Jump to content

Rep:Mod:01188090

From ChemWiki

BH3

        Item               Value     Threshold  Converged?
Maximum Force            0.000047     0.000450     YES
RMS     Force            0.000023     0.000300     YES
Maximum Displacement     0.000183     0.001800     YES
RMS     Displacement     0.000092     0.001200     YES


Frequency analysis log file MAD_BH3_FREQ.LOG

Smf115 (talk) 08:21, 17 May 2018 (BST)Links to the required log files are broken throughout for each structure.

Low frequencies ---   -0.4059   -0.1955   -0.0054   25.3481   27.3325  27.3356
Low frequencies --- 1163.1913 1213.3139 1213.3166
BH3
Summary of IR absorptions and they're respective symmetries
wavenumber (cm-1) intensity (arbitrary units) symmetry IR active? type
1163 93 A1 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
IR spectrum for BH3

There are less than 6 peaks in the IR spectrum, despite the presence of 6 vibrational modes in the table as not all the modes lead to an overall change in dipole moment. For a mode to be IR active, there needs to be a change in dipole moment across the molecule, and when a molecule of BH3 symmetrically stretches, all three bonds stretch at the same time, thus the dipole moment of the molecule doesn't change.

Molecular orbital diagram for BH3

Molecular Orbaital (MO) diagram of BH3 with estimated MOs and computer generated MOs.2

The MOs generated computationally do not differ significantly from the LCAO MOs, showing that qualitative MO theory can be used as a reasonably accurate way of predicting the shapes of MOs.

NH3

        Item               Value     Threshold  Converged?
Maximum Force            0.000006     0.000450     YES
RMS     Force            0.000004     0.000300     YES
Maximum Displacement     0.000014     0.001800     YES
RMS     Displacement     0.000009     0.001200     YES

Frequency analysis log file MAD_NH3_FREQ.LOG

Low frequencies ---  -11.6527  -11.6490   -0.0045    0.0333    0.1312   25.5724
Low frequencies --- 1089.6616 1694.1736 1694.1736
NH3

NH3BH3

        Item               Value     Threshold  Converged?
Maximum Force            0.000153     0.000450     YES
RMS     Force            0.000033     0.000300     YES
Maximum Displacement     0.000465     0.001800     YES
RMS     Displacement     0.000241     0.001200     YES

Frequency analysis log file MAD_NH3BH3_FREQ.LOG

Low frequencies ---   -0.1516   -0.0504   -0.0205   11.4593   17.9090   18.0876
Low frequencies ---  263.1437  631.4267  638.8923


NH3BH3

E(NH3) = -56.55776873 au E(BH3) = -26.61532362 au E(NH3BH3) = -83.22469115 au

ΔE = (E(NH3)+E(BH3)) - E(NH3BH3) =(-56.558 + -26.615) - (-83.224) = 0.051 au =130 ± 10 kJ mol-1 (lit. 130.1 ± 4.2 kJ mol-1)1

Upon comparison with a literature value for the dissociation energy of a normal B-H bond (377.9 ± 8.7 kJ mol-1)1, it is shown that the bond energy calculated for a dative B-N bond is relatively weak in comparison.

BBr3

        Item               Value     Threshold  Converged?
Maximum Force            0.000012     0.000450     YES
RMS     Force            0.000006     0.000300     YES
Maximum Displacement     0.000056     0.001800     YES
RMS     Displacement     0.000028     0.001200     YES


Low frequencies ---   -0.0132   -0.0064   -0.0046    2.5123    2.5124    4.8831
Low frequencies ---  155.9619  155.9639  267.6983
BBr3

Frequency analysis log file Mad_BBr3_freq_opt_pp5.log

DOI:10042/202295

Benzene C6H6

        Item               Value     Threshold  Converged?
Maximum Force            0.000202     0.000450     YES
RMS     Force            0.000090     0.000300     YES
Maximum Displacement     0.000769     0.001800     YES
RMS     Displacement     0.000326     0.001200     YES

Frequency analysis log data MAD_BENZENE_FREQ.LOG

Low frequencies ---   -2.5530   -2.5530   -0.0088   -0.0041   -0.0039   10.3930
Low frequencies ---  413.9723  413.9723  621.1358
Benzene

Borazine B3H6N3

        Item               Value     Threshold  Converged?
Maximum Force            0.000093     0.000450     YES
RMS     Force            0.000027     0.000300     YES
Maximum Displacement     0.000241     0.001800     YES
RMS     Displacement     0.000099     0.001200     YES

Frequency analysis data MAD_BORAZINE_FREQ.LOG

Low frequencies ---  -10.7286  -10.4463  -10.2311   -0.0104   -0.0093    0.0981
Low frequencies ---  289.0927  289.1014  403.7381
Borazine

Benzene vs. Borazine

Charge distribution comparison

Charge distribution for borazine
Charge distribution for benzene

Benzene shows a uniform charge density across the six carbon atoms due to the high symmetry that benzene possesses. The six carbon atoms in benzene have a charge of -0.239 and the six hydrogen atoms have a charge of 0.239. As the hydrogen atoms are attached to more electronegative carbon atoms, the carbon atoms will have a higher electron density as the electrons are drawn more towards the carbon atoms. In borazine, the six-membered ring is comprised of alternating boron and nitrogen atoms, and has less symmetry in comparison to benzene. Nitrogen has a higher electronegativity than boron, therefore there is higher electron density on the nitrogen atoms in comparison with the boron atoms. This is shown through the respective charges calculated, 0.747 for boron and -1.103 for nitrogen. The hydrogen atoms bonded to boron have a higher electron density than those attached to nitrogen atoms, as those attached to nitrogen are attached to the more electronegative atom, and as a result the electron density will be pulled away from hydrogen and onto nitrogen. In comparison, the boron atoms are not as electron withdrawing, thus the hydrogen atoms attached to boron will have a higher electron density in comparison with those attached to nitrogen.


Smf115 (talk) 08:21, 17 May 2018 (BST)Good charge anaysis with considertion to both symmetry and electronegativities of the atoms.

Molecular orbital comparison

caption
Benzene Borazine Discussion
In benzene, the orbital is symmetrical across all six carbon atoms. In borazine, the MO has a similar shape, however on closer inspection, it can be seen that the orbitals are slightly more diffuse over the boron atoms as the boron is more electropositive. The nitrogen atoms draw in electron density a lot more, therefore the orbital is not as diffuse over the nitrogen atoms. This pair of MOs is bonding and comprised mainly of sigma-orbitals.
In benzene, the molecular orbital is symmetrical across all six carbon atoms. In borazine, the molecular orbital is slightly more diffuse over the boron atoms in comparison with the nitrogen atoms. These molecular orbitals are also bonding orbitals, however they are comprised of p orbitals and show pi-character, as shown by the nodal planes in the planes of the molecules.
In benzene, the molecular orbital is highly symmetrical, due to the high symmetry that benzene possesses. In borazine, the molecular orbital shows more character over the boron atoms than over the nitrogen atoms. Boron is more electropositive and as a result, boron's atomic orbitals have a higher relative energy than those for nitrogen. The chosen molecular orbital is antibonding, and as a result will be more diffuse over the boron atoms than over the nitrogen atoms.

Aromaticity

It is generally accepted that there are 4 criteria that need to be fulfilled in order to describe a molecule as aromatic: the molecule must be cyclic, the molecule must be planar, the molecule must have fully conjugated p orbitals on every atom in the system and the molecule must have 4n+2 pi electrons.3

However these rules can be called into contention with a few examples. Firstly the simple model commonly used to portray aromatic compounds of overlapping pz atomic orbitals is not an accurate description of aromaticity in aromatic compounds. Although these overlapping orbitals form a molecular orbital in benzene, this is only one of many molecular orbitals that arise. Other molecular orbitals involve combinations of p and s atomic orbitals combining to give other molecular orbitals. Furthermore, in cases such as borazine where the cyclic system is comprised of heteroatoms, the polarity differences between the heteroatoms is not taken account in the given rules and as a result, this leads to molecular orbitals with less symmetry, than for those in benzene.

A further observation made that can discredit the above set of rules for aromaticity is that not all aromatic molecules are in fact planar. Good examples of systems that show aromatic characteristics but which are not planar are para- and meta- cyclophanes.4 Even at very low temperatures, benzene is observed to adopt a chair conformation instead of a planar conformation due to strong intermolecular forces present when crystal lattices form.4

Smf115 (talk) 08:16, 17 May 2018 (BST)Good references to examples which contradict the planar concept for aromaticity. Further discussion and consideration towards MOs and how the concept of overlapping pZ AOs is a bad descriptor of aromaticity would have improved the answer.

Smf115 (talk) 08:20, 17 May 2018 (BST)Overall a decent and well presented wiki report.

References

[1] - https://notendur.hi.is/agust/rannsoknir/papers/2010-91-CRC-BDEs-Tables.pdf

[2] - http://www.huntresearchgroup.org.uk/teaching/teaching_comp_lab_year2a/Tut_MO_diagram_BH3.pdf

[3] - Clayden Organic chemistry

[4] - https://onlinelibrary.wiley.com/doi/epdf/10.1002/chem.200700250