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NH3

Optimisation

Molecule: NH3

Calculation method: RB3LYP

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

E(RB3LYP) (au): -56.55777

RMS gradient (au): 0.00000323

Point group: C3V

N-H bond distance: 1.02Å

H-N-H bond angle: 105.7°

         Item               Value     Threshold  Converged?
 Maximum Force            0.000006     0.000450     YES
 RMS     Force            0.000004     0.000300     YES
 Maximum Displacement     0.000014     0.001800     YES
 RMS     Displacement     0.000009     0.001200     YES
Jmol dynamic image of NH3

The optimisation file is liked to here

Frequency Analysis

Display vibrations of NH3 molecule.


Wavenumber, Symmetry & Intensity of Each Vibration
wavenumber cm-1 1089 1694 1694 3461 3590 3590
symmetry A1 E E A1 E E
intensity arbitrary units 145 14 14 1 0 0
image





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

6


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

2 modes with frequency of 1694 cm-1 and 2 modes with frequency of 3590 cm-1


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

bending vibration: 1089 cm-1, 1694 cm-1, 1694 cm-1

bond stretch vibration: 3461 cm-1, 3590 cm-1, 3590 cm-1


Which mode is highly symmetric?

3461 cm-1 and 1089 cm-1


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

1089 cm-1


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

2. Theoretically there should be 4 bands due to 2 degenerate modes, but due to the low intensity of the bond stretch vibration (rel. intensity=1 and 0), 2 bond stretch bands cannot be seen in the experimental spectrum.

Charge Analysis

Charges on atoms
N-atom H-atoms image
-1.125 0.375

It is expected that N-atom should have a partially negative charge whereas H-atoms should have partially positive charges, because nitrogen is more electronegative than hydrogen so the electron density on N-atom is higher than the one on H-atoms.

N2

Optimisation

Molecule: N2

Calculation method: RB3LYP

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

E(RB3LYP) (au): -109.52413

RMS gradient (au): 0.00000060

Point group: Nh

N-N bond distance: 1.11Å

For lack of 3 atoms, the bond angle cannot be calculated.

         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
Jmol dynamic image of N2

The optimisation file is liked to here

Frequency Analysis

Display vibrations of N2 molecule.
Wavenumber, Symmetry & Intensity of Each Vibration
wavenumber cm-1 2457
symmetry SGG
intensity arbitrary units 0
image




Charge Analysis

Charges on atoms
N-atom N-atom
0.000 0.000

It is expected that the atoms should have no partial charge because 2 same atoms have the same elctronegativities.

H2

Optimisation

Molecule: H2

Calculation method: RB3LYP

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

E(RB3LYP) (au): -1.17854

RMS gradient (au): 0.00000017

Point group: Nh

H-H bond distance: 0.74Å

For lack of 3 atoms, the bond angle cannot be calculated.

          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
Jmol dynamic image of H2

The optimisation file is liked to here

Frequency Analysis

Display vibrations of H2 molecule.



Wavenumber, Symmetry & Intensity of Each Vibration
wavenumber cm-1 4466
symmetry SGG
intensity arbitrary units 0
image



Charge Analysis

Charges on atoms
H-atom H-atom
0.000 0.000

It is expected that the atoms should have no partial charge because 2 same atoms have the same elctronegativities.

Crystal Structure Comparison

Crystal Structure of Identifier: DOGNEU


The CDDC link to the molecule can be found at:[[1]]

The bond length (1.09Å) is slightly shorter the optimised one (1.11Å) due to the following reasons:

1. From the computational perspective, Gaussian calculates the bond length of the molecule in gas phase, while the experimental bond length is measured in the crystalline structure of the molecule; therefore, two bond lengths will be different.

2. From the experimental perspective, it can be seen from the 3D structure of this molecule that N≡N is a bit stretched and exposed to the outside of the whole molecule; so, due to packing effects of the crystal structure, the bond length may be shortened.

Haber-Bosch Process Energy Calculation

ENH3= -148492.43 kJ/mol

2*ENH3= -296984.86 kJ/mol

EN2= -287555.62 kJ/mol

EH2= -3094.26 kJ/mol

3*EH2= -9282.78 kJ/mol

ΔE=2*ENH3-[EN2+3*EH2]= -146.46 kJ/mol


Ammonia product is more stable than the reactants because the reaction is exothermic and releases energy (i.e. The energy of the reactants is greater than that of the product.).

[CN]-

Optimisation

Molecule: [CN]-

Calculation method: RB3LYP

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

E(RB3LYP) (au): -92.82453

RMS gradient (au): 0.00000704

Point group: Cv

C-N bond distance: 1.18Å

For lack of 3 atoms, the bond angle cannot be calculated.

         Item               Value     Threshold  Converged?
 Maximum Force            0.000012     0.000450     YES
 RMS     Force            0.000012     0.000300     YES
 Maximum Displacement     0.000005     0.001800     YES
 RMS     Displacement     0.000008     0.001200     YES
Jmol dynamic image of [CN]-

The optimisation file is liked to here

Frequency Analysis

Display vibrations of [CN]-.



Wavenumber, Symmetry & Intensity of Each Vibration
wavenumber cm-1 2139
symmetry SG
intensity arbitrary units 8
image

Charge Analysis

Charges on atoms
N-atom C-atom image
-0.754 -0.246

It is expected that N-atom should possess more negative charge than C-atom, for nitrogen is more electronegative than carbon. This charge distribution also converges with the overall charge being -1.

Molecular Orbitals

5 Molecular Orbitals of [CN]-
MO Energy/eV Description
-0.56195 This is an occupied s-p mixing bonding orbital contributed mainly by 2s AOs of C-atom and N-atom and partly by 2p AOs of C-atom and N-atom. The MO shape is not a perfect sphere and is slightly distorted due to s-p mixing. The energy is higher than the core orbitals (around -10 au), but is over 50 times deeper than the third and fourth MOs; therefore, although this is a valence orbital, it is relatively deep in energy, stabilised by s-p mixing interactions.
-0.10626 This is an occupied anti-bonding orbital contributed by 2p and 2s AOs of C-atom and N-atom. The MO shape is also slightly distorted due to s-p mixing. The energy is higher than the bonding orbital above, but is also stabilised by s-p mixing interactions.
-0.01696 This is an occupied π bonding orbital contributed by 2p AOs of C-atom and N-atom. The energy is almost non-negative (high in energy) and contributes to part of the triple bond in [CN]-
-0.01696 This is an occupied π bonding orbital contributed by 2p AOs of C-atom and N-atom. As the energies of this MO and the MO above are the same, these two MOs are degenerate, as there are 2 pairs of 2pAO interactions perpendicular to each other.
0.01857 This is an occupied s-p mixing bonding orbital contributed by 2p and 2s AOs of C-atom and N-atom resulting in a distorted shape of the MO. This MO is in the HOMO region, as it is the last occupied orbital in the MO diagram. The energy is positive (very high in energy), which indicates the reason why [CN]- is highly reactive and often used as a nucleophile. It is noticeable that the positive value indicates that [CN]- is very unstable and the electrons filled in this MO are unfavoured to stay in this orbital. However, experimentally [CN]- is relatively stable, which implies that the calculation method of cyanide ion may be not accurate enough.

Further Analysis

Crystal Structure of Identifier: DUNBIZ


The CDDC link to the molecule can be found at:[[2]]

The bond length (1.57Å) is much longer than the optimised one (1.18Å) probably due to the following reasons:

1. From the computational perspective, Gaussian calculates the bond length of the molecule in gas phase, while the experimental bond length is measured in the crystalline structure of the molecule; therefore, two bond lengths will be different.

2. From the experimental perspective, due to the strong interactions between gold and [CN]-, the π* orbital in [CN]-, for instance, may overlap with the dxy orbital in Au; however, backbonding may also exist when the dz2 overlaps with pz orbital in [CN]- due to symmetry, which may reduce the bond strength between Au and [CN]-.

It is interesting that although [CN]- and N2 are isoelctronic, but their bonding behaviour can be very different in different complexes.


Marking

Note: All grades and comments are provisional and subject to change until your grades are officially returned via blackboard. Please do not contact anyone about anything to do with the marking of this lab until you have received your grade from blackboard.

Wiki structure and presentation 1/1

Is your wiki page clear and easy to follow, with consistent formatting?

YES

Do you effectively use tables, figures and subheadings to communicate your work?

YES

NH3 1/1

Have you completed the calculation and given a link to the file?

YES

Have you included summary and item tables in your wiki?

YES

Have you included a 3d jmol file or an image of the finished structure?

YES

Have you included the bond lengths and angles asked for?

YES

Have you included the “display vibrations” table?

YES

Have you added a table to your wiki listing the wavenumber and intensity of each vibration?

YES

Did you do the optional extra of adding images of the vibrations?

YES

Have you included answers to the questions about vibrations and charges in the lab script?

YES

N2 and H2 0.5/0.5

Have you completed the calculations and included all relevant information? (summary, item table, structural information, jmol image, vibrations and charges)

YES

Crystal structure comparison 0.5/0.5

Have you included a link to a structure from the CCDC that includes a coordinated N2 or H2 molecule?

YES

Have you compared your optimised bond distance to the crystal structure bond distance?

YES

Haber-Bosch reaction energy calculation 0.5/1

Have you correctly calculated the energies asked for? ΔE=2*E(NH3)-[E(N2)+3*E(H2)]

YES

Have you reported your answers to the correct number of decimal places?

NO - Energies in kJ/mol should only be reported up to one decimal place.

Do your energies have the correct +/- sign?

YES

Have you answered the question, Identify which is more stable the gaseous reactants or the ammonia product?

YES

Your choice of small molecule 4/5

Have you completed the calculation and included all relevant information?

YES

Have you added information about MOs and charges on atoms?

YES

You could have discussed the calculated vibrational mode The second displayed MO is a bonding one rather than an anti-bonding. The last displayed MO is not only in the HOMO region, ti is the HOMO of CN-. You could have explained the energetic order of the MOs in more detail (number of nodes...).

Independence 1/1

If you have finished everything else and have spare time in the lab you could:

Check one of your results against the literature, or

YES

Do an extra calculation on another small molecule, or

Do some deeper analysis on your results so far