
Final Energy: E(RB3LYP) = -1.1785393 a.u.&lt;br /&gt;
&lt;br /&gt;
Bond length:0.7428 Å&lt;br /&gt;
&amp;lt;pre&amp;gt;&lt;br /&gt;
Item               Value     Threshold  Converged?&lt;br /&gt;
 Maximum Force            0.000004     0.000450     YES&lt;br /&gt;
 RMS     Force            0.000004     0.000300     YES&lt;br /&gt;
 Maximum Displacement     0.000005     0.001800     YES&lt;br /&gt;
 RMS     Displacement     0.000007     0.001200     YES&amp;lt;/pre&amp;gt;&lt;br /&gt;
&amp;lt;pre&amp;gt;&lt;br /&gt;
Vibrational mode    Frequency    Infrared&lt;br /&gt;
#1             4465.6       0.0000&lt;br /&gt;
&amp;lt;/pre&amp;gt;&lt;br /&gt;
There are no vibrational modes with negative frequencies&lt;br /&gt;
===Analysis of N2===&lt;br /&gt;
Calculation method:RB3LYP&lt;br /&gt;
&lt;br /&gt;
Basis Set = 6-31G(d,p)&lt;br /&gt;
&lt;br /&gt;
Final Energy: E(RB3LYP) = -109.5241268 a.u.&lt;br /&gt;
&lt;br /&gt;
Bond length: 1.1055 Å&lt;br /&gt;
&amp;lt;pre&amp;gt;&lt;br /&gt;
Item               Value     Threshold  Converged?&lt;br /&gt;
 Maximum Force            0.000001     0.000450     YES&lt;br /&gt;
 RMS     Force            0.000001     0.000300     YES&lt;br /&gt;
 Maximum Displacement     0.000000     0.001800     YES&lt;br /&gt;
 RMS     Displacement     0.000000     0.001200     YES&lt;br /&gt;
&amp;lt;/pre&amp;gt;&lt;br /&gt;
&amp;lt;pre&amp;gt;&lt;br /&gt;
Vibrational mode    Frequency    Infrared&lt;br /&gt;
#1             2457.33       0.0000&lt;br /&gt;
&amp;lt;/pre&amp;gt;&lt;br /&gt;
There are no vibrational modes with negative frequencies&lt;br /&gt;
&lt;br /&gt;
===Calculation of the energy of the Haber-Bosch process===&lt;br /&gt;
N&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; + 3H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; -&amp;gt; 2NH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;&lt;br /&gt;
&lt;br /&gt;
E(NH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;)= -56.557768 a u&lt;br /&gt;
&lt;br /&gt;
2*E(NH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;)= -113.115536 a u&lt;br /&gt;
&lt;br /&gt;
E(N&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;)= -109.5251268 a u&lt;br /&gt;
&lt;br /&gt;
E(H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;)= -1.1785393 a u&lt;br /&gt;
&lt;br /&gt;
3*E(H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;)= -3.5359617 a u&lt;br /&gt;
&lt;br /&gt;
ΔE=2*E(NH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;) - [E(N&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;) + 3*E(H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;)] = -145.57 kj/mol&lt;br /&gt;
&lt;br /&gt;
As the reaction is exothermic, the ammonia product is more stable than the gaseous reactants.&lt;br /&gt;
==Analysis of Cl&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;==&lt;br /&gt;
===General Analysis===&lt;br /&gt;
Calculation method:RB3LYP&lt;br /&gt;
&lt;br /&gt;
Basis Set = 6-31G(d,p)&lt;br /&gt;
&lt;br /&gt;
Final Energy: E(RB3LYP) = -920.3498788 a.u.&lt;br /&gt;
&lt;br /&gt;
Bond length: 2.0417 Å&lt;br /&gt;
===Vibrational Analysis===&lt;br /&gt;
&amp;lt;pre&amp;gt;&lt;br /&gt;
 Item               Value     Threshold  Converged?&lt;br /&gt;
 Maximum Force            0.000043     0.000450     YES&lt;br /&gt;
 RMS     Force            0.000043     0.000300     YES&lt;br /&gt;
 Maximum Displacement     0.000121     0.001800     YES&lt;br /&gt;
 RMS     Displacement     0.000172     0.001200     YES&lt;br /&gt;
&lt;br /&gt;
&amp;lt;/pre&amp;gt;&lt;br /&gt;
&amp;lt;pre&amp;gt;&lt;br /&gt;
Vibrational mode    Frequency    Infrared&lt;br /&gt;
#1             520.32       0.0000&lt;br /&gt;
&amp;lt;/pre&amp;gt;&lt;br /&gt;
There are no vibrational modes with negative frequencies&lt;br /&gt;
===Charge Analysis===&lt;br /&gt;
[[File:Adrian_Popescu_Cl2_Charges2.png|400px|center]]&lt;br /&gt;
As the Cl&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; molecule is made up of identical Cl atoms, the bond between them will be 100% covalent, the electrons that form the sigma bond are equally shared between the cl atoms, so the charge on each Cl atom is zero.&lt;br /&gt;
&lt;br /&gt;
===Molecular orbitals Analysis===&lt;br /&gt;
[[File:orbital1_.png|400px|thumb|center|2σg bonding orbital]]&lt;br /&gt;
The 2σg bonding orbital is deep in energy, occupied, and corresponds to the bonding orbital formed by the 2s AOs of the Cl atoms.&lt;/div&gt;</summary>
		<author><name>Ap5817</name></author>
	</entry>
	<entry>
		<id>https://chemwiki.ch.ic.ac.uk/index.php?title=User:Ap5817&amp;diff=679436</id>
		<title>User:Ap5817</title>
		<link rel="alternate" type="text/html" href="https://chemwiki.ch.ic.ac.uk/index.php?title=User:Ap5817&amp;diff=679436"/>
		<updated>2018-03-07T19:50:05Z</updated>

		<summary type="html">&lt;p&gt;Ap5817: /* Molecular orbitals Analysis */&lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;== NH3 molecule ==&lt;br /&gt;
=== NH3 calculations ===&lt;br /&gt;
Calculation method:RB3LYP&lt;br /&gt;
&lt;br /&gt;
Basis Set = 6-31G(d,p)&lt;br /&gt;
&lt;br /&gt;
Final Energy: E(RB3LYP) = -56.557768 a.u.&lt;br /&gt;
&lt;br /&gt;
Bond length:1.01789 Å&lt;br /&gt;
&lt;br /&gt;
Bond angle: 105.741 °C&lt;br /&gt;
&lt;br /&gt;
Point Group: C3v&amp;lt;pre&amp;gt;&lt;br /&gt;
Item               Value     Threshold  Converged?&lt;br /&gt;
 Maximum Force            0.000004     0.000450     YES&lt;br /&gt;
 RMS     Force            0.000004     0.000300     YES&lt;br /&gt;
 Maximum Displacement     0.000072     0.001800     YES&lt;br /&gt;
 RMS     Displacement     0.000035     0.001200     YES&lt;br /&gt;
&amp;lt;/pre&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&amp;lt;jmol&amp;gt;&amp;lt;jmolApplet&amp;gt;&lt;br /&gt;
&amp;lt;script&amp;gt;frame x.y&amp;lt;/script&amp;gt;&lt;br /&gt;
  &amp;lt;title&amp;gt;test molecule&amp;lt;/title&amp;gt;&lt;br /&gt;
  &amp;lt;color&amp;gt;black&amp;lt;/color&amp;gt;&lt;br /&gt;
  &amp;lt;size&amp;gt;200&amp;lt;/size&amp;gt;&lt;br /&gt;
  &amp;lt;uploadedFileContents&amp;gt;ADRIAN_POPESCU_PHUNT_NH3_OPTF_POP.LOG&amp;lt;/uploadedFileContents&amp;gt;&lt;br /&gt;
&amp;lt;/jmolApplet&amp;gt;&amp;lt;/jmol&amp;gt;&lt;br /&gt;
&lt;br /&gt;
[[Media:ADRIAN_POPESCU_PHUNT_NH3_OPTF_POP.LOG]]&lt;br /&gt;
&lt;br /&gt;
==Vibration analysis of NH3==&lt;br /&gt;
[[File:Adrian_Popescu_Display_Vibrations.png|1000px]]&lt;br /&gt;
===Vibrational modes===&lt;br /&gt;
Number of vibrational modes: 6&lt;br /&gt;
&lt;br /&gt;
Number of degenerate modes: 4 (2 pairs of degenerate vibrational modes &lt;br /&gt;
&lt;br /&gt;
Number of bending motions: 3&lt;br /&gt;
&lt;br /&gt;
Number of stretching motions: 3&lt;br /&gt;
&lt;br /&gt;
The most symmetric vibrational mode: mode #4&lt;br /&gt;
&lt;br /&gt;
The &#039;&#039;umbrella mode&#039;&#039;: mode #1&lt;br /&gt;
&lt;br /&gt;
Number of bands expected to be seen in an experimental spectrum of gaseous ammonia: 5&lt;br /&gt;
===Charge Analysis===&lt;br /&gt;
[[File:Adrian_Popescu_Charges2.png|400px|center]]&lt;br /&gt;
&lt;br /&gt;
Charge on the N atom: -1.125&lt;br /&gt;
&lt;br /&gt;
Charge on the H atom: 0.375&lt;br /&gt;
&lt;br /&gt;
As Nitrogen has an electronegativity value of 3.04, which is significantly larger than the one of Hidrogen (2.2), it is expected that on the Nitrogen there will be a negative charge and on Hidrogen a possitive charge.&lt;br /&gt;
&lt;br /&gt;
==Reactivity of the Haber-Bosch process==&lt;br /&gt;
===Analysis of H2===&lt;br /&gt;
Calculation method:RB3LYP&lt;br /&gt;
&lt;br /&gt;
Basis Set = 6-31G(d,p)&lt;br /&gt;
&lt;br /&gt;
Final Energy: E(RB3LYP) = -1.1785393 a.u.&lt;br /&gt;
&lt;br /&gt;
Bond length:0.7428 Å&lt;br /&gt;
&amp;lt;pre&amp;gt;&lt;br /&gt;
Item               Value     Threshold  Converged?&lt;br /&gt;
 Maximum Force            0.000004     0.000450     YES&lt;br /&gt;
 RMS     Force            0.000004     0.000300     YES&lt;br /&gt;
 Maximum Displacement     0.000005     0.001800     YES&lt;br /&gt;
 RMS     Displacement     0.000007     0.001200     YES&amp;lt;/pre&amp;gt;&lt;br /&gt;
&amp;lt;pre&amp;gt;&lt;br /&gt;
Vibrational mode    Frequency    Infrared&lt;br /&gt;
#1             4465.6       0.0000&lt;br /&gt;
&amp;lt;/pre&amp;gt;&lt;br /&gt;
There are no vibrational modes with negative frequencies&lt;br /&gt;
===Analysis of N2===&lt;br /&gt;
Calculation method:RB3LYP&lt;br /&gt;
&lt;br /&gt;
Basis Set = 6-31G(d,p)&lt;br /&gt;
&lt;br /&gt;
Final Energy: E(RB3LYP) = -109.5241268 a.u.&lt;br /&gt;
&lt;br /&gt;
Bond length: 1.1055 Å&lt;br /&gt;
&amp;lt;pre&amp;gt;&lt;br /&gt;
Item               Value     Threshold  Converged?&lt;br /&gt;
 Maximum Force            0.000001     0.000450     YES&lt;br /&gt;
 RMS     Force            0.000001     0.000300     YES&lt;br /&gt;
 Maximum Displacement     0.000000     0.001800     YES&lt;br /&gt;
 RMS     Displacement     0.000000     0.001200     YES&lt;br /&gt;
&amp;lt;/pre&amp;gt;&lt;br /&gt;
&amp;lt;pre&amp;gt;&lt;br /&gt;
Vibrational mode    Frequency    Infrared&lt;br /&gt;
#1             2457.33       0.0000&lt;br /&gt;
&amp;lt;/pre&amp;gt;&lt;br /&gt;
There are no vibrational modes with negative frequencies&lt;br /&gt;
&lt;br /&gt;
===Calculation of the energy of the Haber-Bosch process===&lt;br /&gt;
N&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; + 3H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; -&amp;gt; 2NH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;&lt;br /&gt;
&lt;br /&gt;
E(NH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;)= -56.557768 a u&lt;br /&gt;
&lt;br /&gt;
2*E(NH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;)= -113.115536 a u&lt;br /&gt;
&lt;br /&gt;
E(N&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;)= -109.5251268 a u&lt;br /&gt;
&lt;br /&gt;
E(H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;)= -1.1785393 a u&lt;br /&gt;
&lt;br /&gt;
3*E(H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;)= -3.5359617 a u&lt;br /&gt;
&lt;br /&gt;
ΔE=2*E(NH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;) - [E(N&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;) + 3*E(H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;)] = -145.57 kj/mol&lt;br /&gt;
&lt;br /&gt;
As the reaction is exothermic, the ammonia product is more stable than the gaseous reactants.&lt;br /&gt;
==Analysis of Cl&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;==&lt;br /&gt;
===General Analysis===&lt;br /&gt;
Calculation method:RB3LYP&lt;br /&gt;
&lt;br /&gt;
Basis Set = 6-31G(d,p)&lt;br /&gt;
&lt;br /&gt;
Final Energy: E(RB3LYP) = -920.3498788 a.u.&lt;br /&gt;
&lt;br /&gt;
Bond length: 2.0417 Å&lt;br /&gt;
===Vibrational Analysis===&lt;br /&gt;
&amp;lt;pre&amp;gt;&lt;br /&gt;
 Item               Value     Threshold  Converged?&lt;br /&gt;
 Maximum Force            0.000043     0.000450     YES&lt;br /&gt;
 RMS     Force            0.000043     0.000300     YES&lt;br /&gt;
 Maximum Displacement     0.000121     0.001800     YES&lt;br /&gt;
 RMS     Displacement     0.000172     0.001200     YES&lt;br /&gt;
&lt;br /&gt;
&amp;lt;/pre&amp;gt;&lt;br /&gt;
&amp;lt;pre&amp;gt;&lt;br /&gt;
Vibrational mode    Frequency    Infrared&lt;br /&gt;
#1             520.32       0.0000&lt;br /&gt;
&amp;lt;/pre&amp;gt;&lt;br /&gt;
There are no vibrational modes with negative frequencies&lt;br /&gt;
===Charge Analysis===&lt;br /&gt;
[[File:Adrian_Popescu_Cl2_Charges2.png|400px|center]]&lt;br /&gt;
As the Cl&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; molecule is made up of identical Cl atoms, the bond between them will be 100% covalent, the electrons that form the sigma bond are equally shared between the cl atoms, so the charge on each Cl atom is zero.&lt;br /&gt;
&lt;br /&gt;
===Molecular orbitals Analysis===&lt;br /&gt;
[[File:Adrian_Popescu_orbital1_.png|400px|thumb|center|2σg bonding orbital]]&lt;br /&gt;
The 2σg bonding orbital is deep in energy, occupied, and corresponds to the bonding orbital formed by the 2s AOs of the Cl atoms.&lt;/div&gt;</summary>
		<author><name>Ap5817</name></author>
	</entry>
	<entry>
		<id>https://chemwiki.ch.ic.ac.uk/index.php?title=File:Orbital1_.png&amp;diff=679435</id>
		<title>File:Orbital1 .png</title>
		<link rel="alternate" type="text/html" href="https://chemwiki.ch.ic.ac.uk/index.php?title=File:Orbital1_.png&amp;diff=679435"/>
		<updated>2018-03-07T19:49:38Z</updated>

		<summary type="html">&lt;p&gt;Ap5817: &lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;&lt;/div&gt;</summary>
		<author><name>Ap5817</name></author>
	</entry>
	<entry>
		<id>https://chemwiki.ch.ic.ac.uk/index.php?title=User:Ap5817&amp;diff=679409</id>
		<title>User:Ap5817</title>
		<link rel="alternate" type="text/html" href="https://chemwiki.ch.ic.ac.uk/index.php?title=User:Ap5817&amp;diff=679409"/>
		<updated>2018-03-07T19:36:54Z</updated>

		<summary type="html">&lt;p&gt;Ap5817: /* Charge Analysis */&lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;== NH3 molecule ==&lt;br /&gt;
=== NH3 calculations ===&lt;br /&gt;
Calculation method:RB3LYP&lt;br /&gt;
&lt;br /&gt;
Basis Set = 6-31G(d,p)&lt;br /&gt;
&lt;br /&gt;
Final Energy: E(RB3LYP) = -56.557768 a.u.&lt;br /&gt;
&lt;br /&gt;
Bond length:1.01789 Å&lt;br /&gt;
&lt;br /&gt;
Bond angle: 105.741 °C&lt;br /&gt;
&lt;br /&gt;
Point Group: C3v&amp;lt;pre&amp;gt;&lt;br /&gt;
Item               Value     Threshold  Converged?&lt;br /&gt;
 Maximum Force            0.000004     0.000450     YES&lt;br /&gt;
 RMS     Force            0.000004     0.000300     YES&lt;br /&gt;
 Maximum Displacement     0.000072     0.001800     YES&lt;br /&gt;
 RMS     Displacement     0.000035     0.001200     YES&lt;br /&gt;
&amp;lt;/pre&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&amp;lt;jmol&amp;gt;&amp;lt;jmolApplet&amp;gt;&lt;br /&gt;
&amp;lt;script&amp;gt;frame x.y&amp;lt;/script&amp;gt;&lt;br /&gt;
  &amp;lt;title&amp;gt;test molecule&amp;lt;/title&amp;gt;&lt;br /&gt;
  &amp;lt;color&amp;gt;black&amp;lt;/color&amp;gt;&lt;br /&gt;
  &amp;lt;size&amp;gt;200&amp;lt;/size&amp;gt;&lt;br /&gt;
  &amp;lt;uploadedFileContents&amp;gt;ADRIAN_POPESCU_PHUNT_NH3_OPTF_POP.LOG&amp;lt;/uploadedFileContents&amp;gt;&lt;br /&gt;
&amp;lt;/jmolApplet&amp;gt;&amp;lt;/jmol&amp;gt;&lt;br /&gt;
&lt;br /&gt;
[[Media:ADRIAN_POPESCU_PHUNT_NH3_OPTF_POP.LOG]]&lt;br /&gt;
&lt;br /&gt;
==Vibration analysis of NH3==&lt;br /&gt;
[[File:Adrian_Popescu_Display_Vibrations.png|1000px]]&lt;br /&gt;
===Vibrational modes===&lt;br /&gt;
Number of vibrational modes: 6&lt;br /&gt;
&lt;br /&gt;
Number of degenerate modes: 4 (2 pairs of degenerate vibrational modes &lt;br /&gt;
&lt;br /&gt;
Number of bending motions: 3&lt;br /&gt;
&lt;br /&gt;
Number of stretching motions: 3&lt;br /&gt;
&lt;br /&gt;
The most symmetric vibrational mode: mode #4&lt;br /&gt;
&lt;br /&gt;
The &#039;&#039;umbrella mode&#039;&#039;: mode #1&lt;br /&gt;
&lt;br /&gt;
Number of bands expected to be seen in an experimental spectrum of gaseous ammonia: 5&lt;br /&gt;
===Charge Analysis===&lt;br /&gt;
[[File:Adrian_Popescu_Charges2.png|400px|center]]&lt;br /&gt;
&lt;br /&gt;
Charge on the N atom: -1.125&lt;br /&gt;
&lt;br /&gt;
Charge on the H atom: 0.375&lt;br /&gt;
&lt;br /&gt;
As Nitrogen has an electronegativity value of 3.04, which is significantly larger than the one of Hidrogen (2.2), it is expected that on the Nitrogen there will be a negative charge and on Hidrogen a possitive charge.&lt;br /&gt;
&lt;br /&gt;
==Reactivity of the Haber-Bosch process==&lt;br /&gt;
===Analysis of H2===&lt;br /&gt;
Calculation method:RB3LYP&lt;br /&gt;
&lt;br /&gt;
Basis Set = 6-31G(d,p)&lt;br /&gt;
&lt;br /&gt;
Final Energy: E(RB3LYP) = -1.1785393 a.u.&lt;br /&gt;
&lt;br /&gt;
Bond length:0.7428 Å&lt;br /&gt;
&amp;lt;pre&amp;gt;&lt;br /&gt;
Item               Value     Threshold  Converged?&lt;br /&gt;
 Maximum Force            0.000004     0.000450     YES&lt;br /&gt;
 RMS     Force            0.000004     0.000300     YES&lt;br /&gt;
 Maximum Displacement     0.000005     0.001800     YES&lt;br /&gt;
 RMS     Displacement     0.000007     0.001200     YES&amp;lt;/pre&amp;gt;&lt;br /&gt;
&amp;lt;pre&amp;gt;&lt;br /&gt;
Vibrational mode    Frequency    Infrared&lt;br /&gt;
#1             4465.6       0.0000&lt;br /&gt;
&amp;lt;/pre&amp;gt;&lt;br /&gt;
There are no vibrational modes with negative frequencies&lt;br /&gt;
===Analysis of N2===&lt;br /&gt;
Calculation method:RB3LYP&lt;br /&gt;
&lt;br /&gt;
Basis Set = 6-31G(d,p)&lt;br /&gt;
&lt;br /&gt;
Final Energy: E(RB3LYP) = -109.5241268 a.u.&lt;br /&gt;
&lt;br /&gt;
Bond length: 1.1055 Å&lt;br /&gt;
&amp;lt;pre&amp;gt;&lt;br /&gt;
Item               Value     Threshold  Converged?&lt;br /&gt;
 Maximum Force            0.000001     0.000450     YES&lt;br /&gt;
 RMS     Force            0.000001     0.000300     YES&lt;br /&gt;
 Maximum Displacement     0.000000     0.001800     YES&lt;br /&gt;
 RMS     Displacement     0.000000     0.001200     YES&lt;br /&gt;
&amp;lt;/pre&amp;gt;&lt;br /&gt;
&amp;lt;pre&amp;gt;&lt;br /&gt;
Vibrational mode    Frequency    Infrared&lt;br /&gt;
#1             2457.33       0.0000&lt;br /&gt;
&amp;lt;/pre&amp;gt;&lt;br /&gt;
There are no vibrational modes with negative frequencies&lt;br /&gt;
&lt;br /&gt;
===Calculation of the energy of the Haber-Bosch process===&lt;br /&gt;
N&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; + 3H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; -&amp;gt; 2NH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;&lt;br /&gt;
&lt;br /&gt;
E(NH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;)= -56.557768 a u&lt;br /&gt;
&lt;br /&gt;
2*E(NH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;)= -113.115536 a u&lt;br /&gt;
&lt;br /&gt;
E(N&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;)= -109.5251268 a u&lt;br /&gt;
&lt;br /&gt;
E(H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;)= -1.1785393 a u&lt;br /&gt;
&lt;br /&gt;
3*E(H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;)= -3.5359617 a u&lt;br /&gt;
&lt;br /&gt;
ΔE=2*E(NH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;) - [E(N&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;) + 3*E(H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;)] = -145.57 kj/mol&lt;br /&gt;
&lt;br /&gt;
As the reaction is exothermic, the ammonia product is more stable than the gaseous reactants.&lt;br /&gt;
==Analysis of Cl&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;==&lt;br /&gt;
===General Analysis===&lt;br /&gt;
Calculation method:RB3LYP&lt;br /&gt;
&lt;br /&gt;
Basis Set = 6-31G(d,p)&lt;br /&gt;
&lt;br /&gt;
Final Energy: E(RB3LYP) = -920.3498788 a.u.&lt;br /&gt;
&lt;br /&gt;
Bond length: 2.0417 Å&lt;br /&gt;
===Vibrational Analysis===&lt;br /&gt;
&amp;lt;pre&amp;gt;&lt;br /&gt;
 Item               Value     Threshold  Converged?&lt;br /&gt;
 Maximum Force            0.000043     0.000450     YES&lt;br /&gt;
 RMS     Force            0.000043     0.000300     YES&lt;br /&gt;
 Maximum Displacement     0.000121     0.001800     YES&lt;br /&gt;
 RMS     Displacement     0.000172     0.001200     YES&lt;br /&gt;
&lt;br /&gt;
&amp;lt;/pre&amp;gt;&lt;br /&gt;
&amp;lt;pre&amp;gt;&lt;br /&gt;
Vibrational mode    Frequency    Infrared&lt;br /&gt;
#1             520.32       0.0000&lt;br /&gt;
&amp;lt;/pre&amp;gt;&lt;br /&gt;
There are no vibrational modes with negative frequencies&lt;br /&gt;
===Charge Analysis===&lt;br /&gt;
[[File:Adrian_Popescu_Cl2_Charges2.png|400px|center]]&lt;br /&gt;
As the Cl&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; molecule is made up of identical Cl atoms, the bond between them will be 100% covalent, the electrons that form the sigma bond are equally shared between the cl atoms, so the charge on each Cl atom is zero.&lt;br /&gt;
&lt;br /&gt;
===Molecular orbitals Analysis===&lt;br /&gt;
[[File:Adrian_Popescu_orbital1.png|1000px|thumb|center|2σg bonding orbital]]&lt;br /&gt;
The 2σg bonding orbital is deep in energy, occupied, and corresponds to the bonding orbital formed by the 2s AOs of the Cl atoms.&lt;/div&gt;</summary>
		<author><name>Ap5817</name></author>
	</entry>
	<entry>
		<id>https://chemwiki.ch.ic.ac.uk/index.php?title=User:Ap5817&amp;diff=679408</id>
		<title>User:Ap5817</title>
		<link rel="alternate" type="text/html" href="https://chemwiki.ch.ic.ac.uk/index.php?title=User:Ap5817&amp;diff=679408"/>
		<updated>2018-03-07T19:35:51Z</updated>

		<summary type="html">&lt;p&gt;Ap5817: /* Charge Analysis */&lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;== NH3 molecule ==&lt;br /&gt;
=== NH3 calculations ===&lt;br /&gt;
Calculation method:RB3LYP&lt;br /&gt;
&lt;br /&gt;
Basis Set = 6-31G(d,p)&lt;br /&gt;
&lt;br /&gt;
Final Energy: E(RB3LYP) = -56.557768 a.u.&lt;br /&gt;
&lt;br /&gt;
Bond length:1.01789 Å&lt;br /&gt;
&lt;br /&gt;
Bond angle: 105.741 °C&lt;br /&gt;
&lt;br /&gt;
Point Group: C3v&amp;lt;pre&amp;gt;&lt;br /&gt;
Item               Value     Threshold  Converged?&lt;br /&gt;
 Maximum Force            0.000004     0.000450     YES&lt;br /&gt;
 RMS     Force            0.000004     0.000300     YES&lt;br /&gt;
 Maximum Displacement     0.000072     0.001800     YES&lt;br /&gt;
 RMS     Displacement     0.000035     0.001200     YES&lt;br /&gt;
&amp;lt;/pre&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&amp;lt;jmol&amp;gt;&amp;lt;jmolApplet&amp;gt;&lt;br /&gt;
&amp;lt;script&amp;gt;frame x.y&amp;lt;/script&amp;gt;&lt;br /&gt;
  &amp;lt;title&amp;gt;test molecule&amp;lt;/title&amp;gt;&lt;br /&gt;
  &amp;lt;color&amp;gt;black&amp;lt;/color&amp;gt;&lt;br /&gt;
  &amp;lt;size&amp;gt;200&amp;lt;/size&amp;gt;&lt;br /&gt;
  &amp;lt;uploadedFileContents&amp;gt;ADRIAN_POPESCU_PHUNT_NH3_OPTF_POP.LOG&amp;lt;/uploadedFileContents&amp;gt;&lt;br /&gt;
&amp;lt;/jmolApplet&amp;gt;&amp;lt;/jmol&amp;gt;&lt;br /&gt;
&lt;br /&gt;
[[Media:ADRIAN_POPESCU_PHUNT_NH3_OPTF_POP.LOG]]&lt;br /&gt;
&lt;br /&gt;
==Vibration analysis of NH3==&lt;br /&gt;
[[File:Adrian_Popescu_Display_Vibrations.png|1000px]]&lt;br /&gt;
===Vibrational modes===&lt;br /&gt;
Number of vibrational modes: 6&lt;br /&gt;
&lt;br /&gt;
Number of degenerate modes: 4 (2 pairs of degenerate vibrational modes &lt;br /&gt;
&lt;br /&gt;
Number of bending motions: 3&lt;br /&gt;
&lt;br /&gt;
Number of stretching motions: 3&lt;br /&gt;
&lt;br /&gt;
The most symmetric vibrational mode: mode #4&lt;br /&gt;
&lt;br /&gt;
The &#039;&#039;umbrella mode&#039;&#039;: mode #1&lt;br /&gt;
&lt;br /&gt;
Number of bands expected to be seen in an experimental spectrum of gaseous ammonia: 5&lt;br /&gt;
===Charge Analysis===&lt;br /&gt;
[[File:Adrian_Popescu_Charges2.png|400px]]&lt;br /&gt;
&lt;br /&gt;
Charge on the N atom: -1.125&lt;br /&gt;
&lt;br /&gt;
Charge on the H atom: 0.375&lt;br /&gt;
&lt;br /&gt;
As Nitrogen has an electronegativity value of 3.04, which is significantly larger than the one of Hidrogen (2.2), it is expected that on the Nitrogen there will be a negative charge and on Hidrogen a possitive charge.&lt;br /&gt;
&lt;br /&gt;
==Reactivity of the Haber-Bosch process==&lt;br /&gt;
===Analysis of H2===&lt;br /&gt;
Calculation method:RB3LYP&lt;br /&gt;
&lt;br /&gt;
Basis Set = 6-31G(d,p)&lt;br /&gt;
&lt;br /&gt;
Final Energy: E(RB3LYP) = -1.1785393 a.u.&lt;br /&gt;
&lt;br /&gt;
Bond length:0.7428 Å&lt;br /&gt;
&amp;lt;pre&amp;gt;&lt;br /&gt;
Item               Value     Threshold  Converged?&lt;br /&gt;
 Maximum Force            0.000004     0.000450     YES&lt;br /&gt;
 RMS     Force            0.000004     0.000300     YES&lt;br /&gt;
 Maximum Displacement     0.000005     0.001800     YES&lt;br /&gt;
 RMS     Displacement     0.000007     0.001200     YES&amp;lt;/pre&amp;gt;&lt;br /&gt;
&amp;lt;pre&amp;gt;&lt;br /&gt;
Vibrational mode    Frequency    Infrared&lt;br /&gt;
#1             4465.6       0.0000&lt;br /&gt;
&amp;lt;/pre&amp;gt;&lt;br /&gt;
There are no vibrational modes with negative frequencies&lt;br /&gt;
===Analysis of N2===&lt;br /&gt;
Calculation method:RB3LYP&lt;br /&gt;
&lt;br /&gt;
Basis Set = 6-31G(d,p)&lt;br /&gt;
&lt;br /&gt;
Final Energy: E(RB3LYP) = -109.5241268 a.u.&lt;br /&gt;
&lt;br /&gt;
Bond length: 1.1055 Å&lt;br /&gt;
&amp;lt;pre&amp;gt;&lt;br /&gt;
Item               Value     Threshold  Converged?&lt;br /&gt;
 Maximum Force            0.000001     0.000450     YES&lt;br /&gt;
 RMS     Force            0.000001     0.000300     YES&lt;br /&gt;
 Maximum Displacement     0.000000     0.001800     YES&lt;br /&gt;
 RMS     Displacement     0.000000     0.001200     YES&lt;br /&gt;
&amp;lt;/pre&amp;gt;&lt;br /&gt;
&amp;lt;pre&amp;gt;&lt;br /&gt;
Vibrational mode    Frequency    Infrared&lt;br /&gt;
#1             2457.33       0.0000&lt;br /&gt;
&amp;lt;/pre&amp;gt;&lt;br /&gt;
There are no vibrational modes with negative frequencies&lt;br /&gt;
&lt;br /&gt;
===Calculation of the energy of the Haber-Bosch process===&lt;br /&gt;
N&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; + 3H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; -&amp;gt; 2NH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;&lt;br /&gt;
&lt;br /&gt;
E(NH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;)= -56.557768 a u&lt;br /&gt;
&lt;br /&gt;
2*E(NH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;)= -113.115536 a u&lt;br /&gt;
&lt;br /&gt;
E(N&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;)= -109.5251268 a u&lt;br /&gt;
&lt;br /&gt;
E(H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;)= -1.1785393 a u&lt;br /&gt;
&lt;br /&gt;
3*E(H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;)= -3.5359617 a u&lt;br /&gt;
&lt;br /&gt;
ΔE=2*E(NH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;) - [E(N&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;) + 3*E(H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;)] = -145.57 kj/mol&lt;br /&gt;
&lt;br /&gt;
As the reaction is exothermic, the ammonia product is more stable than the gaseous reactants.&lt;br /&gt;
==Analysis of Cl&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;==&lt;br /&gt;
===General Analysis===&lt;br /&gt;
Calculation method:RB3LYP&lt;br /&gt;
&lt;br /&gt;
Basis Set = 6-31G(d,p)&lt;br /&gt;
&lt;br /&gt;
Final Energy: E(RB3LYP) = -920.3498788 a.u.&lt;br /&gt;
&lt;br /&gt;
Bond length: 2.0417 Å&lt;br /&gt;
===Vibrational Analysis===&lt;br /&gt;
&amp;lt;pre&amp;gt;&lt;br /&gt;
 Item               Value     Threshold  Converged?&lt;br /&gt;
 Maximum Force            0.000043     0.000450     YES&lt;br /&gt;
 RMS     Force            0.000043     0.000300     YES&lt;br /&gt;
 Maximum Displacement     0.000121     0.001800     YES&lt;br /&gt;
 RMS     Displacement     0.000172     0.001200     YES&lt;br /&gt;
&lt;br /&gt;
&amp;lt;/pre&amp;gt;&lt;br /&gt;
&amp;lt;pre&amp;gt;&lt;br /&gt;
Vibrational mode    Frequency    Infrared&lt;br /&gt;
#1             520.32       0.0000&lt;br /&gt;
&amp;lt;/pre&amp;gt;&lt;br /&gt;
There are no vibrational modes with negative frequencies&lt;br /&gt;
===Charge Analysis===&lt;br /&gt;
[[File:Adrian_Popescu_Cl2_Charges2.png|400px|center]]&lt;br /&gt;
As the Cl&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; molecule is made up of identical Cl atoms, the bond between them will be 100% covalent, the electrons that form the sigma bond are equally shared between the cl atoms, so the charge on each Cl atom is zero.&lt;br /&gt;
&lt;br /&gt;
===Molecular orbitals Analysis===&lt;br /&gt;
[[File:Adrian_Popescu_orbital1.png|1000px|thumb|center|2σg bonding orbital]]&lt;br /&gt;
The 2σg bonding orbital is deep in energy, occupied, and corresponds to the bonding orbital formed by the 2s AOs of the Cl atoms.&lt;/div&gt;</summary>
		<author><name>Ap5817</name></author>
	</entry>
	<entry>
		<id>https://chemwiki.ch.ic.ac.uk/index.php?title=File:Adrian_Popescu_Cl2_Charges2.png&amp;diff=679407</id>
		<title>File:Adrian Popescu Cl2 Charges2.png</title>
		<link rel="alternate" type="text/html" href="https://chemwiki.ch.ic.ac.uk/index.php?title=File:Adrian_Popescu_Cl2_Charges2.png&amp;diff=679407"/>
		<updated>2018-03-07T19:35:23Z</updated>

		<summary type="html">&lt;p&gt;Ap5817: &lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;&lt;/div&gt;</summary>
		<author><name>Ap5817</name></author>
	</entry>
	<entry>
		<id>https://chemwiki.ch.ic.ac.uk/index.php?title=User:Ap5817&amp;diff=679404</id>
		<title>User:Ap5817</title>
		<link rel="alternate" type="text/html" href="https://chemwiki.ch.ic.ac.uk/index.php?title=User:Ap5817&amp;diff=679404"/>
		<updated>2018-03-07T19:30:20Z</updated>

		<summary type="html">&lt;p&gt;Ap5817: /* Charge Analysis */&lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;== NH3 molecule ==&lt;br /&gt;
=== NH3 calculations ===&lt;br /&gt;
Calculation method:RB3LYP&lt;br /&gt;
&lt;br /&gt;
Basis Set = 6-31G(d,p)&lt;br /&gt;
&lt;br /&gt;
Final Energy: E(RB3LYP) = -56.557768 a.u.&lt;br /&gt;
&lt;br /&gt;
Bond length:1.01789 Å&lt;br /&gt;
&lt;br /&gt;
Bond angle: 105.741 °C&lt;br /&gt;
&lt;br /&gt;
Point Group: C3v&amp;lt;pre&amp;gt;&lt;br /&gt;
Item               Value     Threshold  Converged?&lt;br /&gt;
 Maximum Force            0.000004     0.000450     YES&lt;br /&gt;
 RMS     Force            0.000004     0.000300     YES&lt;br /&gt;
 Maximum Displacement     0.000072     0.001800     YES&lt;br /&gt;
 RMS     Displacement     0.000035     0.001200     YES&lt;br /&gt;
&amp;lt;/pre&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&amp;lt;jmol&amp;gt;&amp;lt;jmolApplet&amp;gt;&lt;br /&gt;
&amp;lt;script&amp;gt;frame x.y&amp;lt;/script&amp;gt;&lt;br /&gt;
  &amp;lt;title&amp;gt;test molecule&amp;lt;/title&amp;gt;&lt;br /&gt;
  &amp;lt;color&amp;gt;black&amp;lt;/color&amp;gt;&lt;br /&gt;
  &amp;lt;size&amp;gt;200&amp;lt;/size&amp;gt;&lt;br /&gt;
  &amp;lt;uploadedFileContents&amp;gt;ADRIAN_POPESCU_PHUNT_NH3_OPTF_POP.LOG&amp;lt;/uploadedFileContents&amp;gt;&lt;br /&gt;
&amp;lt;/jmolApplet&amp;gt;&amp;lt;/jmol&amp;gt;&lt;br /&gt;
&lt;br /&gt;
[[Media:ADRIAN_POPESCU_PHUNT_NH3_OPTF_POP.LOG]]&lt;br /&gt;
&lt;br /&gt;
==Vibration analysis of NH3==&lt;br /&gt;
[[File:Adrian_Popescu_Display_Vibrations.png|1000px]]&lt;br /&gt;
===Vibrational modes===&lt;br /&gt;
Number of vibrational modes: 6&lt;br /&gt;
&lt;br /&gt;
Number of degenerate modes: 4 (2 pairs of degenerate vibrational modes &lt;br /&gt;
&lt;br /&gt;
Number of bending motions: 3&lt;br /&gt;
&lt;br /&gt;
Number of stretching motions: 3&lt;br /&gt;
&lt;br /&gt;
The most symmetric vibrational mode: mode #4&lt;br /&gt;
&lt;br /&gt;
The &#039;&#039;umbrella mode&#039;&#039;: mode #1&lt;br /&gt;
&lt;br /&gt;
Number of bands expected to be seen in an experimental spectrum of gaseous ammonia: 5&lt;br /&gt;
===Charge Analysis===&lt;br /&gt;
[[File:Adrian_Popescu_Charges2.png|400px]]&lt;br /&gt;
&lt;br /&gt;
Charge on the N atom: -1.125&lt;br /&gt;
&lt;br /&gt;
Charge on the H atom: 0.375&lt;br /&gt;
&lt;br /&gt;
As Nitrogen has an electronegativity value of 3.04, which is significantly larger than the one of Hidrogen (2.2), it is expected that on the Nitrogen there will be a negative charge and on Hidrogen a possitive charge.&lt;br /&gt;
&lt;br /&gt;
==Reactivity of the Haber-Bosch process==&lt;br /&gt;
===Analysis of H2===&lt;br /&gt;
Calculation method:RB3LYP&lt;br /&gt;
&lt;br /&gt;
Basis Set = 6-31G(d,p)&lt;br /&gt;
&lt;br /&gt;
Final Energy: E(RB3LYP) = -1.1785393 a.u.&lt;br /&gt;
&lt;br /&gt;
Bond length:0.7428 Å&lt;br /&gt;
&amp;lt;pre&amp;gt;&lt;br /&gt;
Item               Value     Threshold  Converged?&lt;br /&gt;
 Maximum Force            0.000004     0.000450     YES&lt;br /&gt;
 RMS     Force            0.000004     0.000300     YES&lt;br /&gt;
 Maximum Displacement     0.000005     0.001800     YES&lt;br /&gt;
 RMS     Displacement     0.000007     0.001200     YES&amp;lt;/pre&amp;gt;&lt;br /&gt;
&amp;lt;pre&amp;gt;&lt;br /&gt;
Vibrational mode    Frequency    Infrared&lt;br /&gt;
#1             4465.6       0.0000&lt;br /&gt;
&amp;lt;/pre&amp;gt;&lt;br /&gt;
There are no vibrational modes with negative frequencies&lt;br /&gt;
===Analysis of N2===&lt;br /&gt;
Calculation method:RB3LYP&lt;br /&gt;
&lt;br /&gt;
Basis Set = 6-31G(d,p)&lt;br /&gt;
&lt;br /&gt;
Final Energy: E(RB3LYP) = -109.5241268 a.u.&lt;br /&gt;
&lt;br /&gt;
Bond length: 1.1055 Å&lt;br /&gt;
&amp;lt;pre&amp;gt;&lt;br /&gt;
Item               Value     Threshold  Converged?&lt;br /&gt;
 Maximum Force            0.000001     0.000450     YES&lt;br /&gt;
 RMS     Force            0.000001     0.000300     YES&lt;br /&gt;
 Maximum Displacement     0.000000     0.001800     YES&lt;br /&gt;
 RMS     Displacement     0.000000     0.001200     YES&lt;br /&gt;
&amp;lt;/pre&amp;gt;&lt;br /&gt;
&amp;lt;pre&amp;gt;&lt;br /&gt;
Vibrational mode    Frequency    Infrared&lt;br /&gt;
#1             2457.33       0.0000&lt;br /&gt;
&amp;lt;/pre&amp;gt;&lt;br /&gt;
There are no vibrational modes with negative frequencies&lt;br /&gt;
&lt;br /&gt;
===Calculation of the energy of the Haber-Bosch process===&lt;br /&gt;
N&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; + 3H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; -&amp;gt; 2NH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;&lt;br /&gt;
&lt;br /&gt;
E(NH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;)= -56.557768 a u&lt;br /&gt;
&lt;br /&gt;
2*E(NH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;)= -113.115536 a u&lt;br /&gt;
&lt;br /&gt;
E(N&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;)= -109.5251268 a u&lt;br /&gt;
&lt;br /&gt;
E(H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;)= -1.1785393 a u&lt;br /&gt;
&lt;br /&gt;
3*E(H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;)= -3.5359617 a u&lt;br /&gt;
&lt;br /&gt;
ΔE=2*E(NH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;) - [E(N&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;) + 3*E(H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;)] = -145.57 kj/mol&lt;br /&gt;
&lt;br /&gt;
As the reaction is exothermic, the ammonia product is more stable than the gaseous reactants.&lt;br /&gt;
==Analysis of Cl&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;==&lt;br /&gt;
===General Analysis===&lt;br /&gt;
Calculation method:RB3LYP&lt;br /&gt;
&lt;br /&gt;
Basis Set = 6-31G(d,p)&lt;br /&gt;
&lt;br /&gt;
Final Energy: E(RB3LYP) = -920.3498788 a.u.&lt;br /&gt;
&lt;br /&gt;
Bond length: 2.0417 Å&lt;br /&gt;
===Vibrational Analysis===&lt;br /&gt;
&amp;lt;pre&amp;gt;&lt;br /&gt;
 Item               Value     Threshold  Converged?&lt;br /&gt;
 Maximum Force            0.000043     0.000450     YES&lt;br /&gt;
 RMS     Force            0.000043     0.000300     YES&lt;br /&gt;
 Maximum Displacement     0.000121     0.001800     YES&lt;br /&gt;
 RMS     Displacement     0.000172     0.001200     YES&lt;br /&gt;
&lt;br /&gt;
&amp;lt;/pre&amp;gt;&lt;br /&gt;
&amp;lt;pre&amp;gt;&lt;br /&gt;
Vibrational mode    Frequency    Infrared&lt;br /&gt;
#1             520.32       0.0000&lt;br /&gt;
&amp;lt;/pre&amp;gt;&lt;br /&gt;
There are no vibrational modes with negative frequencies&lt;br /&gt;
===Charge Analysis===&lt;br /&gt;
[[File:Adrian_Popescu_Cl2_Charges.png|1000px|center]]&lt;br /&gt;
As the Cl&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; molecule is made up of identical Cl atoms, the bond between them will be 100% covalent, the electrons that form the sigma bond are equally shared between the cl atoms, so the charge on each Cl atom is zero.&lt;br /&gt;
&lt;br /&gt;
===Molecular orbitals Analysis===&lt;br /&gt;
[[File:Adrian_Popescu_orbital1.png|1000px|thumb|center|2σg bonding orbital]]&lt;br /&gt;
The 2σg bonding orbital is deep in energy, occupied, and corresponds to the bonding orbital formed by the 2s AOs of the Cl atoms.&lt;/div&gt;</summary>
		<author><name>Ap5817</name></author>
	</entry>
	<entry>
		<id>https://chemwiki.ch.ic.ac.uk/index.php?title=User:Ap5817&amp;diff=679403</id>
		<title>User:Ap5817</title>
		<link rel="alternate" type="text/html" href="https://chemwiki.ch.ic.ac.uk/index.php?title=User:Ap5817&amp;diff=679403"/>
		<updated>2018-03-07T19:30:08Z</updated>

		<summary type="html">&lt;p&gt;Ap5817: /* Charge Analysis */&lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;== NH3 molecule ==&lt;br /&gt;
=== NH3 calculations ===&lt;br /&gt;
Calculation method:RB3LYP&lt;br /&gt;
&lt;br /&gt;
Basis Set = 6-31G(d,p)&lt;br /&gt;
&lt;br /&gt;
Final Energy: E(RB3LYP) = -56.557768 a.u.&lt;br /&gt;
&lt;br /&gt;
Bond length:1.01789 Å&lt;br /&gt;
&lt;br /&gt;
Bond angle: 105.741 °C&lt;br /&gt;
&lt;br /&gt;
Point Group: C3v&amp;lt;pre&amp;gt;&lt;br /&gt;
Item               Value     Threshold  Converged?&lt;br /&gt;
 Maximum Force            0.000004     0.000450     YES&lt;br /&gt;
 RMS     Force            0.000004     0.000300     YES&lt;br /&gt;
 Maximum Displacement     0.000072     0.001800     YES&lt;br /&gt;
 RMS     Displacement     0.000035     0.001200     YES&lt;br /&gt;
&amp;lt;/pre&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&amp;lt;jmol&amp;gt;&amp;lt;jmolApplet&amp;gt;&lt;br /&gt;
&amp;lt;script&amp;gt;frame x.y&amp;lt;/script&amp;gt;&lt;br /&gt;
  &amp;lt;title&amp;gt;test molecule&amp;lt;/title&amp;gt;&lt;br /&gt;
  &amp;lt;color&amp;gt;black&amp;lt;/color&amp;gt;&lt;br /&gt;
  &amp;lt;size&amp;gt;200&amp;lt;/size&amp;gt;&lt;br /&gt;
  &amp;lt;uploadedFileContents&amp;gt;ADRIAN_POPESCU_PHUNT_NH3_OPTF_POP.LOG&amp;lt;/uploadedFileContents&amp;gt;&lt;br /&gt;
&amp;lt;/jmolApplet&amp;gt;&amp;lt;/jmol&amp;gt;&lt;br /&gt;
&lt;br /&gt;
[[Media:ADRIAN_POPESCU_PHUNT_NH3_OPTF_POP.LOG]]&lt;br /&gt;
&lt;br /&gt;
==Vibration analysis of NH3==&lt;br /&gt;
[[File:Adrian_Popescu_Display_Vibrations.png|1000px]]&lt;br /&gt;
===Vibrational modes===&lt;br /&gt;
Number of vibrational modes: 6&lt;br /&gt;
&lt;br /&gt;
Number of degenerate modes: 4 (2 pairs of degenerate vibrational modes &lt;br /&gt;
&lt;br /&gt;
Number of bending motions: 3&lt;br /&gt;
&lt;br /&gt;
Number of stretching motions: 3&lt;br /&gt;
&lt;br /&gt;
The most symmetric vibrational mode: mode #4&lt;br /&gt;
&lt;br /&gt;
The &#039;&#039;umbrella mode&#039;&#039;: mode #1&lt;br /&gt;
&lt;br /&gt;
Number of bands expected to be seen in an experimental spectrum of gaseous ammonia: 5&lt;br /&gt;
===Charge Analysis===&lt;br /&gt;
[[File:Adrian_Popescu_Charges2.png|150px]]&lt;br /&gt;
&lt;br /&gt;
Charge on the N atom: -1.125&lt;br /&gt;
&lt;br /&gt;
Charge on the H atom: 0.375&lt;br /&gt;
&lt;br /&gt;
As Nitrogen has an electronegativity value of 3.04, which is significantly larger than the one of Hidrogen (2.2), it is expected that on the Nitrogen there will be a negative charge and on Hidrogen a possitive charge.&lt;br /&gt;
&lt;br /&gt;
==Reactivity of the Haber-Bosch process==&lt;br /&gt;
===Analysis of H2===&lt;br /&gt;
Calculation method:RB3LYP&lt;br /&gt;
&lt;br /&gt;
Basis Set = 6-31G(d,p)&lt;br /&gt;
&lt;br /&gt;
Final Energy: E(RB3LYP) = -1.1785393 a.u.&lt;br /&gt;
&lt;br /&gt;
Bond length:0.7428 Å&lt;br /&gt;
&amp;lt;pre&amp;gt;&lt;br /&gt;
Item               Value     Threshold  Converged?&lt;br /&gt;
 Maximum Force            0.000004     0.000450     YES&lt;br /&gt;
 RMS     Force            0.000004     0.000300     YES&lt;br /&gt;
 Maximum Displacement     0.000005     0.001800     YES&lt;br /&gt;
 RMS     Displacement     0.000007     0.001200     YES&amp;lt;/pre&amp;gt;&lt;br /&gt;
&amp;lt;pre&amp;gt;&lt;br /&gt;
Vibrational mode    Frequency    Infrared&lt;br /&gt;
#1             4465.6       0.0000&lt;br /&gt;
&amp;lt;/pre&amp;gt;&lt;br /&gt;
There are no vibrational modes with negative frequencies&lt;br /&gt;
===Analysis of N2===&lt;br /&gt;
Calculation method:RB3LYP&lt;br /&gt;
&lt;br /&gt;
Basis Set = 6-31G(d,p)&lt;br /&gt;
&lt;br /&gt;
Final Energy: E(RB3LYP) = -109.5241268 a.u.&lt;br /&gt;
&lt;br /&gt;
Bond length: 1.1055 Å&lt;br /&gt;
&amp;lt;pre&amp;gt;&lt;br /&gt;
Item               Value     Threshold  Converged?&lt;br /&gt;
 Maximum Force            0.000001     0.000450     YES&lt;br /&gt;
 RMS     Force            0.000001     0.000300     YES&lt;br /&gt;
 Maximum Displacement     0.000000     0.001800     YES&lt;br /&gt;
 RMS     Displacement     0.000000     0.001200     YES&lt;br /&gt;
&amp;lt;/pre&amp;gt;&lt;br /&gt;
&amp;lt;pre&amp;gt;&lt;br /&gt;
Vibrational mode    Frequency    Infrared&lt;br /&gt;
#1             2457.33       0.0000&lt;br /&gt;
&amp;lt;/pre&amp;gt;&lt;br /&gt;
There are no vibrational modes with negative frequencies&lt;br /&gt;
&lt;br /&gt;
===Calculation of the energy of the Haber-Bosch process===&lt;br /&gt;
N&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; + 3H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; -&amp;gt; 2NH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;&lt;br /&gt;
&lt;br /&gt;
E(NH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;)= -56.557768 a u&lt;br /&gt;
&lt;br /&gt;
2*E(NH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;)= -113.115536 a u&lt;br /&gt;
&lt;br /&gt;
E(N&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;)= -109.5251268 a u&lt;br /&gt;
&lt;br /&gt;
E(H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;)= -1.1785393 a u&lt;br /&gt;
&lt;br /&gt;
3*E(H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;)= -3.5359617 a u&lt;br /&gt;
&lt;br /&gt;
ΔE=2*E(NH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;) - [E(N&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;) + 3*E(H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;)] = -145.57 kj/mol&lt;br /&gt;
&lt;br /&gt;
As the reaction is exothermic, the ammonia product is more stable than the gaseous reactants.&lt;br /&gt;
==Analysis of Cl&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;==&lt;br /&gt;
===General Analysis===&lt;br /&gt;
Calculation method:RB3LYP&lt;br /&gt;
&lt;br /&gt;
Basis Set = 6-31G(d,p)&lt;br /&gt;
&lt;br /&gt;
Final Energy: E(RB3LYP) = -920.3498788 a.u.&lt;br /&gt;
&lt;br /&gt;
Bond length: 2.0417 Å&lt;br /&gt;
===Vibrational Analysis===&lt;br /&gt;
&amp;lt;pre&amp;gt;&lt;br /&gt;
 Item               Value     Threshold  Converged?&lt;br /&gt;
 Maximum Force            0.000043     0.000450     YES&lt;br /&gt;
 RMS     Force            0.000043     0.000300     YES&lt;br /&gt;
 Maximum Displacement     0.000121     0.001800     YES&lt;br /&gt;
 RMS     Displacement     0.000172     0.001200     YES&lt;br /&gt;
&lt;br /&gt;
&amp;lt;/pre&amp;gt;&lt;br /&gt;
&amp;lt;pre&amp;gt;&lt;br /&gt;
Vibrational mode    Frequency    Infrared&lt;br /&gt;
#1             520.32       0.0000&lt;br /&gt;
&amp;lt;/pre&amp;gt;&lt;br /&gt;
There are no vibrational modes with negative frequencies&lt;br /&gt;
===Charge Analysis===&lt;br /&gt;
[[File:Adrian_Popescu_Cl2_Charges.png|1000px|center]]&lt;br /&gt;
As the Cl&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; molecule is made up of identical Cl atoms, the bond between them will be 100% covalent, the electrons that form the sigma bond are equally shared between the cl atoms, so the charge on each Cl atom is zero.&lt;br /&gt;
&lt;br /&gt;
===Molecular orbitals Analysis===&lt;br /&gt;
[[File:Adrian_Popescu_orbital1.png|1000px|thumb|center|2σg bonding orbital]]&lt;br /&gt;
The 2σg bonding orbital is deep in energy, occupied, and corresponds to the bonding orbital formed by the 2s AOs of the Cl atoms.&lt;/div&gt;</summary>
		<author><name>Ap5817</name></author>
	</entry>
	<entry>
		<id>https://chemwiki.ch.ic.ac.uk/index.php?title=User:Ap5817&amp;diff=679402</id>
		<title>User:Ap5817</title>
		<link rel="alternate" type="text/html" href="https://chemwiki.ch.ic.ac.uk/index.php?title=User:Ap5817&amp;diff=679402"/>
		<updated>2018-03-07T19:29:58Z</updated>

		<summary type="html">&lt;p&gt;Ap5817: /* Charge Analysis */&lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;== NH3 molecule ==&lt;br /&gt;
=== NH3 calculations ===&lt;br /&gt;
Calculation method:RB3LYP&lt;br /&gt;
&lt;br /&gt;
Basis Set = 6-31G(d,p)&lt;br /&gt;
&lt;br /&gt;
Final Energy: E(RB3LYP) = -56.557768 a.u.&lt;br /&gt;
&lt;br /&gt;
Bond length:1.01789 Å&lt;br /&gt;
&lt;br /&gt;
Bond angle: 105.741 °C&lt;br /&gt;
&lt;br /&gt;
Point Group: C3v&amp;lt;pre&amp;gt;&lt;br /&gt;
Item               Value     Threshold  Converged?&lt;br /&gt;
 Maximum Force            0.000004     0.000450     YES&lt;br /&gt;
 RMS     Force            0.000004     0.000300     YES&lt;br /&gt;
 Maximum Displacement     0.000072     0.001800     YES&lt;br /&gt;
 RMS     Displacement     0.000035     0.001200     YES&lt;br /&gt;
&amp;lt;/pre&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&amp;lt;jmol&amp;gt;&amp;lt;jmolApplet&amp;gt;&lt;br /&gt;
&amp;lt;script&amp;gt;frame x.y&amp;lt;/script&amp;gt;&lt;br /&gt;
  &amp;lt;title&amp;gt;test molecule&amp;lt;/title&amp;gt;&lt;br /&gt;
  &amp;lt;color&amp;gt;black&amp;lt;/color&amp;gt;&lt;br /&gt;
  &amp;lt;size&amp;gt;200&amp;lt;/size&amp;gt;&lt;br /&gt;
  &amp;lt;uploadedFileContents&amp;gt;ADRIAN_POPESCU_PHUNT_NH3_OPTF_POP.LOG&amp;lt;/uploadedFileContents&amp;gt;&lt;br /&gt;
&amp;lt;/jmolApplet&amp;gt;&amp;lt;/jmol&amp;gt;&lt;br /&gt;
&lt;br /&gt;
[[Media:ADRIAN_POPESCU_PHUNT_NH3_OPTF_POP.LOG]]&lt;br /&gt;
&lt;br /&gt;
==Vibration analysis of NH3==&lt;br /&gt;
[[File:Adrian_Popescu_Display_Vibrations.png|1000px]]&lt;br /&gt;
===Vibrational modes===&lt;br /&gt;
Number of vibrational modes: 6&lt;br /&gt;
&lt;br /&gt;
Number of degenerate modes: 4 (2 pairs of degenerate vibrational modes &lt;br /&gt;
&lt;br /&gt;
Number of bending motions: 3&lt;br /&gt;
&lt;br /&gt;
Number of stretching motions: 3&lt;br /&gt;
&lt;br /&gt;
The most symmetric vibrational mode: mode #4&lt;br /&gt;
&lt;br /&gt;
The &#039;&#039;umbrella mode&#039;&#039;: mode #1&lt;br /&gt;
&lt;br /&gt;
Number of bands expected to be seen in an experimental spectrum of gaseous ammonia: 5&lt;br /&gt;
===Charge Analysis===&lt;br /&gt;
[[File:Adrian_Popescu_Charges2.png|1500px]]&lt;br /&gt;
&lt;br /&gt;
Charge on the N atom: -1.125&lt;br /&gt;
&lt;br /&gt;
Charge on the H atom: 0.375&lt;br /&gt;
&lt;br /&gt;
As Nitrogen has an electronegativity value of 3.04, which is significantly larger than the one of Hidrogen (2.2), it is expected that on the Nitrogen there will be a negative charge and on Hidrogen a possitive charge.&lt;br /&gt;
&lt;br /&gt;
==Reactivity of the Haber-Bosch process==&lt;br /&gt;
===Analysis of H2===&lt;br /&gt;
Calculation method:RB3LYP&lt;br /&gt;
&lt;br /&gt;
Basis Set = 6-31G(d,p)&lt;br /&gt;
&lt;br /&gt;
Final Energy: E(RB3LYP) = -1.1785393 a.u.&lt;br /&gt;
&lt;br /&gt;
Bond length:0.7428 Å&lt;br /&gt;
&amp;lt;pre&amp;gt;&lt;br /&gt;
Item               Value     Threshold  Converged?&lt;br /&gt;
 Maximum Force            0.000004     0.000450     YES&lt;br /&gt;
 RMS     Force            0.000004     0.000300     YES&lt;br /&gt;
 Maximum Displacement     0.000005     0.001800     YES&lt;br /&gt;
 RMS     Displacement     0.000007     0.001200     YES&amp;lt;/pre&amp;gt;&lt;br /&gt;
&amp;lt;pre&amp;gt;&lt;br /&gt;
Vibrational mode    Frequency    Infrared&lt;br /&gt;
#1             4465.6       0.0000&lt;br /&gt;
&amp;lt;/pre&amp;gt;&lt;br /&gt;
There are no vibrational modes with negative frequencies&lt;br /&gt;
===Analysis of N2===&lt;br /&gt;
Calculation method:RB3LYP&lt;br /&gt;
&lt;br /&gt;
Basis Set = 6-31G(d,p)&lt;br /&gt;
&lt;br /&gt;
Final Energy: E(RB3LYP) = -109.5241268 a.u.&lt;br /&gt;
&lt;br /&gt;
Bond length: 1.1055 Å&lt;br /&gt;
&amp;lt;pre&amp;gt;&lt;br /&gt;
Item               Value     Threshold  Converged?&lt;br /&gt;
 Maximum Force            0.000001     0.000450     YES&lt;br /&gt;
 RMS     Force            0.000001     0.000300     YES&lt;br /&gt;
 Maximum Displacement     0.000000     0.001800     YES&lt;br /&gt;
 RMS     Displacement     0.000000     0.001200     YES&lt;br /&gt;
&amp;lt;/pre&amp;gt;&lt;br /&gt;
&amp;lt;pre&amp;gt;&lt;br /&gt;
Vibrational mode    Frequency    Infrared&lt;br /&gt;
#1             2457.33       0.0000&lt;br /&gt;
&amp;lt;/pre&amp;gt;&lt;br /&gt;
There are no vibrational modes with negative frequencies&lt;br /&gt;
&lt;br /&gt;
===Calculation of the energy of the Haber-Bosch process===&lt;br /&gt;
N&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; + 3H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; -&amp;gt; 2NH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;&lt;br /&gt;
&lt;br /&gt;
E(NH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;)= -56.557768 a u&lt;br /&gt;
&lt;br /&gt;
2*E(NH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;)= -113.115536 a u&lt;br /&gt;
&lt;br /&gt;
E(N&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;)= -109.5251268 a u&lt;br /&gt;
&lt;br /&gt;
E(H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;)= -1.1785393 a u&lt;br /&gt;
&lt;br /&gt;
3*E(H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;)= -3.5359617 a u&lt;br /&gt;
&lt;br /&gt;
ΔE=2*E(NH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;) - [E(N&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;) + 3*E(H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;)] = -145.57 kj/mol&lt;br /&gt;
&lt;br /&gt;
As the reaction is exothermic, the ammonia product is more stable than the gaseous reactants.&lt;br /&gt;
==Analysis of Cl&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;==&lt;br /&gt;
===General Analysis===&lt;br /&gt;
Calculation method:RB3LYP&lt;br /&gt;
&lt;br /&gt;
Basis Set = 6-31G(d,p)&lt;br /&gt;
&lt;br /&gt;
Final Energy: E(RB3LYP) = -920.3498788 a.u.&lt;br /&gt;
&lt;br /&gt;
Bond length: 2.0417 Å&lt;br /&gt;
===Vibrational Analysis===&lt;br /&gt;
&amp;lt;pre&amp;gt;&lt;br /&gt;
 Item               Value     Threshold  Converged?&lt;br /&gt;
 Maximum Force            0.000043     0.000450     YES&lt;br /&gt;
 RMS     Force            0.000043     0.000300     YES&lt;br /&gt;
 Maximum Displacement     0.000121     0.001800     YES&lt;br /&gt;
 RMS     Displacement     0.000172     0.001200     YES&lt;br /&gt;
&lt;br /&gt;
&amp;lt;/pre&amp;gt;&lt;br /&gt;
&amp;lt;pre&amp;gt;&lt;br /&gt;
Vibrational mode    Frequency    Infrared&lt;br /&gt;
#1             520.32       0.0000&lt;br /&gt;
&amp;lt;/pre&amp;gt;&lt;br /&gt;
There are no vibrational modes with negative frequencies&lt;br /&gt;
===Charge Analysis===&lt;br /&gt;
[[File:Adrian_Popescu_Cl2_Charges.png|1000px|center]]&lt;br /&gt;
As the Cl&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; molecule is made up of identical Cl atoms, the bond between them will be 100% covalent, the electrons that form the sigma bond are equally shared between the cl atoms, so the charge on each Cl atom is zero.&lt;br /&gt;
&lt;br /&gt;
===Molecular orbitals Analysis===&lt;br /&gt;
[[File:Adrian_Popescu_orbital1.png|1000px|thumb|center|2σg bonding orbital]]&lt;br /&gt;
The 2σg bonding orbital is deep in energy, occupied, and corresponds to the bonding orbital formed by the 2s AOs of the Cl atoms.&lt;/div&gt;</summary>
		<author><name>Ap5817</name></author>
	</entry>
	<entry>
		<id>https://chemwiki.ch.ic.ac.uk/index.php?title=File:Adrian_Popescu_Charges2.png&amp;diff=679400</id>
		<title>File:Adrian Popescu Charges2.png</title>
		<link rel="alternate" type="text/html" href="https://chemwiki.ch.ic.ac.uk/index.php?title=File:Adrian_Popescu_Charges2.png&amp;diff=679400"/>
		<updated>2018-03-07T19:29:42Z</updated>

		<summary type="html">&lt;p&gt;Ap5817: &lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;&lt;/div&gt;</summary>
		<author><name>Ap5817</name></author>
	</entry>
	<entry>
		<id>https://chemwiki.ch.ic.ac.uk/index.php?title=User:Ap5817&amp;diff=679163</id>
		<title>User:Ap5817</title>
		<link rel="alternate" type="text/html" href="https://chemwiki.ch.ic.ac.uk/index.php?title=User:Ap5817&amp;diff=679163"/>
		<updated>2018-03-07T14:41:10Z</updated>

		<summary type="html">&lt;p&gt;Ap5817: /* Charge Analysis */&lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;== NH3 molecule ==&lt;br /&gt;
=== NH3 calculations ===&lt;br /&gt;
Calculation method:RB3LYP&lt;br /&gt;
&lt;br /&gt;
Basis Set = 6-31G(d,p)&lt;br /&gt;
&lt;br /&gt;
Final Energy: E(RB3LYP) = -56.557768 a.u.&lt;br /&gt;
&lt;br /&gt;
Bond length:1.01789 Å&lt;br /&gt;
&lt;br /&gt;
Bond angle: 105.741 °C&lt;br /&gt;
&lt;br /&gt;
Point Group: C3v&amp;lt;pre&amp;gt;&lt;br /&gt;
Item               Value     Threshold  Converged?&lt;br /&gt;
 Maximum Force            0.000004     0.000450     YES&lt;br /&gt;
 RMS     Force            0.000004     0.000300     YES&lt;br /&gt;
 Maximum Displacement     0.000072     0.001800     YES&lt;br /&gt;
 RMS     Displacement     0.000035     0.001200     YES&lt;br /&gt;
&amp;lt;/pre&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&amp;lt;jmol&amp;gt;&amp;lt;jmolApplet&amp;gt;&lt;br /&gt;
&amp;lt;script&amp;gt;frame x.y&amp;lt;/script&amp;gt;&lt;br /&gt;
  &amp;lt;title&amp;gt;test molecule&amp;lt;/title&amp;gt;&lt;br /&gt;
  &amp;lt;color&amp;gt;black&amp;lt;/color&amp;gt;&lt;br /&gt;
  &amp;lt;size&amp;gt;200&amp;lt;/size&amp;gt;&lt;br /&gt;
  &amp;lt;uploadedFileContents&amp;gt;ADRIAN_POPESCU_PHUNT_NH3_OPTF_POP.LOG&amp;lt;/uploadedFileContents&amp;gt;&lt;br /&gt;
&amp;lt;/jmolApplet&amp;gt;&amp;lt;/jmol&amp;gt;&lt;br /&gt;
&lt;br /&gt;
[[Media:ADRIAN_POPESCU_PHUNT_NH3_OPTF_POP.LOG]]&lt;br /&gt;
&lt;br /&gt;
==Vibration analysis of NH3==&lt;br /&gt;
[[File:Adrian_Popescu_Display_Vibrations.png|1000px]]&lt;br /&gt;
===Vibrational modes===&lt;br /&gt;
Number of vibrational modes: 6&lt;br /&gt;
&lt;br /&gt;
Number of degenerate modes: 4 (2 pairs of degenerate vibrational modes &lt;br /&gt;
&lt;br /&gt;
Number of bending motions: 3&lt;br /&gt;
&lt;br /&gt;
Number of stretching motions: 3&lt;br /&gt;
&lt;br /&gt;
The most symmetric vibrational mode: mode #4&lt;br /&gt;
&lt;br /&gt;
The &#039;&#039;umbrella mode&#039;&#039;: mode #1&lt;br /&gt;
&lt;br /&gt;
Number of bands expected to be seen in an experimental spectrum of gaseous ammonia: 5&lt;br /&gt;
===Charge Analysis===&lt;br /&gt;
[[File:Adrian_Popescu_Charges.png|1500px]]&lt;br /&gt;
&lt;br /&gt;
Charge on the N atom: -1.125&lt;br /&gt;
&lt;br /&gt;
Charge on the H atom: 0.375&lt;br /&gt;
&lt;br /&gt;
As Nitrogen has an electronegativity value of 3.04, which is significantly larger than the one of Hidrogen (2.2), it is expected that on the Nitrogen there will be a negative charge and on Hidrogen a possitive charge.&lt;br /&gt;
&lt;br /&gt;
==Reactivity of the Haber-Bosch process==&lt;br /&gt;
===Analysis of H2===&lt;br /&gt;
Calculation method:RB3LYP&lt;br /&gt;
&lt;br /&gt;
Basis Set = 6-31G(d,p)&lt;br /&gt;
&lt;br /&gt;
Final Energy: E(RB3LYP) = -1.1785393 a.u.&lt;br /&gt;
&lt;br /&gt;
Bond length:0.7428 Å&lt;br /&gt;
&amp;lt;pre&amp;gt;&lt;br /&gt;
Item               Value     Threshold  Converged?&lt;br /&gt;
 Maximum Force            0.000004     0.000450     YES&lt;br /&gt;
 RMS     Force            0.000004     0.000300     YES&lt;br /&gt;
 Maximum Displacement     0.000005     0.001800     YES&lt;br /&gt;
 RMS     Displacement     0.000007     0.001200     YES&amp;lt;/pre&amp;gt;&lt;br /&gt;
&amp;lt;pre&amp;gt;&lt;br /&gt;
Vibrational mode    Frequency    Infrared&lt;br /&gt;
#1             4465.6       0.0000&lt;br /&gt;
&amp;lt;/pre&amp;gt;&lt;br /&gt;
There are no vibrational modes with negative frequencies&lt;br /&gt;
===Analysis of N2===&lt;br /&gt;
Calculation method:RB3LYP&lt;br /&gt;
&lt;br /&gt;
Basis Set = 6-31G(d,p)&lt;br /&gt;
&lt;br /&gt;
Final Energy: E(RB3LYP) = -109.5241268 a.u.&lt;br /&gt;
&lt;br /&gt;
Bond length: 1.1055 Å&lt;br /&gt;
&amp;lt;pre&amp;gt;&lt;br /&gt;
Item               Value     Threshold  Converged?&lt;br /&gt;
 Maximum Force            0.000001     0.000450     YES&lt;br /&gt;
 RMS     Force            0.000001     0.000300     YES&lt;br /&gt;
 Maximum Displacement     0.000000     0.001800     YES&lt;br /&gt;
 RMS     Displacement     0.000000     0.001200     YES&lt;br /&gt;
&amp;lt;/pre&amp;gt;&lt;br /&gt;
&amp;lt;pre&amp;gt;&lt;br /&gt;
Vibrational mode    Frequency    Infrared&lt;br /&gt;
#1             2457.33       0.0000&lt;br /&gt;
&amp;lt;/pre&amp;gt;&lt;br /&gt;
There are no vibrational modes with negative frequencies&lt;br /&gt;
&lt;br /&gt;
===Calculation of the energy of the Haber-Bosch process===&lt;br /&gt;
N&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; + 3H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; -&amp;gt; 2NH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;&lt;br /&gt;
&lt;br /&gt;
E(NH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;)= -56.557768 a u&lt;br /&gt;
&lt;br /&gt;
2*E(NH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;)= -113.115536 a u&lt;br /&gt;
&lt;br /&gt;
E(N&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;)= -109.5251268 a u&lt;br /&gt;
&lt;br /&gt;
E(H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;)= -1.1785393 a u&lt;br /&gt;
&lt;br /&gt;
3*E(H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;)= -3.5359617 a u&lt;br /&gt;
&lt;br /&gt;
ΔE=2*E(NH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;) - [E(N&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;) + 3*E(H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;)] = -145.57 kj/mol&lt;br /&gt;
&lt;br /&gt;
As the reaction is exothermic, the ammonia product is more stable than the gaseous reactants.&lt;br /&gt;
==Analysis of Cl&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;==&lt;br /&gt;
===General Analysis===&lt;br /&gt;
Calculation method:RB3LYP&lt;br /&gt;
&lt;br /&gt;
Basis Set = 6-31G(d,p)&lt;br /&gt;
&lt;br /&gt;
Final Energy: E(RB3LYP) = -920.3498788 a.u.&lt;br /&gt;
&lt;br /&gt;
Bond length: 2.0417 Å&lt;br /&gt;
===Vibrational Analysis===&lt;br /&gt;
&amp;lt;pre&amp;gt;&lt;br /&gt;
 Item               Value     Threshold  Converged?&lt;br /&gt;
 Maximum Force            0.000043     0.000450     YES&lt;br /&gt;
 RMS     Force            0.000043     0.000300     YES&lt;br /&gt;
 Maximum Displacement     0.000121     0.001800     YES&lt;br /&gt;
 RMS     Displacement     0.000172     0.001200     YES&lt;br /&gt;
&lt;br /&gt;
&amp;lt;/pre&amp;gt;&lt;br /&gt;
&amp;lt;pre&amp;gt;&lt;br /&gt;
Vibrational mode    Frequency    Infrared&lt;br /&gt;
#1             520.32       0.0000&lt;br /&gt;
&amp;lt;/pre&amp;gt;&lt;br /&gt;
There are no vibrational modes with negative frequencies&lt;br /&gt;
===Charge Analysis===&lt;br /&gt;
[[File:Adrian_Popescu_Cl2_Charges.png|1000px|center]]&lt;br /&gt;
As the Cl&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; molecule is made up of identical Cl atoms, the bond between them will be 100% covalent, the electrons that form the sigma bond are equally shared between the cl atoms, so the charge on each Cl atom is zero.&lt;br /&gt;
&lt;br /&gt;
===Molecular orbitals Analysis===&lt;br /&gt;
[[File:Adrian_Popescu_orbital1.png|1000px|thumb|center|2σg bonding orbital]]&lt;br /&gt;
The 2σg bonding orbital is deep in energy, occupied, and corresponds to the bonding orbital formed by the 2s AOs of the Cl atoms.&lt;/div&gt;</summary>
		<author><name>Ap5817</name></author>
	</entry>
	<entry>
		<id>https://chemwiki.ch.ic.ac.uk/index.php?title=User:Ap5817&amp;diff=679162</id>
		<title>User:Ap5817</title>
		<link rel="alternate" type="text/html" href="https://chemwiki.ch.ic.ac.uk/index.php?title=User:Ap5817&amp;diff=679162"/>
		<updated>2018-03-07T14:40:46Z</updated>

		<summary type="html">&lt;p&gt;Ap5817: /* Molecular orbitals Analysis */&lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;== NH3 molecule ==&lt;br /&gt;
=== NH3 calculations ===&lt;br /&gt;
Calculation method:RB3LYP&lt;br /&gt;
&lt;br /&gt;
Basis Set = 6-31G(d,p)&lt;br /&gt;
&lt;br /&gt;
Final Energy: E(RB3LYP) = -56.557768 a.u.&lt;br /&gt;
&lt;br /&gt;
Bond length:1.01789 Å&lt;br /&gt;
&lt;br /&gt;
Bond angle: 105.741 °C&lt;br /&gt;
&lt;br /&gt;
Point Group: C3v&amp;lt;pre&amp;gt;&lt;br /&gt;
Item               Value     Threshold  Converged?&lt;br /&gt;
 Maximum Force            0.000004     0.000450     YES&lt;br /&gt;
 RMS     Force            0.000004     0.000300     YES&lt;br /&gt;
 Maximum Displacement     0.000072     0.001800     YES&lt;br /&gt;
 RMS     Displacement     0.000035     0.001200     YES&lt;br /&gt;
&amp;lt;/pre&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&amp;lt;jmol&amp;gt;&amp;lt;jmolApplet&amp;gt;&lt;br /&gt;
&amp;lt;script&amp;gt;frame x.y&amp;lt;/script&amp;gt;&lt;br /&gt;
  &amp;lt;title&amp;gt;test molecule&amp;lt;/title&amp;gt;&lt;br /&gt;
  &amp;lt;color&amp;gt;black&amp;lt;/color&amp;gt;&lt;br /&gt;
  &amp;lt;size&amp;gt;200&amp;lt;/size&amp;gt;&lt;br /&gt;
  &amp;lt;uploadedFileContents&amp;gt;ADRIAN_POPESCU_PHUNT_NH3_OPTF_POP.LOG&amp;lt;/uploadedFileContents&amp;gt;&lt;br /&gt;
&amp;lt;/jmolApplet&amp;gt;&amp;lt;/jmol&amp;gt;&lt;br /&gt;
&lt;br /&gt;
[[Media:ADRIAN_POPESCU_PHUNT_NH3_OPTF_POP.LOG]]&lt;br /&gt;
&lt;br /&gt;
==Vibration analysis of NH3==&lt;br /&gt;
[[File:Adrian_Popescu_Display_Vibrations.png|1000px]]&lt;br /&gt;
===Vibrational modes===&lt;br /&gt;
Number of vibrational modes: 6&lt;br /&gt;
&lt;br /&gt;
Number of degenerate modes: 4 (2 pairs of degenerate vibrational modes &lt;br /&gt;
&lt;br /&gt;
Number of bending motions: 3&lt;br /&gt;
&lt;br /&gt;
Number of stretching motions: 3&lt;br /&gt;
&lt;br /&gt;
The most symmetric vibrational mode: mode #4&lt;br /&gt;
&lt;br /&gt;
The &#039;&#039;umbrella mode&#039;&#039;: mode #1&lt;br /&gt;
&lt;br /&gt;
Number of bands expected to be seen in an experimental spectrum of gaseous ammonia: 5&lt;br /&gt;
===Charge Analysis===&lt;br /&gt;
[[File:Adrian_Popescu_Charges.png|1500px]]&lt;br /&gt;
&lt;br /&gt;
Charge on the N atom: -1.125&lt;br /&gt;
&lt;br /&gt;
Charge on the H atom: 0.375&lt;br /&gt;
&lt;br /&gt;
As Nitrogen has an electronegativity value of 3.04, which is significantly larger than the one of Hidrogen (2.2), it is expected that on the Nitrogen there will be a negative charge and on Hidrogen a possitive charge.&lt;br /&gt;
&lt;br /&gt;
==Reactivity of the Haber-Bosch process==&lt;br /&gt;
===Analysis of H2===&lt;br /&gt;
Calculation method:RB3LYP&lt;br /&gt;
&lt;br /&gt;
Basis Set = 6-31G(d,p)&lt;br /&gt;
&lt;br /&gt;
Final Energy: E(RB3LYP) = -1.1785393 a.u.&lt;br /&gt;
&lt;br /&gt;
Bond length:0.7428 Å&lt;br /&gt;
&amp;lt;pre&amp;gt;&lt;br /&gt;
Item               Value     Threshold  Converged?&lt;br /&gt;
 Maximum Force            0.000004     0.000450     YES&lt;br /&gt;
 RMS     Force            0.000004     0.000300     YES&lt;br /&gt;
 Maximum Displacement     0.000005     0.001800     YES&lt;br /&gt;
 RMS     Displacement     0.000007     0.001200     YES&amp;lt;/pre&amp;gt;&lt;br /&gt;
&amp;lt;pre&amp;gt;&lt;br /&gt;
Vibrational mode    Frequency    Infrared&lt;br /&gt;
#1             4465.6       0.0000&lt;br /&gt;
&amp;lt;/pre&amp;gt;&lt;br /&gt;
There are no vibrational modes with negative frequencies&lt;br /&gt;
===Analysis of N2===&lt;br /&gt;
Calculation method:RB3LYP&lt;br /&gt;
&lt;br /&gt;
Basis Set = 6-31G(d,p)&lt;br /&gt;
&lt;br /&gt;
Final Energy: E(RB3LYP) = -109.5241268 a.u.&lt;br /&gt;
&lt;br /&gt;
Bond length: 1.1055 Å&lt;br /&gt;
&amp;lt;pre&amp;gt;&lt;br /&gt;
Item               Value     Threshold  Converged?&lt;br /&gt;
 Maximum Force            0.000001     0.000450     YES&lt;br /&gt;
 RMS     Force            0.000001     0.000300     YES&lt;br /&gt;
 Maximum Displacement     0.000000     0.001800     YES&lt;br /&gt;
 RMS     Displacement     0.000000     0.001200     YES&lt;br /&gt;
&amp;lt;/pre&amp;gt;&lt;br /&gt;
&amp;lt;pre&amp;gt;&lt;br /&gt;
Vibrational mode    Frequency    Infrared&lt;br /&gt;
#1             2457.33       0.0000&lt;br /&gt;
&amp;lt;/pre&amp;gt;&lt;br /&gt;
There are no vibrational modes with negative frequencies&lt;br /&gt;
&lt;br /&gt;
===Calculation of the energy of the Haber-Bosch process===&lt;br /&gt;
N&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; + 3H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; -&amp;gt; 2NH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;&lt;br /&gt;
&lt;br /&gt;
E(NH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;)= -56.557768 a u&lt;br /&gt;
&lt;br /&gt;
2*E(NH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;)= -113.115536 a u&lt;br /&gt;
&lt;br /&gt;
E(N&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;)= -109.5251268 a u&lt;br /&gt;
&lt;br /&gt;
E(H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;)= -1.1785393 a u&lt;br /&gt;
&lt;br /&gt;
3*E(H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;)= -3.5359617 a u&lt;br /&gt;
&lt;br /&gt;
ΔE=2*E(NH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;) - [E(N&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;) + 3*E(H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;)] = -145.57 kj/mol&lt;br /&gt;
&lt;br /&gt;
As the reaction is exothermic, the ammonia product is more stable than the gaseous reactants.&lt;br /&gt;
==Analysis of Cl&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;==&lt;br /&gt;
===General Analysis===&lt;br /&gt;
Calculation method:RB3LYP&lt;br /&gt;
&lt;br /&gt;
Basis Set = 6-31G(d,p)&lt;br /&gt;
&lt;br /&gt;
Final Energy: E(RB3LYP) = -920.3498788 a.u.&lt;br /&gt;
&lt;br /&gt;
Bond length: 2.0417 Å&lt;br /&gt;
===Vibrational Analysis===&lt;br /&gt;
&amp;lt;pre&amp;gt;&lt;br /&gt;
 Item               Value     Threshold  Converged?&lt;br /&gt;
 Maximum Force            0.000043     0.000450     YES&lt;br /&gt;
 RMS     Force            0.000043     0.000300     YES&lt;br /&gt;
 Maximum Displacement     0.000121     0.001800     YES&lt;br /&gt;
 RMS     Displacement     0.000172     0.001200     YES&lt;br /&gt;
&lt;br /&gt;
&amp;lt;/pre&amp;gt;&lt;br /&gt;
&amp;lt;pre&amp;gt;&lt;br /&gt;
Vibrational mode    Frequency    Infrared&lt;br /&gt;
#1             520.32       0.0000&lt;br /&gt;
&amp;lt;/pre&amp;gt;&lt;br /&gt;
There are no vibrational modes with negative frequencies&lt;br /&gt;
===Charge Analysis===&lt;br /&gt;
[[File:Adrian_Popescu_Cl2_Charges.png|1000px]]&lt;br /&gt;
As the Cl&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; molecule is made up of identical Cl atoms, the bond between them will be 100% covalent, the electrons that form the sigma bond are equally shared between the cl atoms, so the charge on each Cl atom is zero.&lt;br /&gt;
===Molecular orbitals Analysis===&lt;br /&gt;
[[File:Adrian_Popescu_orbital1.png|1000px|thumb|center|2σg bonding orbital]]&lt;br /&gt;
The 2σg bonding orbital is deep in energy, occupied, and corresponds to the bonding orbital formed by the 2s AOs of the Cl atoms.&lt;/div&gt;</summary>
		<author><name>Ap5817</name></author>
	</entry>
	<entry>
		<id>https://chemwiki.ch.ic.ac.uk/index.php?title=User:Ap5817&amp;diff=679161</id>
		<title>User:Ap5817</title>
		<link rel="alternate" type="text/html" href="https://chemwiki.ch.ic.ac.uk/index.php?title=User:Ap5817&amp;diff=679161"/>
		<updated>2018-03-07T14:39:13Z</updated>

		<summary type="html">&lt;p&gt;Ap5817: /* Molecular orbitals Analysis */&lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;== NH3 molecule ==&lt;br /&gt;
=== NH3 calculations ===&lt;br /&gt;
Calculation method:RB3LYP&lt;br /&gt;
&lt;br /&gt;
Basis Set = 6-31G(d,p)&lt;br /&gt;
&lt;br /&gt;
Final Energy: E(RB3LYP) = -56.557768 a.u.&lt;br /&gt;
&lt;br /&gt;
Bond length:1.01789 Å&lt;br /&gt;
&lt;br /&gt;
Bond angle: 105.741 °C&lt;br /&gt;
&lt;br /&gt;
Point Group: C3v&amp;lt;pre&amp;gt;&lt;br /&gt;
Item               Value     Threshold  Converged?&lt;br /&gt;
 Maximum Force            0.000004     0.000450     YES&lt;br /&gt;
 RMS     Force            0.000004     0.000300     YES&lt;br /&gt;
 Maximum Displacement     0.000072     0.001800     YES&lt;br /&gt;
 RMS     Displacement     0.000035     0.001200     YES&lt;br /&gt;
&amp;lt;/pre&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&amp;lt;jmol&amp;gt;&amp;lt;jmolApplet&amp;gt;&lt;br /&gt;
&amp;lt;script&amp;gt;frame x.y&amp;lt;/script&amp;gt;&lt;br /&gt;
  &amp;lt;title&amp;gt;test molecule&amp;lt;/title&amp;gt;&lt;br /&gt;
  &amp;lt;color&amp;gt;black&amp;lt;/color&amp;gt;&lt;br /&gt;
  &amp;lt;size&amp;gt;200&amp;lt;/size&amp;gt;&lt;br /&gt;
  &amp;lt;uploadedFileContents&amp;gt;ADRIAN_POPESCU_PHUNT_NH3_OPTF_POP.LOG&amp;lt;/uploadedFileContents&amp;gt;&lt;br /&gt;
&amp;lt;/jmolApplet&amp;gt;&amp;lt;/jmol&amp;gt;&lt;br /&gt;
&lt;br /&gt;
[[Media:ADRIAN_POPESCU_PHUNT_NH3_OPTF_POP.LOG]]&lt;br /&gt;
&lt;br /&gt;
==Vibration analysis of NH3==&lt;br /&gt;
[[File:Adrian_Popescu_Display_Vibrations.png|1000px]]&lt;br /&gt;
===Vibrational modes===&lt;br /&gt;
Number of vibrational modes: 6&lt;br /&gt;
&lt;br /&gt;
Number of degenerate modes: 4 (2 pairs of degenerate vibrational modes &lt;br /&gt;
&lt;br /&gt;
Number of bending motions: 3&lt;br /&gt;
&lt;br /&gt;
Number of stretching motions: 3&lt;br /&gt;
&lt;br /&gt;
The most symmetric vibrational mode: mode #4&lt;br /&gt;
&lt;br /&gt;
The &#039;&#039;umbrella mode&#039;&#039;: mode #1&lt;br /&gt;
&lt;br /&gt;
Number of bands expected to be seen in an experimental spectrum of gaseous ammonia: 5&lt;br /&gt;
===Charge Analysis===&lt;br /&gt;
[[File:Adrian_Popescu_Charges.png|1500px]]&lt;br /&gt;
&lt;br /&gt;
Charge on the N atom: -1.125&lt;br /&gt;
&lt;br /&gt;
Charge on the H atom: 0.375&lt;br /&gt;
&lt;br /&gt;
As Nitrogen has an electronegativity value of 3.04, which is significantly larger than the one of Hidrogen (2.2), it is expected that on the Nitrogen there will be a negative charge and on Hidrogen a possitive charge.&lt;br /&gt;
&lt;br /&gt;
==Reactivity of the Haber-Bosch process==&lt;br /&gt;
===Analysis of H2===&lt;br /&gt;
Calculation method:RB3LYP&lt;br /&gt;
&lt;br /&gt;
Basis Set = 6-31G(d,p)&lt;br /&gt;
&lt;br /&gt;
Final Energy: E(RB3LYP) = -1.1785393 a.u.&lt;br /&gt;
&lt;br /&gt;
Bond length:0.7428 Å&lt;br /&gt;
&amp;lt;pre&amp;gt;&lt;br /&gt;
Item               Value     Threshold  Converged?&lt;br /&gt;
 Maximum Force            0.000004     0.000450     YES&lt;br /&gt;
 RMS     Force            0.000004     0.000300     YES&lt;br /&gt;
 Maximum Displacement     0.000005     0.001800     YES&lt;br /&gt;
 RMS     Displacement     0.000007     0.001200     YES&amp;lt;/pre&amp;gt;&lt;br /&gt;
&amp;lt;pre&amp;gt;&lt;br /&gt;
Vibrational mode    Frequency    Infrared&lt;br /&gt;
#1             4465.6       0.0000&lt;br /&gt;
&amp;lt;/pre&amp;gt;&lt;br /&gt;
There are no vibrational modes with negative frequencies&lt;br /&gt;
===Analysis of N2===&lt;br /&gt;
Calculation method:RB3LYP&lt;br /&gt;
&lt;br /&gt;
Basis Set = 6-31G(d,p)&lt;br /&gt;
&lt;br /&gt;
Final Energy: E(RB3LYP) = -109.5241268 a.u.&lt;br /&gt;
&lt;br /&gt;
Bond length: 1.1055 Å&lt;br /&gt;
&amp;lt;pre&amp;gt;&lt;br /&gt;
Item               Value     Threshold  Converged?&lt;br /&gt;
 Maximum Force            0.000001     0.000450     YES&lt;br /&gt;
 RMS     Force            0.000001     0.000300     YES&lt;br /&gt;
 Maximum Displacement     0.000000     0.001800     YES&lt;br /&gt;
 RMS     Displacement     0.000000     0.001200     YES&lt;br /&gt;
&amp;lt;/pre&amp;gt;&lt;br /&gt;
&amp;lt;pre&amp;gt;&lt;br /&gt;
Vibrational mode    Frequency    Infrared&lt;br /&gt;
#1             2457.33       0.0000&lt;br /&gt;
&amp;lt;/pre&amp;gt;&lt;br /&gt;
There are no vibrational modes with negative frequencies&lt;br /&gt;
&lt;br /&gt;
===Calculation of the energy of the Haber-Bosch process===&lt;br /&gt;
N&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; + 3H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; -&amp;gt; 2NH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;&lt;br /&gt;
&lt;br /&gt;
E(NH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;)= -56.557768 a u&lt;br /&gt;
&lt;br /&gt;
2*E(NH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;)= -113.115536 a u&lt;br /&gt;
&lt;br /&gt;
E(N&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;)= -109.5251268 a u&lt;br /&gt;
&lt;br /&gt;
E(H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;)= -1.1785393 a u&lt;br /&gt;
&lt;br /&gt;
3*E(H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;)= -3.5359617 a u&lt;br /&gt;
&lt;br /&gt;
ΔE=2*E(NH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;) - [E(N&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;) + 3*E(H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;)] = -145.57 kj/mol&lt;br /&gt;
&lt;br /&gt;
As the reaction is exothermic, the ammonia product is more stable than the gaseous reactants.&lt;br /&gt;
==Analysis of Cl&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;==&lt;br /&gt;
===General Analysis===&lt;br /&gt;
Calculation method:RB3LYP&lt;br /&gt;
&lt;br /&gt;
Basis Set = 6-31G(d,p)&lt;br /&gt;
&lt;br /&gt;
Final Energy: E(RB3LYP) = -920.3498788 a.u.&lt;br /&gt;
&lt;br /&gt;
Bond length: 2.0417 Å&lt;br /&gt;
===Vibrational Analysis===&lt;br /&gt;
&amp;lt;pre&amp;gt;&lt;br /&gt;
 Item               Value     Threshold  Converged?&lt;br /&gt;
 Maximum Force            0.000043     0.000450     YES&lt;br /&gt;
 RMS     Force            0.000043     0.000300     YES&lt;br /&gt;
 Maximum Displacement     0.000121     0.001800     YES&lt;br /&gt;
 RMS     Displacement     0.000172     0.001200     YES&lt;br /&gt;
&lt;br /&gt;
&amp;lt;/pre&amp;gt;&lt;br /&gt;
&amp;lt;pre&amp;gt;&lt;br /&gt;
Vibrational mode    Frequency    Infrared&lt;br /&gt;
#1             520.32       0.0000&lt;br /&gt;
&amp;lt;/pre&amp;gt;&lt;br /&gt;
There are no vibrational modes with negative frequencies&lt;br /&gt;
===Charge Analysis===&lt;br /&gt;
[[File:Adrian_Popescu_Cl2_Charges.png|1000px]]&lt;br /&gt;
As the Cl&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; molecule is made up of identical Cl atoms, the bond between them will be 100% covalent, the electrons that form the sigma bond are equally shared between the cl atoms, so the charge on each Cl atom is zero.&lt;br /&gt;
===Molecular orbitals Analysis===&lt;br /&gt;
[[File:Adrian_Popescu_orbital1.png|1000px|thumb|2σg bonding orbital]]&lt;br /&gt;
The 2σg bonding orbital is deep in energy, occupied, and corresponds to the bonding orbital formed by the 2s AOs of the Cl atoms.&lt;/div&gt;</summary>
		<author><name>Ap5817</name></author>
	</entry>
	<entry>
		<id>https://chemwiki.ch.ic.ac.uk/index.php?title=User:Ap5817&amp;diff=679139</id>
		<title>User:Ap5817</title>
		<link rel="alternate" type="text/html" href="https://chemwiki.ch.ic.ac.uk/index.php?title=User:Ap5817&amp;diff=679139"/>
		<updated>2018-03-07T14:30:34Z</updated>

		<summary type="html">&lt;p&gt;Ap5817: /* Molecular orbitals Analysis */&lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;== NH3 molecule ==&lt;br /&gt;
=== NH3 calculations ===&lt;br /&gt;
Calculation method:RB3LYP&lt;br /&gt;
&lt;br /&gt;
Basis Set = 6-31G(d,p)&lt;br /&gt;
&lt;br /&gt;
Final Energy: E(RB3LYP) = -56.557768 a.u.&lt;br /&gt;
&lt;br /&gt;
Bond length:1.01789 Å&lt;br /&gt;
&lt;br /&gt;
Bond angle: 105.741 °C&lt;br /&gt;
&lt;br /&gt;
Point Group: C3v&amp;lt;pre&amp;gt;&lt;br /&gt;
Item               Value     Threshold  Converged?&lt;br /&gt;
 Maximum Force            0.000004     0.000450     YES&lt;br /&gt;
 RMS     Force            0.000004     0.000300     YES&lt;br /&gt;
 Maximum Displacement     0.000072     0.001800     YES&lt;br /&gt;
 RMS     Displacement     0.000035     0.001200     YES&lt;br /&gt;
&amp;lt;/pre&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&amp;lt;jmol&amp;gt;&amp;lt;jmolApplet&amp;gt;&lt;br /&gt;
&amp;lt;script&amp;gt;frame x.y&amp;lt;/script&amp;gt;&lt;br /&gt;
  &amp;lt;title&amp;gt;test molecule&amp;lt;/title&amp;gt;&lt;br /&gt;
  &amp;lt;color&amp;gt;black&amp;lt;/color&amp;gt;&lt;br /&gt;
  &amp;lt;size&amp;gt;200&amp;lt;/size&amp;gt;&lt;br /&gt;
  &amp;lt;uploadedFileContents&amp;gt;ADRIAN_POPESCU_PHUNT_NH3_OPTF_POP.LOG&amp;lt;/uploadedFileContents&amp;gt;&lt;br /&gt;
&amp;lt;/jmolApplet&amp;gt;&amp;lt;/jmol&amp;gt;&lt;br /&gt;
&lt;br /&gt;
[[Media:ADRIAN_POPESCU_PHUNT_NH3_OPTF_POP.LOG]]&lt;br /&gt;
&lt;br /&gt;
==Vibration analysis of NH3==&lt;br /&gt;
[[File:Adrian_Popescu_Display_Vibrations.png|1000px]]&lt;br /&gt;
===Vibrational modes===&lt;br /&gt;
Number of vibrational modes: 6&lt;br /&gt;
&lt;br /&gt;
Number of degenerate modes: 4 (2 pairs of degenerate vibrational modes &lt;br /&gt;
&lt;br /&gt;
Number of bending motions: 3&lt;br /&gt;
&lt;br /&gt;
Number of stretching motions: 3&lt;br /&gt;
&lt;br /&gt;
The most symmetric vibrational mode: mode #4&lt;br /&gt;
&lt;br /&gt;
The &#039;&#039;umbrella mode&#039;&#039;: mode #1&lt;br /&gt;
&lt;br /&gt;
Number of bands expected to be seen in an experimental spectrum of gaseous ammonia: 5&lt;br /&gt;
===Charge Analysis===&lt;br /&gt;
[[File:Adrian_Popescu_Charges.png|1500px]]&lt;br /&gt;
&lt;br /&gt;
Charge on the N atom: -1.125&lt;br /&gt;
&lt;br /&gt;
Charge on the H atom: 0.375&lt;br /&gt;
&lt;br /&gt;
As Nitrogen has an electronegativity value of 3.04, which is significantly larger than the one of Hidrogen (2.2), it is expected that on the Nitrogen there will be a negative charge and on Hidrogen a possitive charge.&lt;br /&gt;
&lt;br /&gt;
==Reactivity of the Haber-Bosch process==&lt;br /&gt;
===Analysis of H2===&lt;br /&gt;
Calculation method:RB3LYP&lt;br /&gt;
&lt;br /&gt;
Basis Set = 6-31G(d,p)&lt;br /&gt;
&lt;br /&gt;
Final Energy: E(RB3LYP) = -1.1785393 a.u.&lt;br /&gt;
&lt;br /&gt;
Bond length:0.7428 Å&lt;br /&gt;
&amp;lt;pre&amp;gt;&lt;br /&gt;
Item               Value     Threshold  Converged?&lt;br /&gt;
 Maximum Force            0.000004     0.000450     YES&lt;br /&gt;
 RMS     Force            0.000004     0.000300     YES&lt;br /&gt;
 Maximum Displacement     0.000005     0.001800     YES&lt;br /&gt;
 RMS     Displacement     0.000007     0.001200     YES&amp;lt;/pre&amp;gt;&lt;br /&gt;
&amp;lt;pre&amp;gt;&lt;br /&gt;
Vibrational mode    Frequency    Infrared&lt;br /&gt;
#1             4465.6       0.0000&lt;br /&gt;
&amp;lt;/pre&amp;gt;&lt;br /&gt;
There are no vibrational modes with negative frequencies&lt;br /&gt;
===Analysis of N2===&lt;br /&gt;
Calculation method:RB3LYP&lt;br /&gt;
&lt;br /&gt;
Basis Set = 6-31G(d,p)&lt;br /&gt;
&lt;br /&gt;
Final Energy: E(RB3LYP) = -109.5241268 a.u.&lt;br /&gt;
&lt;br /&gt;
Bond length: 1.1055 Å&lt;br /&gt;
&amp;lt;pre&amp;gt;&lt;br /&gt;
Item               Value     Threshold  Converged?&lt;br /&gt;
 Maximum Force            0.000001     0.000450     YES&lt;br /&gt;
 RMS     Force            0.000001     0.000300     YES&lt;br /&gt;
 Maximum Displacement     0.000000     0.001800     YES&lt;br /&gt;
 RMS     Displacement     0.000000     0.001200     YES&lt;br /&gt;
&amp;lt;/pre&amp;gt;&lt;br /&gt;
&amp;lt;pre&amp;gt;&lt;br /&gt;
Vibrational mode    Frequency    Infrared&lt;br /&gt;
#1             2457.33       0.0000&lt;br /&gt;
&amp;lt;/pre&amp;gt;&lt;br /&gt;
There are no vibrational modes with negative frequencies&lt;br /&gt;
&lt;br /&gt;
===Calculation of the energy of the Haber-Bosch process===&lt;br /&gt;
N&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; + 3H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; -&amp;gt; 2NH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;&lt;br /&gt;
&lt;br /&gt;
E(NH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;)= -56.557768 a u&lt;br /&gt;
&lt;br /&gt;
2*E(NH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;)= -113.115536 a u&lt;br /&gt;
&lt;br /&gt;
E(N&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;)= -109.5251268 a u&lt;br /&gt;
&lt;br /&gt;
E(H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;)= -1.1785393 a u&lt;br /&gt;
&lt;br /&gt;
3*E(H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;)= -3.5359617 a u&lt;br /&gt;
&lt;br /&gt;
ΔE=2*E(NH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;) - [E(N&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;) + 3*E(H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;)] = -145.57 kj/mol&lt;br /&gt;
&lt;br /&gt;
As the reaction is exothermic, the ammonia product is more stable than the gaseous reactants.&lt;br /&gt;
==Analysis of Cl&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;==&lt;br /&gt;
===General Analysis===&lt;br /&gt;
Calculation method:RB3LYP&lt;br /&gt;
&lt;br /&gt;
Basis Set = 6-31G(d,p)&lt;br /&gt;
&lt;br /&gt;
Final Energy: E(RB3LYP) = -920.3498788 a.u.&lt;br /&gt;
&lt;br /&gt;
Bond length: 2.0417 Å&lt;br /&gt;
===Vibrational Analysis===&lt;br /&gt;
&amp;lt;pre&amp;gt;&lt;br /&gt;
 Item               Value     Threshold  Converged?&lt;br /&gt;
 Maximum Force            0.000043     0.000450     YES&lt;br /&gt;
 RMS     Force            0.000043     0.000300     YES&lt;br /&gt;
 Maximum Displacement     0.000121     0.001800     YES&lt;br /&gt;
 RMS     Displacement     0.000172     0.001200     YES&lt;br /&gt;
&lt;br /&gt;
&amp;lt;/pre&amp;gt;&lt;br /&gt;
&amp;lt;pre&amp;gt;&lt;br /&gt;
Vibrational mode    Frequency    Infrared&lt;br /&gt;
#1             520.32       0.0000&lt;br /&gt;
&amp;lt;/pre&amp;gt;&lt;br /&gt;
There are no vibrational modes with negative frequencies&lt;br /&gt;
===Charge Analysis===&lt;br /&gt;
[[File:Adrian_Popescu_Cl2_Charges.png|1000px]]&lt;br /&gt;
As the Cl&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; molecule is made up of identical Cl atoms, the bond between them will be 100% covalent, the electrons that form the sigma bond are equally shared between the cl atoms, so the charge on each Cl atom is zero.&lt;br /&gt;
===Molecular orbitals Analysis===&lt;br /&gt;
[[File:Adrian_Popescu_orbital1.png|1000px]]&lt;/div&gt;</summary>
		<author><name>Ap5817</name></author>
	</entry>
	<entry>
		<id>https://chemwiki.ch.ic.ac.uk/index.php?title=User:Ap5817&amp;diff=679138</id>
		<title>User:Ap5817</title>
		<link rel="alternate" type="text/html" href="https://chemwiki.ch.ic.ac.uk/index.php?title=User:Ap5817&amp;diff=679138"/>
		<updated>2018-03-07T14:30:23Z</updated>

		<summary type="html">&lt;p&gt;Ap5817: /* Molecular orbitals Analysis */&lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;== NH3 molecule ==&lt;br /&gt;
=== NH3 calculations ===&lt;br /&gt;
Calculation method:RB3LYP&lt;br /&gt;
&lt;br /&gt;
Basis Set = 6-31G(d,p)&lt;br /&gt;
&lt;br /&gt;
Final Energy: E(RB3LYP) = -56.557768 a.u.&lt;br /&gt;
&lt;br /&gt;
Bond length:1.01789 Å&lt;br /&gt;
&lt;br /&gt;
Bond angle: 105.741 °C&lt;br /&gt;
&lt;br /&gt;
Point Group: C3v&amp;lt;pre&amp;gt;&lt;br /&gt;
Item               Value     Threshold  Converged?&lt;br /&gt;
 Maximum Force            0.000004     0.000450     YES&lt;br /&gt;
 RMS     Force            0.000004     0.000300     YES&lt;br /&gt;
 Maximum Displacement     0.000072     0.001800     YES&lt;br /&gt;
 RMS     Displacement     0.000035     0.001200     YES&lt;br /&gt;
&amp;lt;/pre&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&amp;lt;jmol&amp;gt;&amp;lt;jmolApplet&amp;gt;&lt;br /&gt;
&amp;lt;script&amp;gt;frame x.y&amp;lt;/script&amp;gt;&lt;br /&gt;
  &amp;lt;title&amp;gt;test molecule&amp;lt;/title&amp;gt;&lt;br /&gt;
  &amp;lt;color&amp;gt;black&amp;lt;/color&amp;gt;&lt;br /&gt;
  &amp;lt;size&amp;gt;200&amp;lt;/size&amp;gt;&lt;br /&gt;
  &amp;lt;uploadedFileContents&amp;gt;ADRIAN_POPESCU_PHUNT_NH3_OPTF_POP.LOG&amp;lt;/uploadedFileContents&amp;gt;&lt;br /&gt;
&amp;lt;/jmolApplet&amp;gt;&amp;lt;/jmol&amp;gt;&lt;br /&gt;
&lt;br /&gt;
[[Media:ADRIAN_POPESCU_PHUNT_NH3_OPTF_POP.LOG]]&lt;br /&gt;
&lt;br /&gt;
==Vibration analysis of NH3==&lt;br /&gt;
[[File:Adrian_Popescu_Display_Vibrations.png|1000px]]&lt;br /&gt;
===Vibrational modes===&lt;br /&gt;
Number of vibrational modes: 6&lt;br /&gt;
&lt;br /&gt;
Number of degenerate modes: 4 (2 pairs of degenerate vibrational modes &lt;br /&gt;
&lt;br /&gt;
Number of bending motions: 3&lt;br /&gt;
&lt;br /&gt;
Number of stretching motions: 3&lt;br /&gt;
&lt;br /&gt;
The most symmetric vibrational mode: mode #4&lt;br /&gt;
&lt;br /&gt;
The &#039;&#039;umbrella mode&#039;&#039;: mode #1&lt;br /&gt;
&lt;br /&gt;
Number of bands expected to be seen in an experimental spectrum of gaseous ammonia: 5&lt;br /&gt;
===Charge Analysis===&lt;br /&gt;
[[File:Adrian_Popescu_Charges.png|1500px]]&lt;br /&gt;
&lt;br /&gt;
Charge on the N atom: -1.125&lt;br /&gt;
&lt;br /&gt;
Charge on the H atom: 0.375&lt;br /&gt;
&lt;br /&gt;
As Nitrogen has an electronegativity value of 3.04, which is significantly larger than the one of Hidrogen (2.2), it is expected that on the Nitrogen there will be a negative charge and on Hidrogen a possitive charge.&lt;br /&gt;
&lt;br /&gt;
==Reactivity of the Haber-Bosch process==&lt;br /&gt;
===Analysis of H2===&lt;br /&gt;
Calculation method:RB3LYP&lt;br /&gt;
&lt;br /&gt;
Basis Set = 6-31G(d,p)&lt;br /&gt;
&lt;br /&gt;
Final Energy: E(RB3LYP) = -1.1785393 a.u.&lt;br /&gt;
&lt;br /&gt;
Bond length:0.7428 Å&lt;br /&gt;
&amp;lt;pre&amp;gt;&lt;br /&gt;
Item               Value     Threshold  Converged?&lt;br /&gt;
 Maximum Force            0.000004     0.000450     YES&lt;br /&gt;
 RMS     Force            0.000004     0.000300     YES&lt;br /&gt;
 Maximum Displacement     0.000005     0.001800     YES&lt;br /&gt;
 RMS     Displacement     0.000007     0.001200     YES&amp;lt;/pre&amp;gt;&lt;br /&gt;
&amp;lt;pre&amp;gt;&lt;br /&gt;
Vibrational mode    Frequency    Infrared&lt;br /&gt;
#1             4465.6       0.0000&lt;br /&gt;
&amp;lt;/pre&amp;gt;&lt;br /&gt;
There are no vibrational modes with negative frequencies&lt;br /&gt;
===Analysis of N2===&lt;br /&gt;
Calculation method:RB3LYP&lt;br /&gt;
&lt;br /&gt;
Basis Set = 6-31G(d,p)&lt;br /&gt;
&lt;br /&gt;
Final Energy: E(RB3LYP) = -109.5241268 a.u.&lt;br /&gt;
&lt;br /&gt;
Bond length: 1.1055 Å&lt;br /&gt;
&amp;lt;pre&amp;gt;&lt;br /&gt;
Item               Value     Threshold  Converged?&lt;br /&gt;
 Maximum Force            0.000001     0.000450     YES&lt;br /&gt;
 RMS     Force            0.000001     0.000300     YES&lt;br /&gt;
 Maximum Displacement     0.000000     0.001800     YES&lt;br /&gt;
 RMS     Displacement     0.000000     0.001200     YES&lt;br /&gt;
&amp;lt;/pre&amp;gt;&lt;br /&gt;
&amp;lt;pre&amp;gt;&lt;br /&gt;
Vibrational mode    Frequency    Infrared&lt;br /&gt;
#1             2457.33       0.0000&lt;br /&gt;
&amp;lt;/pre&amp;gt;&lt;br /&gt;
There are no vibrational modes with negative frequencies&lt;br /&gt;
&lt;br /&gt;
===Calculation of the energy of the Haber-Bosch process===&lt;br /&gt;
N&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; + 3H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; -&amp;gt; 2NH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;&lt;br /&gt;
&lt;br /&gt;
E(NH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;)= -56.557768 a u&lt;br /&gt;
&lt;br /&gt;
2*E(NH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;)= -113.115536 a u&lt;br /&gt;
&lt;br /&gt;
E(N&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;)= -109.5251268 a u&lt;br /&gt;
&lt;br /&gt;
E(H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;)= -1.1785393 a u&lt;br /&gt;
&lt;br /&gt;
3*E(H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;)= -3.5359617 a u&lt;br /&gt;
&lt;br /&gt;
ΔE=2*E(NH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;) - [E(N&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;) + 3*E(H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;)] = -145.57 kj/mol&lt;br /&gt;
&lt;br /&gt;
As the reaction is exothermic, the ammonia product is more stable than the gaseous reactants.&lt;br /&gt;
==Analysis of Cl&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;==&lt;br /&gt;
===General Analysis===&lt;br /&gt;
Calculation method:RB3LYP&lt;br /&gt;
&lt;br /&gt;
Basis Set = 6-31G(d,p)&lt;br /&gt;
&lt;br /&gt;
Final Energy: E(RB3LYP) = -920.3498788 a.u.&lt;br /&gt;
&lt;br /&gt;
Bond length: 2.0417 Å&lt;br /&gt;
===Vibrational Analysis===&lt;br /&gt;
&amp;lt;pre&amp;gt;&lt;br /&gt;
 Item               Value     Threshold  Converged?&lt;br /&gt;
 Maximum Force            0.000043     0.000450     YES&lt;br /&gt;
 RMS     Force            0.000043     0.000300     YES&lt;br /&gt;
 Maximum Displacement     0.000121     0.001800     YES&lt;br /&gt;
 RMS     Displacement     0.000172     0.001200     YES&lt;br /&gt;
&lt;br /&gt;
&amp;lt;/pre&amp;gt;&lt;br /&gt;
&amp;lt;pre&amp;gt;&lt;br /&gt;
Vibrational mode    Frequency    Infrared&lt;br /&gt;
#1             520.32       0.0000&lt;br /&gt;
&amp;lt;/pre&amp;gt;&lt;br /&gt;
There are no vibrational modes with negative frequencies&lt;br /&gt;
===Charge Analysis===&lt;br /&gt;
[[File:Adrian_Popescu_Cl2_Charges.png|1000px]]&lt;br /&gt;
As the Cl&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; molecule is made up of identical Cl atoms, the bond between them will be 100% covalent, the electrons that form the sigma bond are equally shared between the cl atoms, so the charge on each Cl atom is zero.&lt;br /&gt;
===Molecular orbitals Analysis===&lt;br /&gt;
[[File:Adrian_Popescu_orbital1.png|150px]]&lt;/div&gt;</summary>
		<author><name>Ap5817</name></author>
	</entry>
	<entry>
		<id>https://chemwiki.ch.ic.ac.uk/index.php?title=User:Ap5817&amp;diff=679136</id>
		<title>User:Ap5817</title>
		<link rel="alternate" type="text/html" href="https://chemwiki.ch.ic.ac.uk/index.php?title=User:Ap5817&amp;diff=679136"/>
		<updated>2018-03-07T14:30:12Z</updated>

		<summary type="html">&lt;p&gt;Ap5817: &lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;== NH3 molecule ==&lt;br /&gt;
=== NH3 calculations ===&lt;br /&gt;
Calculation method:RB3LYP&lt;br /&gt;
&lt;br /&gt;
Basis Set = 6-31G(d,p)&lt;br /&gt;
&lt;br /&gt;
Final Energy: E(RB3LYP) = -56.557768 a.u.&lt;br /&gt;
&lt;br /&gt;
Bond length:1.01789 Å&lt;br /&gt;
&lt;br /&gt;
Bond angle: 105.741 °C&lt;br /&gt;
&lt;br /&gt;
Point Group: C3v&amp;lt;pre&amp;gt;&lt;br /&gt;
Item               Value     Threshold  Converged?&lt;br /&gt;
 Maximum Force            0.000004     0.000450     YES&lt;br /&gt;
 RMS     Force            0.000004     0.000300     YES&lt;br /&gt;
 Maximum Displacement     0.000072     0.001800     YES&lt;br /&gt;
 RMS     Displacement     0.000035     0.001200     YES&lt;br /&gt;
&amp;lt;/pre&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&amp;lt;jmol&amp;gt;&amp;lt;jmolApplet&amp;gt;&lt;br /&gt;
&amp;lt;script&amp;gt;frame x.y&amp;lt;/script&amp;gt;&lt;br /&gt;
  &amp;lt;title&amp;gt;test molecule&amp;lt;/title&amp;gt;&lt;br /&gt;
  &amp;lt;color&amp;gt;black&amp;lt;/color&amp;gt;&lt;br /&gt;
  &amp;lt;size&amp;gt;200&amp;lt;/size&amp;gt;&lt;br /&gt;
  &amp;lt;uploadedFileContents&amp;gt;ADRIAN_POPESCU_PHUNT_NH3_OPTF_POP.LOG&amp;lt;/uploadedFileContents&amp;gt;&lt;br /&gt;
&amp;lt;/jmolApplet&amp;gt;&amp;lt;/jmol&amp;gt;&lt;br /&gt;
&lt;br /&gt;
[[Media:ADRIAN_POPESCU_PHUNT_NH3_OPTF_POP.LOG]]&lt;br /&gt;
&lt;br /&gt;
==Vibration analysis of NH3==&lt;br /&gt;
[[File:Adrian_Popescu_Display_Vibrations.png|1000px]]&lt;br /&gt;
===Vibrational modes===&lt;br /&gt;
Number of vibrational modes: 6&lt;br /&gt;
&lt;br /&gt;
Number of degenerate modes: 4 (2 pairs of degenerate vibrational modes &lt;br /&gt;
&lt;br /&gt;
Number of bending motions: 3&lt;br /&gt;
&lt;br /&gt;
Number of stretching motions: 3&lt;br /&gt;
&lt;br /&gt;
The most symmetric vibrational mode: mode #4&lt;br /&gt;
&lt;br /&gt;
The &#039;&#039;umbrella mode&#039;&#039;: mode #1&lt;br /&gt;
&lt;br /&gt;
Number of bands expected to be seen in an experimental spectrum of gaseous ammonia: 5&lt;br /&gt;
===Charge Analysis===&lt;br /&gt;
[[File:Adrian_Popescu_Charges.png|1500px]]&lt;br /&gt;
&lt;br /&gt;
Charge on the N atom: -1.125&lt;br /&gt;
&lt;br /&gt;
Charge on the H atom: 0.375&lt;br /&gt;
&lt;br /&gt;
As Nitrogen has an electronegativity value of 3.04, which is significantly larger than the one of Hidrogen (2.2), it is expected that on the Nitrogen there will be a negative charge and on Hidrogen a possitive charge.&lt;br /&gt;
&lt;br /&gt;
==Reactivity of the Haber-Bosch process==&lt;br /&gt;
===Analysis of H2===&lt;br /&gt;
Calculation method:RB3LYP&lt;br /&gt;
&lt;br /&gt;
Basis Set = 6-31G(d,p)&lt;br /&gt;
&lt;br /&gt;
Final Energy: E(RB3LYP) = -1.1785393 a.u.&lt;br /&gt;
&lt;br /&gt;
Bond length:0.7428 Å&lt;br /&gt;
&amp;lt;pre&amp;gt;&lt;br /&gt;
Item               Value     Threshold  Converged?&lt;br /&gt;
 Maximum Force            0.000004     0.000450     YES&lt;br /&gt;
 RMS     Force            0.000004     0.000300     YES&lt;br /&gt;
 Maximum Displacement     0.000005     0.001800     YES&lt;br /&gt;
 RMS     Displacement     0.000007     0.001200     YES&amp;lt;/pre&amp;gt;&lt;br /&gt;
&amp;lt;pre&amp;gt;&lt;br /&gt;
Vibrational mode    Frequency    Infrared&lt;br /&gt;
#1             4465.6       0.0000&lt;br /&gt;
&amp;lt;/pre&amp;gt;&lt;br /&gt;
There are no vibrational modes with negative frequencies&lt;br /&gt;
===Analysis of N2===&lt;br /&gt;
Calculation method:RB3LYP&lt;br /&gt;
&lt;br /&gt;
Basis Set = 6-31G(d,p)&lt;br /&gt;
&lt;br /&gt;
Final Energy: E(RB3LYP) = -109.5241268 a.u.&lt;br /&gt;
&lt;br /&gt;
Bond length: 1.1055 Å&lt;br /&gt;
&amp;lt;pre&amp;gt;&lt;br /&gt;
Item               Value     Threshold  Converged?&lt;br /&gt;
 Maximum Force            0.000001     0.000450     YES&lt;br /&gt;
 RMS     Force            0.000001     0.000300     YES&lt;br /&gt;
 Maximum Displacement     0.000000     0.001800     YES&lt;br /&gt;
 RMS     Displacement     0.000000     0.001200     YES&lt;br /&gt;
&amp;lt;/pre&amp;gt;&lt;br /&gt;
&amp;lt;pre&amp;gt;&lt;br /&gt;
Vibrational mode    Frequency    Infrared&lt;br /&gt;
#1             2457.33       0.0000&lt;br /&gt;
&amp;lt;/pre&amp;gt;&lt;br /&gt;
There are no vibrational modes with negative frequencies&lt;br /&gt;
&lt;br /&gt;
===Calculation of the energy of the Haber-Bosch process===&lt;br /&gt;
N&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; + 3H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; -&amp;gt; 2NH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;&lt;br /&gt;
&lt;br /&gt;
E(NH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;)= -56.557768 a u&lt;br /&gt;
&lt;br /&gt;
2*E(NH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;)= -113.115536 a u&lt;br /&gt;
&lt;br /&gt;
E(N&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;)= -109.5251268 a u&lt;br /&gt;
&lt;br /&gt;
E(H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;)= -1.1785393 a u&lt;br /&gt;
&lt;br /&gt;
3*E(H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;)= -3.5359617 a u&lt;br /&gt;
&lt;br /&gt;
ΔE=2*E(NH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;) - [E(N&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;) + 3*E(H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;)] = -145.57 kj/mol&lt;br /&gt;
&lt;br /&gt;
As the reaction is exothermic, the ammonia product is more stable than the gaseous reactants.&lt;br /&gt;
==Analysis of Cl&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;==&lt;br /&gt;
===General Analysis===&lt;br /&gt;
Calculation method:RB3LYP&lt;br /&gt;
&lt;br /&gt;
Basis Set = 6-31G(d,p)&lt;br /&gt;
&lt;br /&gt;
Final Energy: E(RB3LYP) = -920.3498788 a.u.&lt;br /&gt;
&lt;br /&gt;
Bond length: 2.0417 Å&lt;br /&gt;
===Vibrational Analysis===&lt;br /&gt;
&amp;lt;pre&amp;gt;&lt;br /&gt;
 Item               Value     Threshold  Converged?&lt;br /&gt;
 Maximum Force            0.000043     0.000450     YES&lt;br /&gt;
 RMS     Force            0.000043     0.000300     YES&lt;br /&gt;
 Maximum Displacement     0.000121     0.001800     YES&lt;br /&gt;
 RMS     Displacement     0.000172     0.001200     YES&lt;br /&gt;
&lt;br /&gt;
&amp;lt;/pre&amp;gt;&lt;br /&gt;
&amp;lt;pre&amp;gt;&lt;br /&gt;
Vibrational mode    Frequency    Infrared&lt;br /&gt;
#1             520.32       0.0000&lt;br /&gt;
&amp;lt;/pre&amp;gt;&lt;br /&gt;
There are no vibrational modes with negative frequencies&lt;br /&gt;
===Charge Analysis===&lt;br /&gt;
[[File:Adrian_Popescu_Cl2_Charges.png|1000px]]&lt;br /&gt;
As the Cl&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; molecule is made up of identical Cl atoms, the bond between them will be 100% covalent, the electrons that form the sigma bond are equally shared between the cl atoms, so the charge on each Cl atom is zero.&lt;br /&gt;
===Molecular orbitals Analysis===&lt;br /&gt;
[[File:Adrian_Popescu_orbital1.png|1500px]]&lt;/div&gt;</summary>
		<author><name>Ap5817</name></author>
	</entry>
	<entry>
		<id>https://chemwiki.ch.ic.ac.uk/index.php?title=File:Adrian_Popescu_orbital1.png&amp;diff=679132</id>
		<title>File:Adrian Popescu orbital1.png</title>
		<link rel="alternate" type="text/html" href="https://chemwiki.ch.ic.ac.uk/index.php?title=File:Adrian_Popescu_orbital1.png&amp;diff=679132"/>
		<updated>2018-03-07T14:29:05Z</updated>

		<summary type="html">&lt;p&gt;Ap5817: &lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;&lt;/div&gt;</summary>
		<author><name>Ap5817</name></author>
	</entry>
	<entry>
		<id>https://chemwiki.ch.ic.ac.uk/index.php?title=User:Ap5817&amp;diff=679020</id>
		<title>User:Ap5817</title>
		<link rel="alternate" type="text/html" href="https://chemwiki.ch.ic.ac.uk/index.php?title=User:Ap5817&amp;diff=679020"/>
		<updated>2018-03-07T13:41:10Z</updated>

		<summary type="html">&lt;p&gt;Ap5817: /* Analysis of Cl2 */&lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;== NH3 molecule ==&lt;br /&gt;
=== NH3 calculations ===&lt;br /&gt;
Calculation method:RB3LYP&lt;br /&gt;
&lt;br /&gt;
Basis Set = 6-31G(d,p)&lt;br /&gt;
&lt;br /&gt;
Final Energy: E(RB3LYP) = -56.557768 a.u.&lt;br /&gt;
&lt;br /&gt;
Bond length:1.01789 Å&lt;br /&gt;
&lt;br /&gt;
Bond angle: 105.741 °C&lt;br /&gt;
&lt;br /&gt;
Point Group: C3v&amp;lt;pre&amp;gt;&lt;br /&gt;
Item               Value     Threshold  Converged?&lt;br /&gt;
 Maximum Force            0.000004     0.000450     YES&lt;br /&gt;
 RMS     Force            0.000004     0.000300     YES&lt;br /&gt;
 Maximum Displacement     0.000072     0.001800     YES&lt;br /&gt;
 RMS     Displacement     0.000035     0.001200     YES&lt;br /&gt;
&amp;lt;/pre&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&amp;lt;jmol&amp;gt;&amp;lt;jmolApplet&amp;gt;&lt;br /&gt;
&amp;lt;script&amp;gt;frame x.y&amp;lt;/script&amp;gt;&lt;br /&gt;
  &amp;lt;title&amp;gt;test molecule&amp;lt;/title&amp;gt;&lt;br /&gt;
  &amp;lt;color&amp;gt;black&amp;lt;/color&amp;gt;&lt;br /&gt;
  &amp;lt;size&amp;gt;200&amp;lt;/size&amp;gt;&lt;br /&gt;
  &amp;lt;uploadedFileContents&amp;gt;ADRIAN_POPESCU_PHUNT_NH3_OPTF_POP.LOG&amp;lt;/uploadedFileContents&amp;gt;&lt;br /&gt;
&amp;lt;/jmolApplet&amp;gt;&amp;lt;/jmol&amp;gt;&lt;br /&gt;
&lt;br /&gt;
[[Media:ADRIAN_POPESCU_PHUNT_NH3_OPTF_POP.LOG]]&lt;br /&gt;
&lt;br /&gt;
==Vibration analysis of NH3==&lt;br /&gt;
[[File:Adrian_Popescu_Display_Vibrations.png|1000px]]&lt;br /&gt;
===Vibrational modes===&lt;br /&gt;
Number of vibrational modes: 6&lt;br /&gt;
&lt;br /&gt;
Number of degenerate modes: 4 (2 pairs of degenerate vibrational modes &lt;br /&gt;
&lt;br /&gt;
Number of bending motions: 3&lt;br /&gt;
&lt;br /&gt;
Number of stretching motions: 3&lt;br /&gt;
&lt;br /&gt;
The most symmetric vibrational mode: mode #4&lt;br /&gt;
&lt;br /&gt;
The &#039;&#039;umbrella mode&#039;&#039;: mode #1&lt;br /&gt;
&lt;br /&gt;
Number of bands expected to be seen in an experimental spectrum of gaseous ammonia: 5&lt;br /&gt;
===Charge Analysis===&lt;br /&gt;
[[File:Adrian_Popescu_Charges.png|1500px]]&lt;br /&gt;
&lt;br /&gt;
Charge on the N atom: -1.125&lt;br /&gt;
&lt;br /&gt;
Charge on the H atom: 0.375&lt;br /&gt;
&lt;br /&gt;
As Nitrogen has an electronegativity value of 3.04, which is significantly larger than the one of Hidrogen (2.2), it is expected that on the Nitrogen there will be a negative charge and on Hidrogen a possitive charge.&lt;br /&gt;
&lt;br /&gt;
==Reactivity of the Haber-Bosch process==&lt;br /&gt;
===Analysis of H2===&lt;br /&gt;
Calculation method:RB3LYP&lt;br /&gt;
&lt;br /&gt;
Basis Set = 6-31G(d,p)&lt;br /&gt;
&lt;br /&gt;
Final Energy: E(RB3LYP) = -1.1785393 a.u.&lt;br /&gt;
&lt;br /&gt;
Bond length:0.7428 Å&lt;br /&gt;
&amp;lt;pre&amp;gt;&lt;br /&gt;
Item               Value     Threshold  Converged?&lt;br /&gt;
 Maximum Force            0.000004     0.000450     YES&lt;br /&gt;
 RMS     Force            0.000004     0.000300     YES&lt;br /&gt;
 Maximum Displacement     0.000005     0.001800     YES&lt;br /&gt;
 RMS     Displacement     0.000007     0.001200     YES&amp;lt;/pre&amp;gt;&lt;br /&gt;
&amp;lt;pre&amp;gt;&lt;br /&gt;
Vibrational mode    Frequency    Infrared&lt;br /&gt;
#1             4465.6       0.0000&lt;br /&gt;
&amp;lt;/pre&amp;gt;&lt;br /&gt;
There are no vibrational modes with negative frequencies&lt;br /&gt;
===Analysis of N2===&lt;br /&gt;
Calculation method:RB3LYP&lt;br /&gt;
&lt;br /&gt;
Basis Set = 6-31G(d,p)&lt;br /&gt;
&lt;br /&gt;
Final Energy: E(RB3LYP) = -109.5241268 a.u.&lt;br /&gt;
&lt;br /&gt;
Bond length: 1.1055 Å&lt;br /&gt;
&amp;lt;pre&amp;gt;&lt;br /&gt;
Item               Value     Threshold  Converged?&lt;br /&gt;
 Maximum Force            0.000001     0.000450     YES&lt;br /&gt;
 RMS     Force            0.000001     0.000300     YES&lt;br /&gt;
 Maximum Displacement     0.000000     0.001800     YES&lt;br /&gt;
 RMS     Displacement     0.000000     0.001200     YES&lt;br /&gt;
&amp;lt;/pre&amp;gt;&lt;br /&gt;
&amp;lt;pre&amp;gt;&lt;br /&gt;
Vibrational mode    Frequency    Infrared&lt;br /&gt;
#1             2457.33       0.0000&lt;br /&gt;
&amp;lt;/pre&amp;gt;&lt;br /&gt;
There are no vibrational modes with negative frequencies&lt;br /&gt;
&lt;br /&gt;
===Calculation of the energy of the Haber-Bosch process===&lt;br /&gt;
N&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; + 3H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; -&amp;gt; 2NH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;&lt;br /&gt;
&lt;br /&gt;
E(NH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;)= -56.557768 a u&lt;br /&gt;
&lt;br /&gt;
2*E(NH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;)= -113.115536 a u&lt;br /&gt;
&lt;br /&gt;
E(N&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;)= -109.5251268 a u&lt;br /&gt;
&lt;br /&gt;
E(H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;)= -1.1785393 a u&lt;br /&gt;
&lt;br /&gt;
3*E(H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;)= -3.5359617 a u&lt;br /&gt;
&lt;br /&gt;
ΔE=2*E(NH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;) - [E(N&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;) + 3*E(H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;)] = -145.57 kj/mol&lt;br /&gt;
&lt;br /&gt;
As the reaction is exothermic, the ammonia product is more stable than the gaseous reactants.&lt;br /&gt;
==Analysis of Cl&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;==&lt;br /&gt;
===General Analysis===&lt;br /&gt;
Calculation method:RB3LYP&lt;br /&gt;
&lt;br /&gt;
Basis Set = 6-31G(d,p)&lt;br /&gt;
&lt;br /&gt;
Final Energy: E(RB3LYP) = -920.3498788 a.u.&lt;br /&gt;
&lt;br /&gt;
Bond length: 2.0417 Å&lt;br /&gt;
===Vibrational Analysis===&lt;br /&gt;
&amp;lt;pre&amp;gt;&lt;br /&gt;
 Item               Value     Threshold  Converged?&lt;br /&gt;
 Maximum Force            0.000043     0.000450     YES&lt;br /&gt;
 RMS     Force            0.000043     0.000300     YES&lt;br /&gt;
 Maximum Displacement     0.000121     0.001800     YES&lt;br /&gt;
 RMS     Displacement     0.000172     0.001200     YES&lt;br /&gt;
&lt;br /&gt;
&amp;lt;/pre&amp;gt;&lt;br /&gt;
&amp;lt;pre&amp;gt;&lt;br /&gt;
Vibrational mode    Frequency    Infrared&lt;br /&gt;
#1             520.32       0.0000&lt;br /&gt;
&amp;lt;/pre&amp;gt;&lt;br /&gt;
There are no vibrational modes with negative frequencies&lt;br /&gt;
===Charge Analysis===&lt;br /&gt;
[[File:Adrian_Popescu_Cl2_Charges.png|1000px]]&lt;br /&gt;
As the Cl&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; molecule is made up of identical Cl atoms, the bond between them will be 100% covalent, the electrons that form the sigma bond are equally shared between the cl atoms, so the charge on each Cl atom is zero.&lt;br /&gt;
===Molecular orbitals Analysis===&lt;/div&gt;</summary>
		<author><name>Ap5817</name></author>
	</entry>
	<entry>
		<id>https://chemwiki.ch.ic.ac.uk/index.php?title=User:Ap5817&amp;diff=679017</id>
		<title>User:Ap5817</title>
		<link rel="alternate" type="text/html" href="https://chemwiki.ch.ic.ac.uk/index.php?title=User:Ap5817&amp;diff=679017"/>
		<updated>2018-03-07T13:36:24Z</updated>

		<summary type="html">&lt;p&gt;Ap5817: /* Charge Analysis */&lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;== NH3 molecule ==&lt;br /&gt;
=== NH3 calculations ===&lt;br /&gt;
Calculation method:RB3LYP&lt;br /&gt;
&lt;br /&gt;
Basis Set = 6-31G(d,p)&lt;br /&gt;
&lt;br /&gt;
Final Energy: E(RB3LYP) = -56.557768 a.u.&lt;br /&gt;
&lt;br /&gt;
Bond length:1.01789 Å&lt;br /&gt;
&lt;br /&gt;
Bond angle: 105.741 °C&lt;br /&gt;
&lt;br /&gt;
Point Group: C3v&amp;lt;pre&amp;gt;&lt;br /&gt;
Item               Value     Threshold  Converged?&lt;br /&gt;
 Maximum Force            0.000004     0.000450     YES&lt;br /&gt;
 RMS     Force            0.000004     0.000300     YES&lt;br /&gt;
 Maximum Displacement     0.000072     0.001800     YES&lt;br /&gt;
 RMS     Displacement     0.000035     0.001200     YES&lt;br /&gt;
&amp;lt;/pre&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&amp;lt;jmol&amp;gt;&amp;lt;jmolApplet&amp;gt;&lt;br /&gt;
&amp;lt;script&amp;gt;frame x.y&amp;lt;/script&amp;gt;&lt;br /&gt;
  &amp;lt;title&amp;gt;test molecule&amp;lt;/title&amp;gt;&lt;br /&gt;
  &amp;lt;color&amp;gt;black&amp;lt;/color&amp;gt;&lt;br /&gt;
  &amp;lt;size&amp;gt;200&amp;lt;/size&amp;gt;&lt;br /&gt;
  &amp;lt;uploadedFileContents&amp;gt;ADRIAN_POPESCU_PHUNT_NH3_OPTF_POP.LOG&amp;lt;/uploadedFileContents&amp;gt;&lt;br /&gt;
&amp;lt;/jmolApplet&amp;gt;&amp;lt;/jmol&amp;gt;&lt;br /&gt;
&lt;br /&gt;
[[Media:ADRIAN_POPESCU_PHUNT_NH3_OPTF_POP.LOG]]&lt;br /&gt;
&lt;br /&gt;
==Vibration analysis of NH3==&lt;br /&gt;
[[File:Adrian_Popescu_Display_Vibrations.png|1000px]]&lt;br /&gt;
===Vibrational modes===&lt;br /&gt;
Number of vibrational modes: 6&lt;br /&gt;
&lt;br /&gt;
Number of degenerate modes: 4 (2 pairs of degenerate vibrational modes &lt;br /&gt;
&lt;br /&gt;
Number of bending motions: 3&lt;br /&gt;
&lt;br /&gt;
Number of stretching motions: 3&lt;br /&gt;
&lt;br /&gt;
The most symmetric vibrational mode: mode #4&lt;br /&gt;
&lt;br /&gt;
The &#039;&#039;umbrella mode&#039;&#039;: mode #1&lt;br /&gt;
&lt;br /&gt;
Number of bands expected to be seen in an experimental spectrum of gaseous ammonia: 5&lt;br /&gt;
===Charge Analysis===&lt;br /&gt;
[[File:Adrian_Popescu_Charges.png|1500px]]&lt;br /&gt;
&lt;br /&gt;
Charge on the N atom: -1.125&lt;br /&gt;
&lt;br /&gt;
Charge on the H atom: 0.375&lt;br /&gt;
&lt;br /&gt;
As Nitrogen has an electronegativity value of 3.04, which is significantly larger than the one of Hidrogen (2.2), it is expected that on the Nitrogen there will be a negative charge and on Hidrogen a possitive charge.&lt;br /&gt;
&lt;br /&gt;
==Reactivity of the Haber-Bosch process==&lt;br /&gt;
===Analysis of H2===&lt;br /&gt;
Calculation method:RB3LYP&lt;br /&gt;
&lt;br /&gt;
Basis Set = 6-31G(d,p)&lt;br /&gt;
&lt;br /&gt;
Final Energy: E(RB3LYP) = -1.1785393 a.u.&lt;br /&gt;
&lt;br /&gt;
Bond length:0.7428 Å&lt;br /&gt;
&amp;lt;pre&amp;gt;&lt;br /&gt;
Item               Value     Threshold  Converged?&lt;br /&gt;
 Maximum Force            0.000004     0.000450     YES&lt;br /&gt;
 RMS     Force            0.000004     0.000300     YES&lt;br /&gt;
 Maximum Displacement     0.000005     0.001800     YES&lt;br /&gt;
 RMS     Displacement     0.000007     0.001200     YES&amp;lt;/pre&amp;gt;&lt;br /&gt;
&amp;lt;pre&amp;gt;&lt;br /&gt;
Vibrational mode    Frequency    Infrared&lt;br /&gt;
#1             4465.6       0.0000&lt;br /&gt;
&amp;lt;/pre&amp;gt;&lt;br /&gt;
There are no vibrational modes with negative frequencies&lt;br /&gt;
===Analysis of N2===&lt;br /&gt;
Calculation method:RB3LYP&lt;br /&gt;
&lt;br /&gt;
Basis Set = 6-31G(d,p)&lt;br /&gt;
&lt;br /&gt;
Final Energy: E(RB3LYP) = -109.5241268 a.u.&lt;br /&gt;
&lt;br /&gt;
Bond length: 1.1055 Å&lt;br /&gt;
&amp;lt;pre&amp;gt;&lt;br /&gt;
Item               Value     Threshold  Converged?&lt;br /&gt;
 Maximum Force            0.000001     0.000450     YES&lt;br /&gt;
 RMS     Force            0.000001     0.000300     YES&lt;br /&gt;
 Maximum Displacement     0.000000     0.001800     YES&lt;br /&gt;
 RMS     Displacement     0.000000     0.001200     YES&lt;br /&gt;
&amp;lt;/pre&amp;gt;&lt;br /&gt;
&amp;lt;pre&amp;gt;&lt;br /&gt;
Vibrational mode    Frequency    Infrared&lt;br /&gt;
#1             2457.33       0.0000&lt;br /&gt;
&amp;lt;/pre&amp;gt;&lt;br /&gt;
There are no vibrational modes with negative frequencies&lt;br /&gt;
&lt;br /&gt;
===Calculation of the energy of the Haber-Bosch process===&lt;br /&gt;
N&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; + 3H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; -&amp;gt; 2NH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;&lt;br /&gt;
&lt;br /&gt;
E(NH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;)= -56.557768 a u&lt;br /&gt;
&lt;br /&gt;
2*E(NH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;)= -113.115536 a u&lt;br /&gt;
&lt;br /&gt;
E(N&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;)= -109.5251268 a u&lt;br /&gt;
&lt;br /&gt;
E(H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;)= -1.1785393 a u&lt;br /&gt;
&lt;br /&gt;
3*E(H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;)= -3.5359617 a u&lt;br /&gt;
&lt;br /&gt;
ΔE=2*E(NH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;) - [E(N&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;) + 3*E(H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;)] = -145.57 kj/mol&lt;br /&gt;
&lt;br /&gt;
As the reaction is exothermic, the ammonia product is more stable than the gaseous reactants.&lt;br /&gt;
==Analysis of Cl&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;==&lt;br /&gt;
===General Analysis===&lt;br /&gt;
Calculation method:RB3LYP&lt;br /&gt;
&lt;br /&gt;
Basis Set = 6-31G(d,p)&lt;br /&gt;
&lt;br /&gt;
Final Energy: E(RB3LYP) = -920.3498788 a.u.&lt;br /&gt;
&lt;br /&gt;
Bond length: 2.0417 Å&lt;br /&gt;
===Vibrational Analysis===&lt;br /&gt;
&amp;lt;pre&amp;gt;&lt;br /&gt;
 Item               Value     Threshold  Converged?&lt;br /&gt;
 Maximum Force            0.000043     0.000450     YES&lt;br /&gt;
 RMS     Force            0.000043     0.000300     YES&lt;br /&gt;
 Maximum Displacement     0.000121     0.001800     YES&lt;br /&gt;
 RMS     Displacement     0.000172     0.001200     YES&lt;br /&gt;
&lt;br /&gt;
&amp;lt;/pre&amp;gt;&lt;br /&gt;
&amp;lt;pre&amp;gt;&lt;br /&gt;
Vibrational mode    Frequency    Infrared&lt;br /&gt;
#1             520.32       0.0000&lt;br /&gt;
&amp;lt;/pre&amp;gt;&lt;br /&gt;
There are no vibrational modes with negative frequencies&lt;br /&gt;
===Charge Analysis===&lt;br /&gt;
[[File:Adrian_Popescu_Cl2_Charges.png|1000px]]&lt;br /&gt;
As the Cl&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; molecule is made up of identical Cl atoms, the bond between them will be 100% covalent, the electrons that form the sigma bond are equally shared between the cl atoms, so the charge on each Cl atom is zero.&lt;/div&gt;</summary>
		<author><name>Ap5817</name></author>
	</entry>
	<entry>
		<id>https://chemwiki.ch.ic.ac.uk/index.php?title=User:Ap5817&amp;diff=679007</id>
		<title>User:Ap5817</title>
		<link rel="alternate" type="text/html" href="https://chemwiki.ch.ic.ac.uk/index.php?title=User:Ap5817&amp;diff=679007"/>
		<updated>2018-03-07T13:27:48Z</updated>

		<summary type="html">&lt;p&gt;Ap5817: &lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;== NH3 molecule ==&lt;br /&gt;
=== NH3 calculations ===&lt;br /&gt;
Calculation method:RB3LYP&lt;br /&gt;
&lt;br /&gt;
Basis Set = 6-31G(d,p)&lt;br /&gt;
&lt;br /&gt;
Final Energy: E(RB3LYP) = -56.557768 a.u.&lt;br /&gt;
&lt;br /&gt;
Bond length:1.01789 Å&lt;br /&gt;
&lt;br /&gt;
Bond angle: 105.741 °C&lt;br /&gt;
&lt;br /&gt;
Point Group: C3v&amp;lt;pre&amp;gt;&lt;br /&gt;
Item               Value     Threshold  Converged?&lt;br /&gt;
 Maximum Force            0.000004     0.000450     YES&lt;br /&gt;
 RMS     Force            0.000004     0.000300     YES&lt;br /&gt;
 Maximum Displacement     0.000072     0.001800     YES&lt;br /&gt;
 RMS     Displacement     0.000035     0.001200     YES&lt;br /&gt;
&amp;lt;/pre&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&amp;lt;jmol&amp;gt;&amp;lt;jmolApplet&amp;gt;&lt;br /&gt;
&amp;lt;script&amp;gt;frame x.y&amp;lt;/script&amp;gt;&lt;br /&gt;
  &amp;lt;title&amp;gt;test molecule&amp;lt;/title&amp;gt;&lt;br /&gt;
  &amp;lt;color&amp;gt;black&amp;lt;/color&amp;gt;&lt;br /&gt;
  &amp;lt;size&amp;gt;200&amp;lt;/size&amp;gt;&lt;br /&gt;
  &amp;lt;uploadedFileContents&amp;gt;ADRIAN_POPESCU_PHUNT_NH3_OPTF_POP.LOG&amp;lt;/uploadedFileContents&amp;gt;&lt;br /&gt;
&amp;lt;/jmolApplet&amp;gt;&amp;lt;/jmol&amp;gt;&lt;br /&gt;
&lt;br /&gt;
[[Media:ADRIAN_POPESCU_PHUNT_NH3_OPTF_POP.LOG]]&lt;br /&gt;
&lt;br /&gt;
==Vibration analysis of NH3==&lt;br /&gt;
[[File:Adrian_Popescu_Display_Vibrations.png|1000px]]&lt;br /&gt;
===Vibrational modes===&lt;br /&gt;
Number of vibrational modes: 6&lt;br /&gt;
&lt;br /&gt;
Number of degenerate modes: 4 (2 pairs of degenerate vibrational modes &lt;br /&gt;
&lt;br /&gt;
Number of bending motions: 3&lt;br /&gt;
&lt;br /&gt;
Number of stretching motions: 3&lt;br /&gt;
&lt;br /&gt;
The most symmetric vibrational mode: mode #4&lt;br /&gt;
&lt;br /&gt;
The &#039;&#039;umbrella mode&#039;&#039;: mode #1&lt;br /&gt;
&lt;br /&gt;
Number of bands expected to be seen in an experimental spectrum of gaseous ammonia: 5&lt;br /&gt;
===Charge Analysis===&lt;br /&gt;
[[File:Adrian_Popescu_Charges.png|1500px]]&lt;br /&gt;
&lt;br /&gt;
Charge on the N atom: -1.125&lt;br /&gt;
&lt;br /&gt;
Charge on the H atom: 0.375&lt;br /&gt;
&lt;br /&gt;
As Nitrogen has an electronegativity value of 3.04, which is significantly larger than the one of Hidrogen (2.2), it is expected that on the Nitrogen there will be a negative charge and on Hidrogen a possitive charge.&lt;br /&gt;
&lt;br /&gt;
==Reactivity of the Haber-Bosch process==&lt;br /&gt;
===Analysis of H2===&lt;br /&gt;
Calculation method:RB3LYP&lt;br /&gt;
&lt;br /&gt;
Basis Set = 6-31G(d,p)&lt;br /&gt;
&lt;br /&gt;
Final Energy: E(RB3LYP) = -1.1785393 a.u.&lt;br /&gt;
&lt;br /&gt;
Bond length:0.7428 Å&lt;br /&gt;
&amp;lt;pre&amp;gt;&lt;br /&gt;
Item               Value     Threshold  Converged?&lt;br /&gt;
 Maximum Force            0.000004     0.000450     YES&lt;br /&gt;
 RMS     Force            0.000004     0.000300     YES&lt;br /&gt;
 Maximum Displacement     0.000005     0.001800     YES&lt;br /&gt;
 RMS     Displacement     0.000007     0.001200     YES&amp;lt;/pre&amp;gt;&lt;br /&gt;
&amp;lt;pre&amp;gt;&lt;br /&gt;
Vibrational mode    Frequency    Infrared&lt;br /&gt;
#1             4465.6       0.0000&lt;br /&gt;
&amp;lt;/pre&amp;gt;&lt;br /&gt;
There are no vibrational modes with negative frequencies&lt;br /&gt;
===Analysis of N2===&lt;br /&gt;
Calculation method:RB3LYP&lt;br /&gt;
&lt;br /&gt;
Basis Set = 6-31G(d,p)&lt;br /&gt;
&lt;br /&gt;
Final Energy: E(RB3LYP) = -109.5241268 a.u.&lt;br /&gt;
&lt;br /&gt;
Bond length: 1.1055 Å&lt;br /&gt;
&amp;lt;pre&amp;gt;&lt;br /&gt;
Item               Value     Threshold  Converged?&lt;br /&gt;
 Maximum Force            0.000001     0.000450     YES&lt;br /&gt;
 RMS     Force            0.000001     0.000300     YES&lt;br /&gt;
 Maximum Displacement     0.000000     0.001800     YES&lt;br /&gt;
 RMS     Displacement     0.000000     0.001200     YES&lt;br /&gt;
&amp;lt;/pre&amp;gt;&lt;br /&gt;
&amp;lt;pre&amp;gt;&lt;br /&gt;
Vibrational mode    Frequency    Infrared&lt;br /&gt;
#1             2457.33       0.0000&lt;br /&gt;
&amp;lt;/pre&amp;gt;&lt;br /&gt;
There are no vibrational modes with negative frequencies&lt;br /&gt;
&lt;br /&gt;
===Calculation of the energy of the Haber-Bosch process===&lt;br /&gt;
N&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; + 3H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; -&amp;gt; 2NH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;&lt;br /&gt;
&lt;br /&gt;
E(NH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;)= -56.557768 a u&lt;br /&gt;
&lt;br /&gt;
2*E(NH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;)= -113.115536 a u&lt;br /&gt;
&lt;br /&gt;
E(N&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;)= -109.5251268 a u&lt;br /&gt;
&lt;br /&gt;
E(H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;)= -1.1785393 a u&lt;br /&gt;
&lt;br /&gt;
3*E(H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;)= -3.5359617 a u&lt;br /&gt;
&lt;br /&gt;
ΔE=2*E(NH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;) - [E(N&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;) + 3*E(H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;)] = -145.57 kj/mol&lt;br /&gt;
&lt;br /&gt;
As the reaction is exothermic, the ammonia product is more stable than the gaseous reactants.&lt;br /&gt;
==Analysis of Cl&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;==&lt;br /&gt;
===General Analysis===&lt;br /&gt;
Calculation method:RB3LYP&lt;br /&gt;
&lt;br /&gt;
Basis Set = 6-31G(d,p)&lt;br /&gt;
&lt;br /&gt;
Final Energy: E(RB3LYP) = -920.3498788 a.u.&lt;br /&gt;
&lt;br /&gt;
Bond length: 2.0417 Å&lt;br /&gt;
===Vibrational Analysis===&lt;br /&gt;
&amp;lt;pre&amp;gt;&lt;br /&gt;
 Item               Value     Threshold  Converged?&lt;br /&gt;
 Maximum Force            0.000043     0.000450     YES&lt;br /&gt;
 RMS     Force            0.000043     0.000300     YES&lt;br /&gt;
 Maximum Displacement     0.000121     0.001800     YES&lt;br /&gt;
 RMS     Displacement     0.000172     0.001200     YES&lt;br /&gt;
&lt;br /&gt;
&amp;lt;/pre&amp;gt;&lt;br /&gt;
&amp;lt;pre&amp;gt;&lt;br /&gt;
Vibrational mode    Frequency    Infrared&lt;br /&gt;
#1             520.32       0.0000&lt;br /&gt;
&amp;lt;/pre&amp;gt;&lt;br /&gt;
There are no vibrational modes with negative frequencies&lt;br /&gt;
===Charge Analysis===&lt;br /&gt;
[[File:Adrian_Popescu_Cl2_Charges.png|1000px]]&lt;/div&gt;</summary>
		<author><name>Ap5817</name></author>
	</entry>
	<entry>
		<id>https://chemwiki.ch.ic.ac.uk/index.php?title=User:Ap5817&amp;diff=679005</id>
		<title>User:Ap5817</title>
		<link rel="alternate" type="text/html" href="https://chemwiki.ch.ic.ac.uk/index.php?title=User:Ap5817&amp;diff=679005"/>
		<updated>2018-03-07T13:27:08Z</updated>

		<summary type="html">&lt;p&gt;Ap5817: &lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;== NH3 molecule ==&lt;br /&gt;
=== NH3 calculations ===&lt;br /&gt;
Calculation method:RB3LYP&lt;br /&gt;
&lt;br /&gt;
Basis Set = 6-31G(d,p)&lt;br /&gt;
&lt;br /&gt;
Final Energy: E(RB3LYP) = -56.557768 a.u.&lt;br /&gt;
&lt;br /&gt;
Bond length:1.01789 Å&lt;br /&gt;
&lt;br /&gt;
Bond angle: 105.741 °C&lt;br /&gt;
&lt;br /&gt;
Point Group: C3v&amp;lt;pre&amp;gt;&lt;br /&gt;
Item               Value     Threshold  Converged?&lt;br /&gt;
 Maximum Force            0.000004     0.000450     YES&lt;br /&gt;
 RMS     Force            0.000004     0.000300     YES&lt;br /&gt;
 Maximum Displacement     0.000072     0.001800     YES&lt;br /&gt;
 RMS     Displacement     0.000035     0.001200     YES&lt;br /&gt;
&amp;lt;/pre&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&amp;lt;jmol&amp;gt;&amp;lt;jmolApplet&amp;gt;&lt;br /&gt;
&amp;lt;script&amp;gt;frame x.y&amp;lt;/script&amp;gt;&lt;br /&gt;
  &amp;lt;title&amp;gt;test molecule&amp;lt;/title&amp;gt;&lt;br /&gt;
  &amp;lt;color&amp;gt;black&amp;lt;/color&amp;gt;&lt;br /&gt;
  &amp;lt;size&amp;gt;200&amp;lt;/size&amp;gt;&lt;br /&gt;
  &amp;lt;uploadedFileContents&amp;gt;ADRIAN_POPESCU_PHUNT_NH3_OPTF_POP.LOG&amp;lt;/uploadedFileContents&amp;gt;&lt;br /&gt;
&amp;lt;/jmolApplet&amp;gt;&amp;lt;/jmol&amp;gt;&lt;br /&gt;
&lt;br /&gt;
[[Media:ADRIAN_POPESCU_PHUNT_NH3_OPTF_POP.LOG]]&lt;br /&gt;
&lt;br /&gt;
==Vibration analysis of NH3==&lt;br /&gt;
[[File:Adrian_Popescu_Display_Vibrations.png|1000px]]&lt;br /&gt;
===Vibrational modes===&lt;br /&gt;
Number of vibrational modes: 6&lt;br /&gt;
&lt;br /&gt;
Number of degenerate modes: 4 (2 pairs of degenerate vibrational modes &lt;br /&gt;
&lt;br /&gt;
Number of bending motions: 3&lt;br /&gt;
&lt;br /&gt;
Number of stretching motions: 3&lt;br /&gt;
&lt;br /&gt;
The most symmetric vibrational mode: mode #4&lt;br /&gt;
&lt;br /&gt;
The &#039;&#039;umbrella mode&#039;&#039;: mode #1&lt;br /&gt;
&lt;br /&gt;
Number of bands expected to be seen in an experimental spectrum of gaseous ammonia: 5&lt;br /&gt;
===Charge Analysis===&lt;br /&gt;
[[File:Adrian_Popescu_Charges.png|1500px]]&lt;br /&gt;
&lt;br /&gt;
Charge on the N atom: -1.125&lt;br /&gt;
&lt;br /&gt;
Charge on the H atom: 0.375&lt;br /&gt;
&lt;br /&gt;
As Nitrogen has an electronegativity value of 3.04, which is significantly larger than the one of Hidrogen (2.2), it is expected that on the Nitrogen there will be a negative charge and on Hidrogen a possitive charge.&lt;br /&gt;
&lt;br /&gt;
==Reactivity of the Haber-Bosch process==&lt;br /&gt;
===Analysis of H2===&lt;br /&gt;
Calculation method:RB3LYP&lt;br /&gt;
&lt;br /&gt;
Basis Set = 6-31G(d,p)&lt;br /&gt;
&lt;br /&gt;
Final Energy: E(RB3LYP) = -1.1785393 a.u.&lt;br /&gt;
&lt;br /&gt;
Bond length:0.7428 Å&lt;br /&gt;
&amp;lt;pre&amp;gt;&lt;br /&gt;
Item               Value     Threshold  Converged?&lt;br /&gt;
 Maximum Force            0.000004     0.000450     YES&lt;br /&gt;
 RMS     Force            0.000004     0.000300     YES&lt;br /&gt;
 Maximum Displacement     0.000005     0.001800     YES&lt;br /&gt;
 RMS     Displacement     0.000007     0.001200     YES&amp;lt;/pre&amp;gt;&lt;br /&gt;
&amp;lt;pre&amp;gt;&lt;br /&gt;
Vibrational mode    Frequency    Infrared&lt;br /&gt;
#1             4465.6       0.0000&lt;br /&gt;
&amp;lt;/pre&amp;gt;&lt;br /&gt;
There are no vibrational modes with negative frequencies&lt;br /&gt;
===Analysis of N2===&lt;br /&gt;
Calculation method:RB3LYP&lt;br /&gt;
&lt;br /&gt;
Basis Set = 6-31G(d,p)&lt;br /&gt;
&lt;br /&gt;
Final Energy: E(RB3LYP) = -109.5241268 a.u.&lt;br /&gt;
&lt;br /&gt;
Bond length: 1.1055 Å&lt;br /&gt;
&amp;lt;pre&amp;gt;&lt;br /&gt;
Item               Value     Threshold  Converged?&lt;br /&gt;
 Maximum Force            0.000001     0.000450     YES&lt;br /&gt;
 RMS     Force            0.000001     0.000300     YES&lt;br /&gt;
 Maximum Displacement     0.000000     0.001800     YES&lt;br /&gt;
 RMS     Displacement     0.000000     0.001200     YES&lt;br /&gt;
&amp;lt;/pre&amp;gt;&lt;br /&gt;
&amp;lt;pre&amp;gt;&lt;br /&gt;
Vibrational mode    Frequency    Infrared&lt;br /&gt;
#1             2457.33       0.0000&lt;br /&gt;
&amp;lt;/pre&amp;gt;&lt;br /&gt;
There are no vibrational modes with negative frequencies&lt;br /&gt;
&lt;br /&gt;
===Calculation of the energy of the Haber-Bosch process===&lt;br /&gt;
N&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; + 3H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; -&amp;gt; 2NH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;&lt;br /&gt;
&lt;br /&gt;
E(NH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;)= -56.557768 a u&lt;br /&gt;
&lt;br /&gt;
2*E(NH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;)= -113.115536 a u&lt;br /&gt;
&lt;br /&gt;
E(N&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;)= -109.5251268 a u&lt;br /&gt;
&lt;br /&gt;
E(H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;)= -1.1785393 a u&lt;br /&gt;
&lt;br /&gt;
3*E(H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;)= -3.5359617 a u&lt;br /&gt;
&lt;br /&gt;
ΔE=2*E(NH&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt;) - [E(N&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;) + 3*E(H&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;)] = -145.57 kj/mol&lt;br /&gt;
&lt;br /&gt;
As the reaction is exothermic, the ammonia product is more stable than the gaseous reactants.&lt;br /&gt;
==Analysis of Cl&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;==&lt;br /&gt;
===General Analysis===&lt;br /&gt;
Calculation method:RB3LYP&lt;br /&gt;
&lt;br /&gt;
Basis Set = 6-31G(d,p)&lt;br /&gt;
&lt;br /&gt;
Final Energy: E(RB3LYP) = -920.3498788 a.u.&lt;br /&gt;
&lt;br /&gt;
Bond length: 2.0417 Å&lt;br /&gt;
===Vibrational Analysis===&lt;br /&gt;
&amp;lt;pre&amp;gt;&lt;br /&gt;
 Item               Value     Threshold  Converged?&lt;br /&gt;
 Maximum Force            0.000043     0.000450     YES&lt;br /&gt;
 RMS     Force            0.000043     0.000300     YES&lt;br /&gt;
 Maximum Displacement     0.000121     0.001800     YES&lt;br /&gt;
 RMS     Displacement     0.000172     0.001200     YES&lt;br /&gt;
&lt;br /&gt;
&amp;lt;/pre&amp;gt;&lt;br /&gt;
&amp;lt;pre&amp;gt;&lt;br /&gt;
Vibrational mode    Frequency    Infrared&lt;br /&gt;
#1             520.32       0.0000&lt;br /&gt;
&amp;lt;/pre&amp;gt;&lt;br /&gt;
There are no vibrational modes with negative frequencies&lt;br /&gt;
===Charge Analysis===&lt;br /&gt;
[[File:Adrian_Popescu_Cl2_Charges.png]]&lt;/div&gt;</summary>
		<author><name>Ap5817</name></author>
	</entry>
	<entry>
		<id>https://chemwiki.ch.ic.ac.uk/index.php?title=File:Adrian_Popescu_Cl2_Charges.png&amp;diff=678999</id>
		<title>File:Adrian Popescu Cl2 Charges.png</title>
		<link rel="alternate" type="text/html" href="https://chemwiki.ch.ic.ac.uk/index.php?title=File:Adrian_Popescu_Cl2_Charges.png&amp;diff=678999"/>
		<updated>2018-03-07T13:25:53Z</updated>

		<summary type="html">&lt;p&gt;Ap5817: &lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;&lt;/div&gt;</summary>
		<author><name>Ap5817</name></author>
	</entry>
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