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NH3 molecule

Information

Molecule name      Ammonia
Calculation Method RB3LYP
Basis set          6-31G(d.p)
Final energy       -56.55776873
RMS gradient       0.00000485
Point group        C3V
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

 N-H bond length 1.01798 Å 
 Bond angle is 37.129 degrees

Image of NH33 Molecule

File:PG1616 NH3 OPT POP.LOG

NH3 Molecule

Vibrations of Nh3

Questions

1. From the 3N-6 rule we expect there to be 6 vibrational nodes as there are 4 atoms in the ammonia molecule.
2. Vibrational modes that are degenerate are pairs  2 and 3 and 5 and 6.
3. Modes 1,2 and 3 are bending vibrations and modes 4,5 and 6 are stretching vibrations.
4. Mode 4 is highly symmetric
5.Mode 1 is known as the umbrella mode
6.You would expect to see 2 bands.


The charge on the N atom is -1.125 and the charge on the H atoms is 0.375. You would expect this as the nitrogen 
atom is more electronegative then the hydrogen atom and so would have an increased electron density surrounding it
 giving it a higher negative charge. The hydrogen has less electrons surrounding it but only one proton so has a small positive charge.

N2 molecule

Information

Molecule            Nitrogen
Calculation Method  RB3LYP
Basis set           6-31G(d.p)
Final energy        -109.52412868
RMS gradient        0.00000017
Point group          D*H
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
Bond length 1.1055 Å

Image of N2

File:PG1616 N2 OPT POP.LOG


N2 molecule

Vibrations of N2

This shows that the molecule is optimized because there are no negative vibrational energies.

H2 molecule

Information

Molecule            H<sub>2</sub>
Calculation Method  RB3LYP
Basis set           6-31G(d.p)
Final energy        -1.17853936
Point group          D*H
 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
Bond length 0.074279 Å

Image of H2 molecule

File:PG1616 H2 OPT POP.LOG

Hydrogen

Virbrations of H2

This shows that the molecule is fully optimized because there are no negative vibrational modes.

Reaction energies

E(NH3)= -56.55776873
2*E(NH3)= -113.115537
E(N2)= -109.52412868
E(H2)= -1.17853936
3*E(H2)= -3.53561808
ΔE=2*E(NH3)-[E(N2)+3*E(H2)]= -0.055791

This is -146.48 kj/mol, therefore the ammonia product is the most stable as the reaction is exothermic
so energy is released into the environment.. This figure is far off from one found in the literature* of -45.93kJ/mol this is due to the fact 
that they are measured under different conditions.

*J. Chem. Soc., Trans., 1903,83, 1168-1184
DOI: 10.1039/CT9038301168

F2

Information

Molecule            F<sub>2</sub>
Calculation Method  RB3LYP
Basis set           6-31G(d.p)
Final energy        -199.49825218
RMS gradient        0.00007365
Point group          D*H


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
Bond length 1.40281 Å. A literature value gives 1.417 Å. This is very close to the value obtained using Gaussian. 
http://www.wiredchemist.com/chemistry/data/fluorine-iodine-compounds

Image

File:PG1616 F2 OPT POP.LOG

Fluorine molecule

Vibrations

There a no negative vibrational energies which shows that the molecule is fully optimized.

Atomic Charges

There is no charge on either of the fluorine atoms as it is a homonuclear diatomic molecule 
and so share evenly the electrons in the compound.

Molecular Orbitals

This is the 1s non bonding molecular orbital, it is non bonding  because there is no overlap between the orbitals. The atomic orbitals are in phase and the orbital is so small it is 
found inside the fluorine atom. It is very deep in energy as they are core molecular orbitals.

This is the bonding sigma orbital. It is formed from the valence 2s atomic orbitals, these overlap more strongly and have a higher energy of -1.337 atomic units.
It is very much involved in chemical bonding as it is the valence shell.

This is the anti bonding sigma* orbital and it has a higher energy than the sigma orbital as the s atomic orbitals do not overlap. The energy difference between the bonding
and anti bonding orbital is greater than the 1s orbitals  because the molecules in the bonding orbital overlap more.

This is a sigma  bonding orbital made from atomic p orbitals overlapping along the bond.
Its has a higher energy than the s orbitals of -0.58753 atomic units.

This is the pi bonding molecular orbital made from p atomic orbitals perpendicular
to the plane of the bond.
All of above orbitals are occupied.