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NH3 Molecule

Optimised Structure

Ammonia molecule

N-H bond distance = 1.018 Å

H-N-H bond angle = 105.74 degrees

Molecule name: Ammonia (NH3)

Calculation method: RB3LYP

Basis Set: 6-31G(d,p)

Type of Calculation: FREQ

Final Energy: Energy=-56.55776873 a.u.

Point group: C3V

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

Ammonia optimisation log file

How many modes do you expect from the 3N-6 rule?

Ammonia is non-linear, so it will have 3N-6 vibrational modes. Expected number of modes = 3x4 - 6 = 12 - 6 = 6

Which modes are degenerate?

Modes 2&3 and modes 5&6

Which modes are bending vibrations and which are bond stretch vibrations?

Bending: 1,2,3

Stretching: 4,5,6

Which mode is highly symmetric?

1&4

Which is the umbrella mode?

1

How many bands would you expect to see in an experimental spectrum?

4 bands, as there are 2 degenerate pairs of modes.

Screenshot of Vibration Modes in Ammonia

Charge distribution of ammonia

Charge on N: -1.125

Charge on H: +0.375

As Nitrogen is more electronegative than Hydrogen, one would expect the Nitrogen to be negatively charged, and the Hydrogens positively charged. The overall charge of the molecule should add up to 0 as ammonia carries no formal charge.

Molecular Orbitals in Ammonia

File:Ammonia MO diagram.jpg
Ammonia MO diagram [1]

HOMO

Nitrogen is sp3 hybridised. The HOMO is its lone pair, that sits in an sp3 orbital which does not overlap with the Hydrogen 1s AOs. This orbital is occupied, but does not contribute to bonding.

LUMO

The LUMO in Ammonia is formed by the overlap of 3 Nitrogen sp3 orbitals with 3 out-of-phase Hydrogen 1s orbitals. It is an unoccupied antibonding molecular orbital.

N2 Molecule

Nitrogen molecule

Nitrogen optimisation log file

Point Group: D∞h

Molecule name: Nitrogen (N2)

Calculation method: RB3LYP

Basis Set: 6-31G(d,p)

Type of Calculation: FREQ

Final Energy: Energy= -109.52359111 a.u.

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
Screenshot of Vibrational Modes in Nitrogen.

This shows that there is only one active vibrational mode - which is what is expected for a diatomic molecule. The active mode is the symmetrical bond stretch.

Nitrogen charge distribution

Charge Distribution in Nitrogen.

As expected, the Nitrogen atoms are uncharged: N2 is a homodinuclear molecule and this is the predicted result.

Molecular orbitals in Nitrogen

HOMO

The HOMO in Nitrogen is the 3σg orbital formed by the overlap of two 2pz atomic orbitals. In Nitrogen, the 3σg MO is higher in energy than the 1πu orbital due to MO mixing with the 2σg (since they are of the same symmetry and similar energy, they are able to mix quite strongly).

LUMO

The LUMO in Nitrogen is the 1π*g orbital. Two such orbitals exist, that are degenerate: one MO is formed by the overlap of two 2px atomic orbitals, the other is formed by two 2py atomic orbitals. The picture below shows the 1π*g orbital formed by the 2px orbitals.

H2 Molecule

Hydrogen molecule

Hydrogen optimisation log file

Point Group: D∞h

Molecule name: Hydrogen (H2)

Calculation method: RB3LYP

Basis Set: 6-31G(d,p)

Type of Calculation: FREQ

Final Energy: Energy = -1.17853936 a.u.

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
Screenshot of Vibrational Modes in Hydrogen.

This shows that there is only one active vibrational mode - which is what is expected for a diatomic molecule. The active mode is the symmetrical bond stretch.

Charge distribution in Hydrogen

Charge Distribution in Hydrogen.

Molecular orbitals in Hydrogen

HOMO

The HOMO in Hydrogen is the 1σg orbital formed by the overlap of two in-phase 1s atomic orbitals.

LUMO

The LUMO in Hydrogen is the 1σ*u orbital, formed by the overlap of two out-of-phase 1s atomic orbitals.

Reaction energies

E(NH3)=-56.55776873 a.u. 2*E(NH3)=113.11553746

E(N2)=-109.52359111

E(H2)=-1.17853936

3*E(H2)=3.53561808

ΔE=2*E(NH3)-[E(N2+3*E(H2)]=-0.05632827 a.u.

ΔE=-147.89 kJ/mol

The Ammonia product is more stable.

My choice of small molecule: Cl2

Optimised structure

Chlorine molecule

Chlorine optimisation log file

Cl-CL Bond length: 2.04163 Å

Point Group: D∞h

Molecule name: Chlorine (Cl2)

Calculation method: RB3LYP

Calculation type: FREQ

Basis Set: 6-31G(d,p)

Type of Calculation: FREQ

Final Energy: Energy= -920.34987887 a.u.

Item table:

Item               Value     Threshold  Converged?
 Maximum Force            0.000007     0.000450     YES
 RMS     Force            0.000007     0.000300     YES
 Maximum Displacement     0.000018     0.001800     YES
 RMS     Displacement     0.000026     0.001200     YES

Charge Distribution of Chlorine

Charge Distribution of Chlorine.

Chlorine is a linear, homodinuclear molecule, so we would expect the chlorine atoms to be uncharged and the molecule to be neutral overall. This is indeed what we observe from the optimised structure.

Vibrations

Chlorine is a linear molecule. Using the 3n-5 rule, we would expect 1 mode of vibration. The optimised structure confirms this idea: there is one mode of vibration, at a frequency of 520.46 cm-1. This is the symmetric stretch, as shown in the animation below:

Molecular orbitals in Chlorine

The electron configuration of chlorine is 1s2 2s2 2p6 3s2 3p5. Each chlorine atom has 9 AOs, which overlap to form the 18 MOs in Cl2, the energies of which are shown below:

HOMO

The HOMO in Cl2 is a π* orbital formed by the overlap of two out-of-phase 3px or 3py orbitals. There are two such π* orbitals which are degenerate (MOs 16 and 17 in the picture above). The resultant antibonding orbital formed by the overlap of two out-of-phase 3py orbitals is shown below. These are both filled orbitals that contribute to antibonding in the chlorine molecule.

LUMO

The LUMO in Cl2 is a σ* orbital formed by the overlap of two out-of-phase 3pz orbitals. This MO corresponds to MO 18 in the list. It is the lowest energy unoccupied molecular orbital in chlorine.

π Bonding

Shown below is MO 15: the π bonding orbital formed from the overlap of two in-phase 3py orbitals. MO 14 is a degenerate π bonding orbital formed from the overlap of two in-phase 3px orbitals. It is an occupied orbital that contributes to the bonding in the chlorine molecule.

σ Bonding

MO 13 is a σ bonding orbital formed by the overlap of two in-phase 3pz orbitals. It is filled and lower in energy than the HOMO, contributing to the bonding in the chlorine molecule.

σ* Bonding

MO 12 is a σ* antibonding orbital formed by the overlap of two out-of-phase 3s orbitals. It is filled and lower in energy compared to the HOMO, contributing to the antibonding in the chlorine molecule.

Bibliography

  1. This MO Diagram was made in Photoshop by Wikimedia user Tem5psu, uploaded 31 December 2013, 14:00:25