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EX3

Molecules

BH3

RB3LYP/6-31G(d,p) level

 
 Item               Value     Threshold  Converged?
 Maximum Force            0.000161     0.000450     YES
 RMS     Force            0.000105     0.000300     YES
 Maximum Displacement     0.000638     0.001800     YES
 RMS     Displacement     0.000417     0.001200     YES

Frequency analysis log file EMCK_BH3_FREQ1.log

 Low frequencies ---   -0.1187   -0.0049   -0.0009   42.2482   42.2484   43.3387
 Low frequencies --- 1163.5889 1213.5519 1213.5521
optimised BH3 molecule

Vibrational Spectrum for BH3

wavenumber (cm-1) Intensity (arbitrary units) symmetry IR active? type
1164 93 A2 yes out-of-plane bend
1214 14 E very slight in-plane bend
1214 14 E very slight in-plane bend
2580 0 A1 no symmetric stretch
2713 126 E yes asymmetric stretch
2713 126 E yes asymmetric stretch

Although there are 6 vibrations for this molecule, as predicted by the 3N-6 rule (N=4), the vibrational spectrum for BH3 only shows 3 peaks. This is due to the two degenerate vibrations at both 1214 and at 2713 cm-1, which thus show only one peak at each frequency. The vibration at 2580 cm-1 is not IR active, and so doesn't show a peak on the spectrum.

Reference: Molecular Orbitals in Inorganic Chemistry, P. Hunt, Imperial College London, URL: http://www.huntresearchgroup.org.uk/teaching/year2_mos.html, [date accessed: 11/05/18]

Answer these questions: Are there any significant differences between the real and LCAO MOs? What does this say about the accuracy and usefulness of qualitative MO theory?

NH3

B3LYP/6-31G(d,p) level

 Item               Value     Threshold  Converged?
 Maximum Force            0.000059     0.000450     YES
 RMS     Force            0.000040     0.000300     YES
 Maximum Displacement     0.000174     0.001800     YES
 RMS     Displacement     0.000082     0.001200     YES

Frequency analysis log file EMCK_NH3_FREQ.log

 Low frequencies ---  -30.2465  -30.2464  -27.9012   -0.0012    0.0012    0.0033
 Low frequencies --- 1088.3845 1693.7755 1693.7755
optimised NH3 molecule

NH3BH3

B3LYP/6-31G(d,p) level

 Item               Value     Threshold  Converged?
 Maximum Force            0.000272     0.000450     YES
 RMS     Force            0.000060     0.000300     YES
 Maximum Displacement     0.001497     0.001800     YES
 RMS     Displacement     0.000379     0.001200     YES

Frequency analysis log file EMCK_NH3BH3_FREQ.log

 Low frequencies ---  -12.2521   -0.0251   -0.0056    0.0213    9.9744   10.0237
 Low frequencies ---  262.7785  631.1507  638.0575
optimised NH3BH3 molecule

B-N Dative Bond Energy

Total energies, a.u. E(NH3)= -56.55776 E(BH3)=-26.61532 E(NH3BH3)= -83.22468

Calculation for association energy

ΔE= E(NH3BH3)-[E(NH3)+E(BH3)] = -83.22468-(-56.55776 + -26.61532) = -0.05159 a.u.

NB conversion factor: 1 a.u. = 2625.5 kJ/mol

B-N dative bond strength = -135.4671 kJ/mol

This bond is stronger than the B-H bond, but weaker than the B-C bond.

BBr3

B3LYP/6-31G(d,p)LANL2DZ level

File:Emck bbr3 opt summary.png

 Item               Value     Threshold  Converged?
 Maximum Force            0.000008     0.000450     YES
 RMS     Force            0.000005     0.000300     YES
 Maximum Displacement     0.000036     0.001800     YES
 RMS     Displacement     0.000024     0.001200     YES

Frequency analysis log file (via DSpace) DOI:10042/202393

 Low frequencies ---   -2.3055   -0.0029   -0.0018    0.0774    0.7534    0.7534
 Low frequencies ---  155.9402  155.9405  267.6894
optimised BBr3 molecule

Project Section: Aromaticity

Molecules

Benzene

B3LYP/6-31G(d,p) level

 Item               Value     Threshold  Converged?
 Maximum Force            0.000045     0.000450     YES
 RMS     Force            0.000016     0.000300     YES
 Maximum Displacement     0.000097     0.001800     YES
 RMS     Displacement     0.000036     0.001200     YES

Frequency analysis log file EMCK_BENZENE_FREQ.log

 Low frequencies ---  -11.2122   -7.2552   -7.2552   -0.0055   -0.0054    0.0002
 Low frequencies ---  414.4981  414.4981  621.0619
optimised benzene molecule


Borazine

B3LYP/6-31G(d,p) level

NOTE TO MARKER: My log file for borazine has been uploaded before the deadline, but the link is as follows : File:EMCK BORAZINE FREQ.LOG

 Item               Value     Threshold  Converged?
 Maximum Force            0.000028     0.000450     YES
 RMS     Force            0.000011     0.000300     YES
 Maximum Displacement     0.000105     0.001800     YES
 RMS     Displacement     0.000037     0.001200     YES
 Low frequencies ---   -5.3732   -5.3575   -5.1081   -0.0036    0.0013    0.0113
 Low frequencies ---  289.6801  289.6807  404.4817
optimised borazine molecule

Molecular Orbitals

Molecular Orbitals
MO # Benzene MO # Borazine Comparison
14 14 MO14 for benzene and borazine is similar in shape and energy, however its energy in borazine (-0.43402 hartrees) is slightly lower than in benzene (-0.43853 hartrees). This is an antibonding MO, formed via overlap of antibonding sigma orbitals of the C-C bonds in benzene and B-N bonds in borazine, and the lower energy of borazine reflects the weaker sigma overlap along the B-N axis, which results in less antibonding character and thus a lower total energy.
17 17 MO 17 for benzene (left) and borazine (right) are also very similar in shape and energy, and the borazine MO is again lower in energy(-0.36134 hartrees) than that of benzene(-0.35996 hartrees). These bonding MOs are formed by the sideways in-phase overlap of the 6 p-orbitals on each atom in the conjugated pi ring. There are slight differences in the MO shapes visible as a small bulge around the nitrogen atoms due to the increased electron deficiency surrounding them as a result of the higher electronegativity of nitrogen. This causes MO17 in borazine to be lower in energy due to the increased electrostatic attraction between nitrogen and boron. In both MOs, there is no contribution from the hydrogens as they have no p orbitals.
21 21 MO21 are similar in shape and energy in both molecules. It is an antibonding MO that results from the sideways overlap of p orbitals. Three of the p orbitals are in phase and 3 are out of phase thus there are 2 nodal planes dividing the MO, and hydrogen atoms don't contribute in either as they have no p-orbitals the MO. Increased mismatch in size of the overlapping p-orbitals in borazine leads to more distorsion and less symmetry in borazine.


Smf115 (talk) 00:25, 23 May 2018 (BST)Good attempt at comparing the MOs. However, energies are not comparable between the MOs and it was the shape of the orbitals which needed to be considered when selecting two to compare. MO 14 from benzene is instead comparable to MO 15 from borazine which should have been noticed. The comparison for the remaining MOs could be improved with inclusion of details such as pi- or sigma-orbitals/interactions and to the symmetries.

Charge Distributions

Charge Distributions
Benzene Key Borazine Key
C(red)= -0.239

H(green)= +0.239

N (red) -1.102

B (green)=0.747 H (dark green)=0.432 H (black)= -0.077

Comparison
Benzene has a more symmetrical charge distribution, as all of the carbon atoms have the same electronegativity. It is clear that the charge difference along the C-H bond is low, and that this bond is non-polar. In borazine, the significant charge difference between the boron and nitrogen atoms in the ring(0.747 and -1.102, respectively) reflects the difference in their electronegativities. The nitrogen atoms withdraw electron density from the hydrogens bonded to them and into the pi system of the borazine ring, resulting in the hydrogens (shown in darker green) having a charge of +0.432. This value is more positive than that of the benzene hydrogen atoms (+0.239), reflecting their decreased electron density. The electropositive boron atoms donate electron density to their hydrogens (shown in black), leading to the hydrogens having a charge of -0.077 which shows their increased electron density relative to the benzene hydrogens.

These charge differences within the borazine molecule lead to increased ionic character in its bonds, causing increased bond strengths.

Smf115 (talk) 00:27, 23 May 2018 (BST)Good charge analysis with a clear explaination due to electronegativies and the same colour range has been used for the charge distribution across both molecules.

Aromaticity

discuss in your wiki (2-3 paragraphs) the concept of aromaticity, the simple ideas and also the more complex descriptions.

   how do the real MOs relate to the common (very basic) conceptions of aromaticity?
   you are expected to explain why the concept of overlapping pz AOs is NOT a good description for aromaticity.

Smf115 (talk) 00:30, 23 May 2018 (BST)Overall, a good attempt in places but a disapointing, unfinished project section and broken log file links throughout the report. Where the questions have been given time and thought, such as the charge analysis, then the answers are good.