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BH3 molecule

Summary

Method and Basis Set: B3LYP/6-31G(d,p)

Summary Table of an optimised BH3 molecule.

Optimisation

         Item               Value     Threshold  Converged?
 Maximum Force            0.000000     0.000450     YES
 RMS     Force            0.000000     0.000300     YES
 Maximum Displacement     0.000002     0.001800     YES
 RMS     Displacement     0.000001     0.001200     YES

Link: File:ANGUS BH3 FREQ.LOG

Frequency Analysis

Low frequencies ---   -0.7840   -0.5083   -0.0054    9.7343   14.1292   14.1509
Low frequencies ---   1163.0162 1213.1960 1213.1987

Rotatable 3d image of optimized BH3

Vibrational spectrum for BH3

wavenumber (cm-1 Intensity (arbitrary units) symmetry IR active? type
1163 93 A2 yes out-of-plane bend
1213 14 E very slight bend
1213 14 E very slight bend
2582 0 A1 no symmetric stretch
2715 126 E yes asymmetric stretch
2715 126 E yes asymmetric stretch
Vibrational anlysis of an optimised BH3 molecule.

Only 3 bands are observed in the experimental spectrum of BH3. Although there are 6 vibrational frequencies calculated according to GaussView, vibrational modes 2 and 3, 5 and 6 are degenerate as their stretching frequencies are the same. So 4 bands should be observed. However, vibrational modes 4 is highly symmetric and there is no overall dipole moment. As a result, it is not IR active.

Molecular Orbitals of BH3

MO Diagram of BH3. Reference: Molecular Orbitals in Inorganic Chemistry Lecture 4 Tutorial Problem Answers, Prof. Patricia Hunt

There are only slight differences between the real and LCAO MOs, especially for 3a1 and 2e MOs. Other LCAO MOs are the same as the real MOs, suggesting high accuracy of MO theory. MO theory is useful in predicting the shapes and energies of the MOs, and hence the properties of the molecules.

Well noticed that there are differences between the real and LCAO Mos, to improve you could actually discuss further what the differences actually are. Smf115 (talk) 21:32, 17 May 2019 (BST)

NH3 molecule

Summary

Method and Basis Set: B3LYP/6-31G(d,p)

Summary Table of an optimised NH3 molecule.

Optimisation

         Item               Value     Threshold  Converged?
 Maximum Force            0.000100     0.000450     YES
 RMS     Force            0.000042     0.000300     YES
 Maximum Displacement     0.000344     0.001800     YES
 RMS     Displacement     0.000115     0.001200     YES

Link: File:ANGUS NH3 FREQ.LOG

Frequency Analysis

 Low frequencies ---  -33.0992  -33.0981  -12.4484   -0.0046    0.0113    0.0466
 Low frequencies --- 1088.6659 1694.0140 1694.0140

Rotatable 3d image of optimized NH3

NH3BH3 molecule

Summary

Method and Basis Set: B3LYP/6-31G(d,p)

Summary Table of an optimised NH3BH3 molecule.

Optimisation

         Item               Value     Threshold  Converged?
 Maximum Force            0.000157     0.000450     YES
 RMS     Force            0.000062     0.000300     YES
 Maximum Displacement     0.000554     0.001800     YES
 RMS     Displacement     0.000297     0.001200     YES

Link: File:ANGUS NH3BH3 FREQ.LOG

Frequency Analysis

Low frequencies ---   -0.0778   -0.0456   -0.0127   19.1319   19.2987   35.9786
Low frequencies ---  265.2495  633.0064  639.9688

Rotatable 3d image of optimized NH3BH3

Association Energies: Ammonia-Borane

Results and Calculations

From the Summary Tables of NH3, BH3 and NH3BH3, the energy are reported as follows:

Method and Basis Set: B3LYP/6-31G(d,p)

  • E(NH3)= -56.55777 a.u.
  • E(BH3)= -26.61532 a.u.
  • E(NH3BH3)= -83.22469 a.u.
  • ΔE=E(NH3BH3)-[E(NH3)+E(BH3)]
ΔE=[-83.22469-(-56.55777-26.61532)]a.u.
ΔE=-0.0516 a.u.
ΔE=-135 kJ/mol
  • The association energy of ammonia borane is -135 kJ/mol.
  • The association energy of a C-C bond is about -350 kJ/mol and the association energy of a C-H bond is about -410 kJ/mol.
  • The bond strength of B-N dative bond is three times weaker than that of C-C bond. As a conclusion, the B-N dative bond is weak.

Clear presentation of the energies, correct calculation and accuracy of the final reported answer. Your comparisons to evaluate the bond strength are good, you're just missing references for your literature values! Smf115 (talk) 21:31, 17 May 2019 (BST)

NI3 molecule

Summary

Method and Basis Set: RB3LYP/Gen

Summary Table of an optimised NI3 molecule.

Optimisation

Optimised N-I distance: 2.18363 Angstrom

      
        Item               Value     Threshold  Converged?
 Maximum Force            0.000063     0.000450     YES
 RMS     Force            0.000038     0.000300     YES
 Maximum Displacement     0.000476     0.001800     YES
 RMS     Displacement     0.000273     0.001200     YES

Link: File:ANGUS NI3 FREQ.LOG.log

Frequency Analysis

Low frequencies ---  -12.7347  -12.7286   -6.2858   -0.0040    0.0188    0.0634
Low frequencies ---  101.0320  101.0328  147.4111

Rotatable 3d image of optimized NI3

Project Section: Lewis acids and bases

Conformers and symmetries of Al2Cl4Br2

The five conformers of Al2Cl4Br2 and their point groups.


Clear presentation of the isomers and the correct assignment of the symmetries, you have repeated your C1 isomer though and have missed the one where the Br groups can be terminal of the same Al. Smf115 (talk) 08:02, 22 May 2019 (BST)

Isomer with 2 bridging Br ions

Summary

Method and Basis Set: RB3LYP/Gen

Summary Table of an optimised Isomer with 2 bridging Br ions.

Optimisation

      
         Item               Value     Threshold  Converged?
 Maximum Force            0.000029     0.000450     YES
 RMS     Force            0.000011     0.000300     YES
 Maximum Displacement     0.000230     0.001800     YES
 RMS     Displacement     0.000101     0.001200     YES

Link: File:Angus cis opt freq.gjf

Frequency Analysis

Low frequencies ---   -4.5023   -3.1305   -2.3662   -0.0045    0.0067    0.0106
Low frequencies ---   10.5714   65.1250   88.5355

Rotatable 3d image of isomer with 2 bridging Br ions

Isomer with trans terminal Br and bridging Cl ions

Summary

Method and Basis Set: RB3LYP/Gen

Summary Table of an optimised isomer with trans terminal Br and bridging Cl ions.

Optimisation

      
         Item               Value     Threshold  Converged?
 Maximum Force            0.000053     0.000450     YES
 RMS     Force            0.000019     0.000300     YES
 Maximum Displacement     0.000444     0.001800     YES
 RMS     Displacement     0.000170     0.001200     YES

Link: File:Angus trans opt freq.gjf

Frequency Analysis

Low frequencies ---   -4.9219   -3.1867   -0.0096    0.0060    0.0064    2.6066
Low frequencies ---   14.9013   52.1840   73.8329

Rotatable 3d image of isomer with trans terminal Br and bridging Cl ions

Good inclusion of all the necessary information about the structures and calculation and the energies imply that you correctly implemented the pseudopotential. However, the summary tables should be from the Frequency calculations and you are missing the corresponding frequency log files. The files submitted are input scripts and the D2h one, in particular, doesn't have the pseudopotential set up correctly. Smf115 (talk) 08:10, 22 May 2019 (BST)

Energy Analysis

Energies of conformers

  • Energy of isomer with 2 bridging Br ions: -2352.40631 a.u.
  • Energy of isomer with trans terminal Br and bridging Cl ions: -2352.41629 a.u.
  • Relative energy of these isomers: 0.00507 a.u. = 26 kJ/mol

Relative stability of the two isomers

  • From the energies of the isomers, it can be concluded that the isomer with 2 bridging Br ions is less stable as it has a higher energy. The isomer with trans terminal Br and bridging Cl ions has a lower energy and is more stable as the large and electron-rich Br are placed at terminal positions, therefore less electron repulsion than in bridging position. Also, more electronegative ligands increase tendancy to higher coordination numbers, which explain the relative stability of the two isomers.

Correct calculation, good accuracy of final energy value and nice justification of the relative stability! Just note, the complexes both have the same 'ligands' overall in terms of electronegativity so are actually equal in this respect. Smf115 (talk) 08:13, 22 May 2019 (BST)

AlCl2Br

Summary

Method and Basis Set: RB3LYP/Gen

Summary Table of an optimised AlCl2Br.

Optimisation

      
         Item               Value     Threshold  Converged?
 Maximum Force            0.000036     0.000450     YES
 RMS     Force            0.000023     0.000300     YES
 Maximum Displacement     0.000263     0.001800     YES
 RMS     Displacement     0.000154     0.001200     YES

Link: File:Angus Al opt freq.gjf.log

Frequency Analysis

Low frequencies ---   -3.2441   -0.0025   -0.0013    0.0005    0.7695    2.3428
Low frequencies ---  120.4978  133.8276  185.7207

Rotatable 3d image of AlCl2Br

Dissociation Energy for lowest energy conformer to AlCl2Br

  • E(AlCl2Br)= -1176.19014 a.u.
  • E(Al2Cl4Br2)= -2352.41629 a.u.
  • ΔE=-E(Al2Cl4Br2)+[2*E(AlCl2Br)]
ΔE=[2*-1176.19014-(-2352.41629)]a.u.
ΔE=0.03601 a.u.
ΔE=95 kJ/mol

Al2Cl4Br2 is more stable than the monomer as energy is needed to put in when breaking the Al-Br bonds. Also, it is easier to break a C-Br bond than a C-Cl bond due to poorer overlap of orbitals. Orbitals in Br are more diffused.

MO analysis on the lowest energy isomer

From the MO analysis of this conformer, there is a significant jump in energy from the core to the valence orbitals from MO30 to MO31. Therefore the MO 31 to MO59 (lowest 5 unoccupied MOs) were visualised and the following three MOs were chosen to do further analysis.


Clearly presented MOs using the two complementary screenshots and LCAOs. You've correctly identified the main interactions but there are a few mistakes, especially when evaluating the strength of the interaction e.g. the 'long-range weak antibonding' interaction between the two trans groups, the distance between them is so large that there is no evidential overlap. For the bottom two MOs, you also need to consider whether there is any contribution from the Al at all? Overall though, a good attempt at the analysis and evaluating the MO character. Smf115 (talk) 08:47, 22 May 2019 (BST)

A good report, well done! Smf115 (talk) 08:47, 22 May 2019 (BST)

Analysis of a highly bonding MO

MO40 Analysis of the lowest energy conformer of Al2Cl4Br2.

Analysis of a weakly bonding MO

MO41 Analysis of the lowest energy conformer of Al2Cl4Br2.

Analysis of a highly antibonding MO

MO43 Analysis of the lowest energy conformer of Al2Cl4Br2.