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Rep:Mod:KL

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Using Gaussian to optimise molecules

NH3 Molecule

Properties

Pre-optimised NH3 molecule

The NH3 molecule on the left was optimised using a B3LYP method and a 6-31G(d,p) basis set with the following steps:


Molecule Name Ammonia (NH3)
Calculation Method RB3LYP
Basis set 6-31G(d,p)
E(RB3LYP) -56.5577687 a.u
Point Group C3V
Optimised N-H bond length 1.01798Å
Optimised N-H bond angle 105.741°

Link to the optimisation file

         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 

Vibrational modes

Table of different vibrational frequencies.
NHmolecule



The number of vibrational modes expected using the 3N-6 rule is 6. Referring to the table of vibrational frequencies, modes 2 and 3 are degenerate with eachother and so are modes 5 and 6. Modes 1,2 and 3 are bending modes and modes 4,5 and 6 are stretching modes. Mode 4 is a highly symmetric mode. The umbrella mode is mode 1. There would be 4 bands in the spectrum due to the degeneracy of modes 2 and 3 and modes 5 and 6. This leaves 4 distinct vibrational frequencies at which ammonia absorbs electromagnetic radiation.

Charge Distributions

A diagram to show how the charge is distributed in an NH3 molecule.

I would expect there to be a negative charge on the nitrogen atom and positive charges on the hydrogen atoms as nitrogen is the more electronegative of the two.

Reactivity

Nitrogen

An optimised nitrogen (N2) molecule.

Link to the optimisation file

There is only one vibrational mode in this diatmomic molecule with an intensity of 0 because there is no overall dipole shift.


Molecule Name Nitrogen (N2)
Calculation Method RB3LYP
Basis set 6-31G(d,p)
E(RB3LYP) -109.52359111 a.u
Point Group D*H
Optimised N-N bond length 1.10550Å
Optimised N-H 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 
N molecule

Hydrogen

Link to the optimisation file

An optimised model of the hydrogen molecule
Molecule Name Hydrogen (H2)
Calculation Method RB3LYP
Basis set 6-31G(d,p)
E(RB3LYP) -1.17853936 a.u
Point Group D*H
Optimised N-N bond length 0.74279Å
Optimised N-H bond angle 180°
The table shows there is only one vibration mode for the linear molecule and this value in IR is 0.00 as therer is no overall dipole shift because both atoms are the same.
Hmolecule


 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 
E(NH3) -56.5577687 a.u
2*E(NH3) =-113.1155374 a.u
E(N2) -109.52359111 a.u
E(H2) -1.17853936 a.u
3*E(H2) -3.53561808 a.u
ΔE=2*E(NH3)-[E(N2)+3*E(H2)] -0.05579070 a.u
ΔE -146.48kJ/mol

The energy of the reaction is a negative value indicating that the gaseous product, ammonia, is the more stable than the gaseous reactants.

N2 Molecular Orbitals

ClF3

Properties

An optimised ClF3 molecule.

Link to the optimisation file

Molecule Name Chlorine Trifluoride (ClF3)
Calculation Method RB3LYP
Basis set 6-31G(d,p)
E(RB3LYP) -759.46531682 a.u
Point Group C2V
Optimised Cl-F bond length(short bond) 1.65143 Å
Optimised Cl-F bond length (long) 1.72863 Å
Optimised F-Cl-F bond angle (small angle) 87.140°
Optimised F-Cl-F bond angle (large angle) 174.281°
Item               Value     Threshold  Converged?
 Maximum Force            0.000050     0.000450     YES
 RMS     Force            0.000028     0.000300     YES
 Maximum Displacement     0.000204     0.001800     YES
 RMS     Displacement     0.000134     0.001200     YES 

Vibrational Modes

A table showing the frequencies and the IR values of the vibrations in the molecule

The number of vibrational modes expected using the 3N-6 rule is 6. Referring to the table of vibrational frequencies,none of the modes are degenerate and in the IR spectrum I would expect to find 4 bands as two would overlap being very similar in frequency (modes 1 and 2).

Hmolecule
A digram showing the charge distribution in the molecule.

Molecular Orbitals

As the 3 fluorine atoms together have 21 electrons which is a higher number than the chlorine which has only 17, the d orbitals in the chlorine are able to be occupied. This is because when the atomic orbitals combine, the resulting bonding molecular orbitals will be lower in energy than some of the antibonding orbitals.

All the molecular orbitals are occupied.