Rep:Mod:klw14
Optimizing the NH3 Molecule, Frequency and NBO Charge
Optimisation
Method : B3LYP
Basis Set : 6-31G(d,p)
Results
Final Energy a.u. : -56.55776863
R.M.S Gradient : 0.00000478
Point Group : C3V
N-H Bond Distance : 1.01797 Å
H-N-H Bond Angle : 105.743 °
Item Value Threshold Converged? Maximum Force 0.000004 0.000450 YES RMS Force 0.000004 0.000300 YES Maximum Displacement 0.000071 0.001800 YES RMS Displacement 0.000034 0.001200 YES
NH |
Frequency Analysis
Using the 3N-6 rule for the expected number of vibrational modes
3*4-6=6
The number of computed vibrational modes is also 6. There are 2 sets of degenerate vibraitonal modes. One being with vibraitons of about 1695 cm-1 and those with vibrations at about 3590 cm-1 The bending modes of the molecule are those that occur at lower frequency, 1090 cm-1 and the degenerate modes at 1695 cm-1. The bond stretching modes are higher frequency, occuring at 3460 cm-1 and 3590 cm-1. The vibrational mode at 3460 cm-1 is the highly symmetric stretching mode and the vibration at 1090 cm-1 is the highly symmetric bending mode, sometimes referred to as the umbrella mode.
In an experimental gaseous vibrational spectra, 2 peaks would be expected. The vibration at 1090 cm-1 and the degenerate peaks at 1695 cm-1 will combine to give a single peak.
NBO Charge Analysis
N Charge = -1.125 H Charge = +0.375
As the nitrogen is more electronegative it is able to pull the electron density away from the Hydrogen atoms, leaving H atoms slightly positive and the Nitrogen with a negative charge.
The Haber-Bosch Procsee
To determine the most stable gasoues species within the Haber-Bosch process the reactants need to be calculated.
H2
The computational details are the same as those discussed for the NH3 molecule, so wont be repeated here.
Results
Final energy a.u. : -1.17853934
R.M.S. gradient : 0.00000017
Point Group :DinfH
H-H bond Distance
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
Frequency Analysis
This vibrational mode should not be visible in the gas phase IR.
NBO Charge Analysis
As the H2 is a homo-diatomic molecule there is no change in electron distribution to affect the charges on the Hydrogen atoms.
N2
The optimisation method and basis set is the same as for the NH3 and the H2 molecules.
Optimisation Results
Final energy a.u. : -109.52412907
R.M.S. gradient : 0.00000059
Point Group :DinfH
N-N bond distance
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
Frequency and NBO Charge Analysis
As was the case with Hydrogen, as this is a homo-diatomic molecule the vibrational mode will not appear in the gas phase IR spectra. The charge of the ions will also not change.
Calculating Energy for the Reaction
N2 + 3H2 --> 2NH3
All energy values in a.u.
E(NH3)= -56.55776863
2*E(NH3)= -113.11553726
E(N2)= -109.52412907
E(H2)= -1.17853934
3*E(H2)= -3.53561802
ΔE=2*E(NH3)-[E(N2)+3*E(H2)= -0.05579017
The ΔE value in kJ/mol is -140.89
As the ΔE value is negative, this shows that the products of the reaction (NH3) is the most stable species in the reaction.