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Rep:MOD:mjr116

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NH3

Molecule: NH3

Calulation Method: RB3LYP

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

Final Energy E(RB3LYP) in au: -56.55776873

RMS Gradient: 0.00000485

Point Group: C3V

N-H Bond Distance: 1.01798

H-N-H Bond Angle: 105.741

   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


The optimisation file is linked to here


test molecule

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

12

which modes are degenerate (ie have the same energy)?

2 and 3 5 and 6

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

1 - bending 2 - bending 3 - bending 4 - stretch 5 - stretch 6 - stetch

which mode is highly symmetric?

4

one mode is known as the "umbrella" mode, which one is this?

1

how many bands would you expect to see in an experimental spectrum of gaseous ammonia?

6

N - atom charge: -1.125 H - atom charge: 0.375

N2

Molecule: N2

Calculation Method: RB3LYP

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

Final energy E(RB3LYP) in au: -109.52412868

RMS gradient: 0.00000365

Point Group: D*H

N-N bond length: 1.10550

Item               Value     Threshold  Converged?
 Maximum Force            0.000006     0.000450     YES
 RMS     Force            0.000006     0.000300     YES
 Maximum Displacement     0.000002     0.001800     YES
 RMS     Displacement     0.000003     0.001200     YES

Frequencies: 2457.31

The optimisation file is linked to here


test molecule


H2

Molecule: H2

Calculation Method: RB3LYP

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

E(RB3LYP): -1.09691172

RMS Gradient: 0.05487992

Point Group: D*H

Item               Value     Threshold  Converged?
 Maximum Force            0.000211     0.000450     YES
 RMS     Force            0.000211     0.000300     YES
 Maximum Displacement     0.000278     0.001800     YES
 RMS     Displacement     0.000393     0.001200     YES
 


The optimisation file is linked to here


test molecule


Energy for the reaction

N2 + 3H2 -> 2NH3

E(NH3)= -56.55776873

2*E(NH3)= -113.11553746

E(N2)= -109.52412868

E(H2)= -1.09691172

3*E(H2)= -3.29073516

ΔE=2*E(NH3)-[E(N2)+3*E(H2)]= -113.11553746 - (-109.52412868 + -3.29073516) = -0.30067362


Energy for converting hydrogen and nitrogen gas into ammonia gas in kJ/mol = -789.418649445

The ammonia product is therefore more stable.

F2

Molecule: F2

Calculation Method: RB3LYP

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

E(RB3LYP): -199.48874381

RMS Gradient: 0.06248728

Point Group: D*H

Item               Value     Threshold  Converged?
 Maximum Force            0.000250     0.000450     YES
 RMS     Force            0.000250     0.000300     YES
 Maximum Displacement     0.000308     0.001800     YES
 RMS     Displacement     0.000435     0.001200     YES

The optimisation file is linked to here



test molecule

Frequency 1063.53

Charge: 0.0000



Orbitals

This is the 2σ_g F2 orbital. One electron from each of the 2s atomic orbitals on the Fluorine atoms combine in-phase to make the 2σ_g molecular orbital. This molecular is an occupied orbital and it is a bonding MO. The electron density is spread between the two atoms and therefore this MO will have a stabilising effect on the bonding between the two F atoms.


This is the 2σ_u* orbital. Two electrons contribute to this molecular orbital, one from each of the 2s atomic orbitals of the fluorine atoms. This is an occupied molecular orbital and it is a result of the out of phase combination of orbitals, therefore this is an antibonding molecular orbital. This reduces the stability of the bond between the F atoms as the electron density is over the atoms but there is a node (gap) between the two atoms of lower electron density.

This is the 3σ_g F2 molecular orbital. It is the result of the in-phase combination of the 2p orbitals on the fluorine atoms, therefore this is an occupied bonding MO. The electron density is in between the two nuclei therefore this MO contributes to the stability of the bonding.


This is the 1π_u F2 molecular orbital. It is the result of in-phase combination of the 2p orbitals, and is therefore an occupied bonding MO which contributes to the stability of the molecule.

This is the 1π_g* F2 molecular orbital. It is an anti-bonding orbital resulting from the out of phase combination of the 2p atomic orbitals. This is the HOMO (Highest Occupied Molecular Orbital) of the F¬2 molecule.

This is the 3σ_u* F2 molecular orbital. It is an anti-bonding MO resulting from the out of phase combination of the 2p atomic orbitals of the fluorine atoms. It is the LUMO (Lowest Unoccupied Molecular Orbital) of the F2 molecule.