Birdjo
Contents
- 1 Trimethylammonium Chloride
- 2 BH3 Molecule
- 3 NH3BH3 Molecule
- 4 Lab marking
- 5 NH3 molecule
- 6 Cis N2F2 molecule
Trimethylammonium Chloride
Calculation Data
| name of submitted log file | BH3 Opt.log |
| molecule | C3H10NCl |
| method | RB3LYP |
| basis set | 3-21G |
| final energy | -632.16208 |
| RMS gradient | 6.133e-06 |
| point group | C1 |
Convergence Data
Item Table
Item Value Threshold Converged? Maximum Force 0.000017 0.000450 YES RMS Force 0.000007 0.000300 YES Maximum Displacement 0.002004 0.001800 NO RMS Displacement 0.000651 0.001200 YES
=Low Frequencies
Low frequencies --- -5.4821 -2.3017 -0.0033 -0.0020 0.0020 7.2673 Low frequencies --- 55.7661 56.4186 189.8351
Optimised C3H10NCl LOG file
File:TRIMETHYLAMMONIUM CHLORIDE OPT.LOG
Optimised C3H10NCl Molecule
Jmol Rotatable Molecule
Optimised CHNCl Molecule |
BH3 Molecule
Calculation Data
| name of submitted log file | BH3 Opt.log |
| molecule | BH3 |
| method | RB3LYP |
| basis set | 6-31G(d,p) |
| final energy | -26.615324 |
| RMS gradient | 2.114e-06 |
| point group | D3H |
Convergence Data
Item Table
Item Value Threshold Converged? Maximum Force 0.000004 0.000015 YES RMS Force 0.000003 0.000010 YES Maximum Displacement 0.000017 0.000060 YES RMS Displacement 0.000011 0.000040 YES
Low Frequencies
Low frequencies --- -11.6940 -11.6861 -6.5543 0.0007 0.0280 0.4289 Low frequencies --- 1162.9745 1213.1390 1213.1392
Optimised BH3 Log File
Important Geometric Parameters
r(B-H)=1.19Â
θ (H-B-H)= 120°
Optimised BH3 Molecule
Jmol Rotatable Molecule
Optimised BH Molecule |
Infrared Info
| Mode | 1 | 2 | 3 | 4 | 5 | 6 |
| Wavenumber(cm-1) | 1163 | 1213 | 1213 | 2583 | 2716 | 2716 |
| Symmetry | A2 | E | E | A1 | E | E |
| Intensity (arbitrary units) | 93 | 14 | 14 | 0 | 126 | 126 |
Infrared Spectrum
NH3BH3 Molecule
| name of submitted log file | NH3BH3 opt2.log |
| molecule | NH3BH3 |
| method | RB3LYP |
| basis set | 6-31G(d,p) |
| final energy | -83.224689 |
| RMS gradient | 1.162e-06 |
| point group | C3V |
Convergence Data
Item Value Threshold Converged? Maximum Force 0.000002 0.000015 YES RMS Force 0.000001 0.000010 YES Maximum Displacement 0.000017 0.000060 YES RMS Displacement 0.000008 0.000040 YES
Low Frequencies
Low frequencies --- -5.4185 -0.3223 -0.0475 0.0010 1.1367 1.2199 Low frequencies --- 263.2927 632.9711 638.4651
Important Geometric Parameters
r(B-N)=1.67Â
r(B-H)=1.21Â
r(N-H)=1.02Â
θ (H-B-H)= 114°
θ (H-N-H)= 108°
Optimised NH3BH3
Jmol Rotatable Molecule
Optimised NHBH Molecule |
NH3BH3 Log File
Energies
E(NH3)= -26.615324 au E(BH3)= -56.557769 au E(NH3BH3)= -83.224689 au
Association Energy of NH3BH3
E= -0.051596 au E= -136 kJ/mol
Lab marking
You have a good working wiki. It would be good if you present your work more neatly and clearly. Overall, a good attempt. If you have any specific question, do email Prof. Hunt
NH3 molecule
Calculation Data
| name of submitted log file | JSDB_NH3OPT-POP.log |
| molecule | NH3 |
| method | RB3LYP |
| basis set | 6-31G(d,p) |
| final energy | -56.557769 |
| RMS gradient | 1.53e-07 |
| point group | C3v |
Convergence Data
Item Table
Item Value Threshold Converged? Maximum Force 0.000000 0.000015 YES RMS Force 0.000000 0.000010 YES Maximum Displacement 0.000003 0.000060 YES RMS Displacement 0.000001 0.000040 YES
Low Frequencies
Low frequencies --- -5.6864 -3.6131 -3.6124 0.0017 0.0048 0.0162 Low frequencies --- 1089.3674 1693.9284 1693.9284
Optimised NH3 Log File
Optimised NH3 Molecule
Optimised NH3 Molecule Rotatable Jmol
Important Geometric Parameters
r(N-H)=1.02Â
θ (H-N-H)= 106°
Infrared Information
| Mode | 1 | 2 | 3 | 4 | 5 | 6 |
| 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 |
Charge Distribution Data
| Atom | N | H |
| Charge | -1.13 | 0.38 |
Cis N2F2 molecule
Calculation Data
| name of submitted log file | birdjo_n2f2opt_pop.log |
| molecule | N2F2 |
| method | RB3LYP |
| basis set | 6-31G(d,p) |
| final energy | -309.01241 |
| RMS gradient | 3.17e-07 |
| point group | C2V |
Convergence Data
Item Table
Item Value Threshold Converged? Maximum Force 0.000001 0.000015 YES RMS Force 0.000000 0.000010 YES Maximum Displacement 0.000001 0.000060 YES RMS Displacement 0.000001 0.000040 YES
Low Frequencies
Low frequencies --- 0.0016 0.0018 0.0018 3.2233 4.3533 5.0998 Low frequencies --- 347.8772 561.2472 771.6105
Optimised N2F2 Log File
Optimised N2F2 Molecule
Why are there no bonds?
The reason there appears to be no bonds present is because Gaussview only represents bonds within a certain distance parameter. So the N-F bonds are in fact present; they are just not represented on the programme as they are outside this parameter.
Optimised N2F2 Molecule
Important Geometric Parameters
r(N-F)=1.22Â
r(N-F)=1.39Â
θ (F-N-N)=114°
θ (F-N-N-F)=0°
Infrared Information
Low frequencies --- 0.0016 0.0018 0.0018 3.2233 4.3533 5.0998 Low frequencies --- 347.8772 561.2472 771.6105
| Mode | 1 | 2 | 3 | 4 | 5 | 6 |
| Wavenumber(cm-1) | 348 | 561 | 772 | 949 | 987 | 1637 |
| Symmetry | A1 | A2 | B2 | A1 | B2 | A1 |
| Intensity (arbitrary units) | 1 | 0 | 75 | 75 | 81 | 21 |
Based on the 3N-6 rule we would expect to see 6 vibrational modes, so why do we only see 4 on the IR spectrum? Because mode 1 at 348cm-1 and mode 2 at 561cm-1 have essentially no absorption value so they are not present on the spectrum.
Which vibration is the asymmetric N-F stretch? The asymmetric N-F stretch is at 949cm-1.
What is the nature of the highest energy vibration? It is a symmetric stretch between the two N atoms.
Charge Distribution Data
| Atom | N | F |
| Charge | 0.22 | -0.22 |
Molecular Orbital Data
Which MOs are the core MOs?
MOs 1 and 2 are the core S orbitals for the Fluorine atoms MOs 3 and 4 are the core S orbitals for the Nitrogen atoms