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Introduction to Molecular Modelling

NH3

Analysis of ammonia
Component Result
Calculation method RB3LYP
Basis set 631-G(d.p)
Final energy in a.u. -56.5576873 a.u.
RMS gradient 0.00000485 a.u.
Point group C3v
Optimised NH bond length 1.01798 Å
Optimised H-N-H bond angle 105.741°

Item table:

         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 molecule

File:BDAVIES NH3 OPTIMISATION.LOG

Vibration Analysis

Number of modes expected from the 3N-6 rule 6
Degenerate modes #5 and #6, and #2 and #3
Bending vibrations #1, #2 and #3
Bond stretch vibrations #4, #5 and #6
Highly symmetric mode #4
Umbrella mode #1
Bands expected in an experimental spectrum of gaseous ammonia 2

Charge Analysis

Charge on N atom = -1.125

Charge on H atom = 0.035

I would expect a positive charge on the H atoms and a negative charge on the N atom due to nitrogen being more electronegative than hydrogen and attracting more of the electron density in the N-H bond.

N2

Analysis of N2
Component Result
Calculation method RB3LYP
Basis set 631-G(d.p)
Final energy in a.u. -109.52412868 a.u.
RMS gradient 0.00000060 a.u.
Point group D(inf)H
Optimised N-N bond length 1.10550 Å

Item table:

         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

File:BDAVIES N2 OPTIMISATION.LOG

N2 molecule

There is only one vibrational frequency: 2457.33 cm-1

H2

Analysis of H2
Component Result
Calculation method RB3LYP
Basis set 631-G(d.p)
Final energy in a.u. -1.17853936 a.u.
RMS gradient 0.00000017 a.u.
Point group D(inf)H
Optimised H-H bond length 0.74279 Å

Item table:

         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

File:BDAVIES H2 OPTIMISATION.LOG

H2 molecule

There is also only one vibrational frequency for H2: 4465.68 cm-1

Energies for the Haber-Bosch Process

E(NH3) = -56.5576873 a.u.

2*E(NH3) = -113.1153746 a.u.

E(N2) = -109.52412868 a.u.

E(H2) = -1.17853936 a.u.

3*E(H2) = -3.53561808 a.u.

ΔE = 2*E(NH3)-[E(N2)+3*E(H2)] = -0.05562784 a.u. = -146.0508939 kJ/mol

Literature value for ΔE ~-50 kJ/mol(Prezhdo, 2016).

The ammonia product is more stable than the gaseous reactants.

Citation

Prezhdo, V. V. (2016). Haber Process Made Efficient by Hydroxylated Graphene: Ab Initio. The Journal of Physical Chemistry Letters.

Chosen molecule: F2

Analysis of F2
Component Result
Calculation method RB3LYP
Basis set 631-G(d.p)
Final energy in a.u. -199.49825218 a.u.
RMS gradient 0.00007365 a.u.
Point group D(inf)H
Optimised F-F bond length 1.40281 Å

Item table:

         Item               Value     Threshold  Converged?
 Maximum Force            0.000128     0.000450     YES
 RMS     Force            0.000128     0.000300     YES
 Maximum Displacement     0.000156     0.001800     YES
 RMS     Displacement     0.000221     0.001200     YES

File:BDAVIES F2 OPTIMISATION.LOG

F2 molecule

There is one vibrational frequency: 1065.09 cm-1. It is a stretch vibration. I would expect to see one band in the gaseous spectrum of flourine, corresponding to its one vibrational frequency.

There is 0 charge on each F atom, because it is a single-element molecule: therefore the electrons in the covalent bond are distributed equally.

P orbital A

Energy = -0.58753 a.u.

This is the occupied δ bonding orbital. It is formed with two Pz atomic orbitals, one from each flourine atom.

p orbital A in F2.

P orbitals B and C

Energy = -0.52332 a.u. These are the occupied bonding pi orbitals. They are formed with one px and one py atomic orbital from each flourine atom.

p orbital B in F2.
p orbital C in F2.

P orbitals D and E

Energy = -0.39190 a.u. These are the occupied anti-bonding pi orbitals. They are also formed with one px and one py atomic orbital from each flourine atom. These are the HOMOs.

The LUMO is the unoccupied δ* orbital, not shown here.

P orbital D in F2.
p orbital E in F2.