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Rep:Mod:VN3944

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BH3

B3LYP/6-31G level


       Item               Value     Threshold  Converged?
Maximum Force            0.000190     0.000450     YES
RMS     Force            0.000095     0.000300     YES
Maximum Displacement     0.000747     0.001800     YES
RMS     Displacement     0.000374     0.001200     YES


Optimisation log file: logfile

Frequency analysis log file: logfile

Low frequencies ---   -0.2260   -0.1035   -0.0054   48.0278   49.0875   49.0880
Low frequencies --- 1163.7224 1213.6715 1213.6741
Optimised BH3

IR analysis

IR spectrum of BH3
IR analysis
Freq (cm-1 Mode IR active? Intensity
1163 Wag YES Strong
1213 Bend YES Weak
1213 Bend YES Weak
2579 Symm Stretch NO No peak
2712 Asymm Stretch YES Strong
2712 Asymm Stretch YES Strong

Only three peaks can be observed in the IR because two of the vibrational modes are degenerate in energy (1213 and 2712 cm-1) and the symmetric stretch at 2579 cm-1 is not IR active.

Ng611 (talk) 17:47, 17 May 2018 (BST) Good analysis -- remember to report the intensities of the various modes too

MO diagram


Ng611 (talk) 17:49, 17 May 2018 (BST) Good MO analysis. From comparing the calculated and qualitative MOs, are there any differences at all between them, and what does this tell you about qualitative MO theory?

Association Energy: ammonia-borane

NH3

       Item               Value     Threshold  Converged?
Maximum Force            0.000006     0.000450     YES
RMS     Force            0.000004     0.000300     YES
Maximum Displacement     0.000012     0.001800     YES
RMS     Displacement     0.000008     0.001200     YES

Optimisation output file: File

Frequency analysis: File

Low frequencies ---   -8.5646   -8.5588   -0.0041    0.0455    0.1784   26.4183
Low frequencies --- 1089.7603 1694.1865 1694.1865

BH3-NH3

        Item               Value     Threshold  Converged?
Maximum Force            0.000233     0.000450     YES
RMS     Force            0.000083     0.000300     YES
Maximum Displacement     0.000981     0.001800     YES
RMS     Displacement     0.000370     0.001200     YES

Output of optimisaton: File

Frequency analysis: File

Low frequencies ---   -0.1144   -0.1063   -0.0333   15.1196   15.2002   38.3644
Low frequencies ---  265.8918  634.5284  639.3073

Calculation of Association Energy

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)]= -0.0516 a.u. = -135.47 kJ/mol

The dissociation energy will therefore be 135.47 kJ/mol.

Based on these calculations, the Nitrogen-Boron dative bond can be considered quite strong. A C-C bond, in fact, has a dissociation energy of about 154 kJ/mol.

Ng611 (talk) 19:38, 15 May 2018 (BST) Remember to round your figures to the nearest Kj/mol and to include specific literature references for any numbers you provide.

BBr3

The optimisation and the frequency analysis were both carried out using the SCAN server. DOI:10.14469/ch/198191 Link of the file on DSpace: click here

Optimisation logfile: logfile

Frequency analysis log file: logfile

The basis set used for B was 6-31G(d,p) and for Br(LanL2DZ).

        Item               Value     Threshold  Converged?
Maximum Force            0.000008     0.000450     YES
RMS     Force            0.000004     0.000300     YES
Maximum Displacement     0.000036     0.001800     YES
RMS     Displacement     0.000018     0.001200     YES
Low frequencies ---   -0.0137   -0.0064   -0.0046    2.4315    2.4315    4.8421
Low frequencies ---  155.9631  155.9651  267.7052

Main group halides

Isomers

Isomers of AL2Cl4Br2 and respective point groups.

The C2h and the D2h isomers were analysed. The former was found to be the lowest energy isomer, as it can be seen in the summary tables below.

Summaries

The basis set used for Al and Cl was 6-31G(d,p) and for Br(LanL2DZ)

Logfile of first isomer: log

Logfile of second isomer: log

Item table of first isomer:

        Item               Value     Threshold  Converged?
Maximum Force            0.000039     0.000450     YES
RMS     Force            0.000014     0.000300     YES
Maximum Displacement     0.001573     0.001800     YES
RMS     Displacement     0.000748     0.001200     YES

Item table of second isomer:

        Item               Value     Threshold  Converged?
Maximum Force            0.000026     0.000450     YES
RMS     Force            0.000010     0.000300     YES
Maximum Displacement     0.001036     0.001800     YES
RMS     Displacement     0.000354     0.001200     YES
Optimised First Isomer

The energy of the first isomer is -6176269.44 kJ/mol, whereas for the second isomer it is -6176243.26 kJ/mol.

Summary of optimisation of monomer

Logfile of the monomer: log

Item table of the monomer:

       Item               Value     Threshold  Converged?
Maximum Force            0.000040     0.000450     YES
RMS     Force            0.000025     0.000300     YES
Maximum Displacement     0.000283     0.001800     YES
RMS     Displacement     0.000165     0.001200     YES

Relative stability

The isomer with two bridging Cl atoms is more stable than the isomer with Br bridging atoms because there is a better overlap in the three-center bond, and less steric hindrance.

Ng611 (talk) 19:41, 15 May 2018 (BST) A calculation demonstrating the change in relative energies of these two molecules would have improved this section significantly.

Dissociation energy

The monomer has an energy of -1176.19012 a.u. and the dissociation energy of the first isomer can be calculated with the equation:

ΔE=E(Al2Cl4Br2 (trans))-[2*E(AlCl2Br)]=-6176269.44 - [2(-3088087.42)]= -94.6 kJ/mol

The dissociation energy will therefore be 94.6 kJ/mol. The product is found to be more stable than the single monomers and this is the force that drives the association of the monomers.

Ng611 (talk) 19:42, 15 May 2018 (BST) Remember to round your results!

Molecular orbitals and LCAO

The MOs of the lowest energy isomer were visualised. The LCAO analysis of three of these MOs can be seen below.

In MO40 there is a good overlap between the p orbitals on Cl and Br and the p orbitals of the Al atoms. Also, there is a good p-p overlap between the Al atoms and the bridging Cl atoms. MO54 has an intermediate character because the thrgough-space interactions are not strong enough to make it a full antibonding orbital. The overlap is not good. MO60 has a strong antibonding character because there is a strong thorugh-bond interaction between the p orbitals on the bridging Cl atoms and the Al atoms, and also a quite strong antibonding interaction between the p orbitals on the terminal groups and the Al p orbitals.

Ng611 (talk) 19:49, 15 May 2018 (BST) A good analysis here. For your second entry in the table, describing an orbital as being of 'intermediate' character doesn't tell us anything. Other LCAO decompositions and analyses were good though.


Ng611 (talk) 19:49, 15 May 2018 (BST) Overall a good report. You missed out a number of marks by reporting figures to too high an accuracy value (remember, DFT results are only accurate to about 1kJ/mol, and potentially even less accurate than that). YOur section on LCAO and bonding was very good.