Rep:Mod:CET2016
NH3 molecule
NH3 optimisation
| Property | value |
|---|---|
| Calculation method | RB3LYP |
| Basis set | 6-31G(d,p) |
| Final energy E(RB3LYP) | -56.55776873 au |
| RMS gradient | 0.00000485 au |
| Point group | C3v |
| Bond length | 1.01798 |
| Bond angle | 105.741 |
Optimization results
Item Value Threshold Converged? Maximum Force 0.000004 0.000450 YES RMS Force 0.000004 0.000300 YES Maximum Displacement 0.000072 0.001800 YES RMS Displacement 0.000035 0.001200 YES
NH3 |
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Vibrations

For NH3, following the 3N-6 rule, 6 vibrational modes would be expected. These include, symmetrical stretching, asymmetrical stretching, scissoring (bending), rocking, wagging and twisting. From our table, vibrations 2 and 3, and 5 and 6 are degenerate. Vibrations 1,2, and 3 are bending, and 4, 5, and 6 are stretching. Vibrational mode 4 is highly symmetric. Mode 1 is known as the "umbrella" mode, as it looks like an inversion. As an IR of gaseous ammonia, you would expect 4 peaks, however, the last peak would have a very small intensity (~0.2711) and is negligible.
Charge analysis

In NH3, the nitrogen adopts a negative charge of -1.125, and hydrogen has a charge of +0.375. The nitrogen has a negative charge because it is more electronegative so draws the bonding electrons towards it to make the charge density negative. Nitrogen also has a lone pair of electrons, making it more negative. As the bonding electrons are drawn away from the hydrogen atoms, these adopt a positive charge. The net charge of the molecule is zero, as the positive hydrogen charge cancels out the negative charge on nitrogen. The molecule is not ionised.
N2 optimisation
| Property | value |
|---|---|
| Calculation method | RB3LYP |
| Basis set | 6-31G(d,p) |
| Final energy E(RB3LYP) | -109.52412868 au |
| RMS gradient | 0.00000060 au |
| Point group | D*H |
| Bond length | 1.10550 |
| Bond angle | 180 |
Item Value Threshold Converged? Maximum Force 0.000001 0.000450 YES RMS Force 0.000001 0.000300 YES Maximum Displacement 0.000000 0.001800 YES RMS Displacement 0.000000 0.001200 YES
There is only one vibrational frequency for N2, which is a stretch at frequency of 2457.33 cm^-1. However, the intensity is 0, so this peak will not show on an IR spectra. N2 is IR inactive.
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H2 optimisation
| Property | value |
|---|---|
| Calculation method | RB3LYP |
| Basis set | 6-31G(d,p) |
| Final energy E(RB3LYP) | -1.17853936 au |
| RMS gradient | 0.00000017 au |
| Point group | D*H |
| Bond length | 0.74729 |
| Bond angle | 180 |
Item Value Threshold Converged? Maximum Force 0.000000 0.000450 YES RMS Force 0.000000 0.000300 YES Maximum Displacement 0.000000 0.001800 YES RMS Displacement 0.000001 0.001200 YES
There is only one vibrational frequency for H2, which is a stretch at frequency of 4465.68 cm^-1. However, the intensity is 0, so this peak will not show on an IR spectra. H2 is IR inactive.
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Haber-Bosch process
N2 + 3H2 -> 2NH3
E(NH3)= -56.55776873 au
2*E(NH3)= -113.1155375 au
E(N2)= -109.52412868 au
E(H2)= -1.17853936 au
3*E(H2)= -3.53591808 au
ΔE=2*E(NH3)-[E(N2)+3*E(H2)]= -0.05549074 au = -145.6909489681 kJ/mol
The ammonia products are more stable as they have a more negative enthalpy than the reactants [1][2].
Project molecule CN-
| Property | value |
|---|---|
| Calculation method | RB3LYP |
| Basis set | 6-31G(d,p) |
| Final energy E(RB3LYP) | -92.82453153 au |
| RMS gradient | 0.00000704 au |
| Point group | C*v |
| Bond length | 1.18409 |
| Bond angle | 180 |
Item Value Threshold Converged? Maximum Force 0.000012 0.000450 YES RMS Force 0.000012 0.000300 YES Maximum Displacement 0.000005 0.001800 YES RMS Displacement 0.000008 0.001200 YES
CN molecule |
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Vibrations

There is one vibrational mode at 2139.19cm^-1, with an intensity of 7.7521. This is a bond stretch. There are no negative frequencies.
Charge Analysis

In the CN- molecule, the nitrogen atom adopts a charge of -0.750, and the carbon atom adopts a charge of -0.250. The overall charge of the atom is -1, and the substituent charges on the atoms add up to this value. The nitrogen has a more negative value because it is the more electronegative atom, so draws the bonding electrons and hence negative charge towards it. However, as the molecule is negative, there is still negative charges that reside on the carbon.
Molecular orbitals




