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Yr2Mod:j cos inorganic 2019

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Day 1

BH3 Borane link

B3LYP/6-31G(d,p)

Summary Table for BH3

Low frequencies and convergence:

 Low frequencies ---  -15.9849  -15.9818  -12.7207    0.0006    0.0143    0.3137
 Low frequencies --- 1162.9365 1213.1134 1213.1136


         Item               Value     Threshold  Converged?
 Maximum Force            0.000014     0.000450     YES
 RMS     Force            0.000007     0.000300     YES
 Maximum Displacement     0.000057     0.001800     YES
 RMS     Displacement     0.000028     0.001200     YES

Jmol:

BH3

Vibration analysis:

Vibration Modes for BH3



IR spectrum for BH3

Vibrational mode number IR Frequency (cm^-1) Type
1 92.5721 Symmetric out-of-plane bend
2 14.0532 Symmetric wag
3 14.0527 Asymmetric wag
4 0.0000 Symmetric stretch (inactive)
5 126.3274 Asymmetric stretch
6 126.3214 Asymmetric stretch
Answers to questions about vibrations

While the molecule has 6 vibrational modes, however only three peaks are visible in the IR spectrum. This is due to there being one non-degenerate IR-active mode (1), two pairs of denegerate IR-active modes (2&3, 5&6) and one IR-inactive mode (4.) (it is inactive due to having no change in dipole moment).

Correct reasons are given for the number of visible peaks but they could have been explained a bit better. There are some mistakes in the information reported (e.g. mix up between frequencies and IR intensity) and you haven't thought about the symmetry of the modes. Smf115 (talk) 08:09, 13 May 2019 (BST)

MO Diagram for BH3

Lecture_4_Tut_MO_diagram_BH3,http://www.huntresearchgroup.org.uk/teaching/teaching_comp_lab_year2a/Tut_MO_diagram_BH3.pdf, P.Hunt, accessed 03/05/2019

Answers to questions about MOs

As can be seen in this diagram, the qualitative MO diagram obtained by LCAO, is a close qualitative fit of the actual orbitals calculated computationally. While LCAO cannot give reliable numerical solutions, it can closely and accurately predict the electron distribution in real MOs.

NH3 Ammonia link

B3LYP/6-31G(d,p)

Summary Table for NH3

Low frequencies and convergence:

Low frequencies ---   -0.0131   -0.0028   -0.0019    7.0747    8.1044    8.1047
Low frequencies --- 1089.3849 1693.9369 1693.9369

        Item               Value     Threshold  Converged?
Maximum Force            0.000006     0.000450     YES
RMS     Force            0.000003     0.000300     YES
Maximum Displacement     0.000013     0.001800     YES
RMS     Displacement     0.000007     0.001200     YES

Jmol:

NH3

BH3NH3 link

B3LYP/6-31G(d,p)

Summary Table for BH3NH3

Low frequencies and convergence:

Low frequencies ---   -0.0006    0.0002    0.0010   16.8256   17.3871   37.9705
Low frequencies ---  265.9699  632.2062  639.3209

        Item               Value     Threshold  Converged?
Maximum Force            0.000006     0.000450     YES
RMS     Force            0.000003     0.000300     YES
Maximum Displacement     0.000013     0.001800     YES
RMS     Displacement     0.000007     0.001200     YES

Jmol:

BH3NH3

Energetic Calculations

ΔE = E[BH3NH3] - (E[BH3] + E[NH3])

-83.22468894 a.u. - (-26.61532364 a.u. + -56.55776873 a.u.) = -0.05159657 a.u

ans*2625.5 kJ/mol = -135 kJ/mol

Normal B-N bond energy is 389 kJ/mol, our B-N dative bond is weak.

Correct calculation, energy conversion and consideration of the accuracy of the final result. Good comparison but your literature value lacks a literature reference!Smf115 (talk) 08:12, 13 May 2019 (BST)

NI3 link

B3LYP/6-31G(d,p) ; pseudo-potential LANL2DZ

Summary Table for NI3

Low frequencies and convergence:

Low frequencies ---   -7.1402   -4.8083   -3.3178   -0.0004   -0.0003   -0.0001
Low frequencies ---  101.0869  101.1948  148.1919

        Item               Value     Threshold  Converged?
Maximum Force            0.000133     0.000450     YES
RMS     Force            0.000053     0.000300     YES
Maximum Displacement     0.001104     0.001800     YES
RMS     Displacement     0.000471     0.001200     YES

Jmol:

NI3

Optimised N-I distance

The optimised N-I distance was found to be 2.18293 Å.

Day 2 and 3 Mini-Project: Lewis Acids

The 5 possible isomers of Al2Cl4Br2. The point groups of each of these isomers are; in order D2h,C2h,C2v,C1,C2v
Energy Calculations

Comparing the energies of the two isomers of Al2Cl4Br2:

E[Al2Cl4Br2](Br bridge)= -571.43282350 a.u. E[Al2Cl4Br2](Br trans)= -571.43793017 a.u. The difference in energy between the two isomers is: 13 kJ/mol

The isomer with bridging Cl and trans terminal Br is lower in energy. Since Br has n quantum number n=4, it is large, and having the Br be terminal trans to each other minimises repulsion while having bridging Br maximises it, leading to higher energy.


Obtaining the dissociation energy of the Al2Cl4Br2</sub dimer:

ΔE = E[Al2Cl4Br2] - 2(E[AlCl2Br]) ΔE = -571.43793017 a.u. - 2(-285.70300109 a.u.)

ΔE = -0.003192799 a.u. ΔE = -0.003192799 a.u. * 2625.5 kJ/mol = -84 kJ/mol

Dissociation energy of this Dimer is 84 kJ/mol. Its dimer form is favoured with respect to its monomer form. Cl and Br are electronegative elements, thus, forming a dimer in which the most electronegative of the two, Cl (3.16 cf. 2.6) is bridging is favoured.

Good assignment of the symmetries to all 5 isomers. The calculations are in general good, however, you've calculated the association energy not dissociation and your energies are incorrect due to the incorrect pseudopotential input. Smf115 (talk) 08:16, 13 May 2019 (BST)

Al2Cl4Br2 with bridging Br link

GEN; N B3LYP/6-31G(d,p) , pseudo-potential Br Cl LANL2DZ

Summary table for Al2Cl4Br2


Low frequencies and convergence:

 Low frequencies ---   -1.1123    0.0001    0.0007    0.0007    1.0417    1.8073
 Low frequencies ---   16.1837   62.5427   84.8372

         Item               Value     Threshold  Converged?
 Maximum Force            0.000045     0.000450     YES
 RMS     Force            0.000020     0.000300     YES
 Maximum Displacement     0.001233     0.001800     YES
 RMS     Displacement     0.000523     0.001200     YES

Jmol:

Al2Cl4Br2

Al2Cl4Br2 with trans terminal Br and bridging Cl link

GEN; N B3LYP/6-31G(d,p) , pseudo-potential Br Cl LANL2DZ

Summary table for Al2Cl4Br2

Low frequencies and convergence:

 Low frequencies ---   -4.3978   -2.4768   -1.5835   -0.0010    0.0004    0.0007
 Low frequencies ---   18.6602   47.6012   71.2010

 Item               Value     Threshold  Converged?
 Maximum Force            0.000244     0.000450     YES
 RMS     Force            0.000084     0.000300     YES
 Maximum Displacement     0.002000     0.001800     NO 
 RMS     Displacement     0.000849     0.001200     YES

This output file shows that the Maximum Displacement has not converged; this is due to the fact that the basis set that we're using is not accurate enough for calculations of this molecule.
As Br is quite diffuse, the gradient of the maximum displacement is not close enough to zero.
In any case, this is to be expected considering the approximations that are being used, however the Maximum Displacement gradient is small enough that we can use these results.

Nice to see this awareness and addressing it in your report! Great to see the pseudopotential correctly implemented for Br, however, you weren't meant to include it on the Cl which is where the likely convergence issue has probably arisen. Smf115 (talk) 08:16, 13 May 2019 (BST)

Jmol:

Al2Cl4Br2

AlCl2Br Monomer link

GEN; N B3LYP/6-31G(d,p) , pseudo-potential Br Cl LANL2DZ

Summary table for AlCl2Br

Low frequencies and convergence:

 Low frequencies ---   -0.0009   -0.0009    0.0007    1.3337    2.3401    4.2420
 Low frequencies ---  119.7829  132.7164  182.6113

         Item               Value     Threshold  Converged?
 Maximum Force            0.000084     0.000450     YES
 RMS     Force            0.000033     0.000300     YES
 Maximum Displacement     0.001205     0.001800     YES
 RMS     Displacement     0.000690     0.001200     YES

Jmol:

AlCl2Br

MO analysis of lower energy isomer (trans terminal Br)

MO 17

MO 23

MO 31

Good range of MOs selected and you've evaluated the overall bonding/anti-bonding character well. Your LCAO diagrams are ok but there are a few mistakes, such as whether the Al contributes to the MO at all. Really good attempt at labelling some of the interactions and nodal planes, to improve though you've missed out quite a few interactions and the presentation of the annotations could be clearer .Smf115 (talk) 08:21, 13 May 2019 (BST)

Overall, good report and great effort across both sections, particularly all the structures and optimisation information is good. Smf115 (talk) 08:21, 13 May 2019 (BST)