Rep:Mod:haien910
NH3
test molecule |
NH3 is a colorless gas with a characteristic pungent smell. Fritz Haber and Carl Bosch developed the Haber–Bosch process in 1909 to produce ammonia from the nitrogen in the air.
Calculation Method | RB3LYP |
Basis Set | 6-31G(d.p) |
Final Energy | -56.55776873 a.u., -148492.43 kJ/mol |
RMS Gradient Norm | 0.00000485 a.u. |
Point Group | C3V |
Optimised N-H bond distance = 1.01798 Å
Optimised H-N-H bond angle = 105.741°
Optimisation Table
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 Predicted change in Energy=-5.986281D-10 Optimization completed. -- Stationary point found. ---------------------------- ! Optimized Parameters ! ! (Angstroms and Degrees) ! -------------------------- -------------------------- ! Name Definition Value Derivative Info. ! -------------------------------------------------------------------------------- ! R1 R(1,2) 1.018 -DE/DX = 0.0 ! ! R2 R(1,3) 1.018 -DE/DX = 0.0 ! ! R3 R(1,4) 1.018 -DE/DX = 0.0 ! ! A1 A(2,1,3) 105.7412 -DE/DX = 0.0 ! ! A2 A(2,1,4) 105.7412 -DE/DX = 0.0 ! ! A3 A(3,1,4) 105.7412 -DE/DX = 0.0 ! ! D1 D(2,1,4,3) -111.8571 -DE/DX = 0.0 ! --------------------------------------------------------------------------------
Vibrational Modes of NH3
Since NH3 is a non-linear molecule, using the rule 3N-6 where N = 4, we would expect it to have 6 vibrational modes. This is correctly predicted by the Gaussview software.
Degenerate orbitals are orbitals that have the same energy. Modes 2 & 3 are degenerate to each other whereas 5 & 6 are degenerate to each other. This is deduced by looking at their frequencies; if they're degenerate, they would have equivalent frequencies. Modes 1, 2 and 3 are bending modes whereas 4, 5 and 6 are stretching modes.
Mode 4 is highly symmetric and Mode 1 is known as the 'umbrella' mode.
Charge distribution on N = - 1.125
Charge distribution on H = + 0.375
N is more electronegative than H, it has a higher tendency to attract a bonding pair of electrons and so there is a partial negative charge on N atom and a partial positive charge on H atom. The magnitude of charge of N atom about 3 times greater than of H atom because there is only 1 N for every 3 H.
IR Spectrum of NH3
2 peaks were observed and this is due to the 2 degenerate pairs (2 & 3 and 5 & 6). Mode 4 is a symmetric stretch, it has no change in dipole moment therefore is IR inactive. It is worth noting that intramolecular interaction like hydrogen bonding between NH3 was not detected by Gaussview.
H2
test molecule |
Calculation Method | RB3LYP |
Basis Set | 6-31G(d.p) |
Final Energy | -1.17853936 a.u., -3094.26 kJ/mol |
RMS Gradient Norm | 0.00000017 a.u. |
Point Group | D∞H |
Bond Length | 0.74279 Å |
H2 does have any charge distribution because there is no difference in electronegativity values.
Optimisation Table
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 Predicted change in Energy=-1.164080D-13 Optimization completed. -- Stationary point found. ---------------------------- ! Optimized Parameters ! ! (Angstroms and Degrees) ! -------------------------- -------------------------- ! Name Definition Value Derivative Info. ! -------------------------------------------------------------------------------- ! R1 R(1,2) 0.7428 -DE/DX = 0.0 ! --------------------------------------------------------------------------------
Vibrational Modes of H2
H2 is a linear molecule, using the rule 3N-5 where N = 2, we would expect it to only have 1 vibrational mode.
IR Spectrum of H2
H2 has no net change in dipole moment, so it is IR inactive, therefore no peaks were observed on IR spectrum.
N2
test molecule |
Calculation Method | RB3LYP |
Basis Set | 6-31G(d.p) |
Final Energy | -109.52412868 a.u., -287555.62 kJ/mol |
RMS Gradient Norm | 0.00000060 a.u. |
Point Group | D∞H |
Bond Length | 1.10550 Å |
N2 does have any charge distribution because there is no difference in electronegativity values.
Optimisation Table
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 Predicted change in Energy=-3.401020D-13 Optimization completed. -- Stationary point found. ---------------------------- ! Optimized Parameters ! ! (Angstroms and Degrees) ! -------------------------- -------------------------- ! Name Definition Value Derivative Info. ! -------------------------------------------------------------------------------- ! R1 R(1,2) 1.1055 -DE/DX = 0.0 ! --------------------------------------------------------------------------------
Vibrational Modes of N2
N2 is a linear molecule, using the rule 3N-5 where N = 2, we would expect it to only have 1 vibrational mode.
IR Spectrum of H2
N2 has no net change in dipole moment, so it is IR inactive, therefore no peaks were observed on IR spectrum.
Thermodynamics of Haber Process
E(NH3) = -148492.43 kJ/mol
2*E(NH3) = -296984.86 kJ/mol
E(N2) = -287555.62 kJ/mol
E(H2) = -3094.26 kJ/mol
3*E(H2) = -9282.78 kJ/mol
ΔE = 2*E(NH3) - [E(N2) + 3*E(H2)] = -146.46 kJ/mol
The Haber Process is an exothermic reaction. However, the literature value is quoted to be -45.940 kJ/mol so our value is greatly deviated. [1]
- ↑ Klemola, K., Chemical Reaction Equilibrium Calculation Task For ChE Undergraduates–Simulating Fritz Haber’s Ammonia Synthesis With Thermodynamic Software. Chemical Engineering Education, 48(2), pp.115-120
HCl
test molecule |
Calculation Method | RB3LYP |
Basis Set | 6-31G(d.p) |
Final Energy | -460.80077875 a.u. |
RMS Gradient Norm | 0.00005211 a.u. |
Point Group | C∞V |
Bond Length | 1.10550 Å |
Charge distribution on H = + 0.284
Charge distribution on Cl = - 0.284
Chlorine atom is more electronegative than Hydrogen atom thus has a higher tendency of attracting a pair of bonding electrons.
Optimisation Table
Item Value Threshold Converged? Maximum Force 0.000090 0.000450 YES RMS Force 0.000090 0.000300 YES Maximum Displacement 0.000139 0.001800 YES RMS Displacement 0.000197 0.001200 YES Predicted change in Energy=-1.256951D-08 Optimization completed. -- Stationary point found. ---------------------------- ! Optimized Parameters ! ! (Angstroms and Degrees) ! -------------------------- -------------------------- ! Name Definition Value Derivative Info. ! -------------------------------------------------------------------------------- ! R1 R(1,2) 1.286 -DE/DX = 0.0001 ! --------------------------------------------------------------------------------
Vibrational Modes of HCl
HCl is a linear molecule, using the rule 3N-5 where N = 2, we would expect it to only have 1 vibrational mode.
IR Spectrum of HCl
HCl has a change in dipole moment therefore it is IR active. It only has one peak as predicted and it is a stretching frequency at around 2957 cm-1.
Molecular Orbital Analysis of HCl
The Cl electrons residing up to 3s orbitals (1s, 2s, 2px, 2py, 2pz, 3s) are largely stabilised than the electron in 1s orbital of H atom, therefore they cannot mix and form bond. The 3p electron in Cl atom has similar energy to 1s electron in H atom therefore they can mix. However, due to the different symmetries of 3px and 3py orbitals compared to that of 1s orbital, the only possible mixing is σ overlap between 1s orbital of H atom and 3pz orbital of Cl atom. Both of these orbitals are half-filled thus are allowed to form a bond.
The bond order of HCl is 1 because there are 2 electrons in the bonding orbital but none in the non-bonding orbital.

Molecular Coefficient Table of HCl
1 2 3 4 5 O O O O O Eigenvalues -- -101.55786 -9.47437 -7.23847 -7.22836 -7.22836 1 1 Cl 1S 0.99600 -0.28467 -0.00189 0.00000 0.00000 2 2S 0.01517 1.02220 0.00687 0.00000 0.00000 3 2PX 0.00000 0.00000 0.00000 0.99117 0.00000 4 2PY 0.00000 0.00000 0.00000 0.00000 0.99117 5 2PZ -0.00004 -0.00630 0.99047 0.00000 0.00000 6 3S -0.02109 0.07379 0.00034 0.00000 0.00000 7 3PX 0.00000 0.00000 0.00000 0.02799 0.00000 8 3PY 0.00000 0.00000 0.00000 0.00000 0.02799 9 3PZ -0.00002 -0.00120 0.03045 0.00000 0.00000 10 4S 0.00171 -0.01358 0.00215 0.00000 0.00000 11 4PX 0.00000 0.00000 0.00000 -0.00736 0.00000 12 4PY 0.00000 0.00000 0.00000 0.00000 -0.00736 13 4PZ -0.00010 0.00178 -0.00945 0.00000 0.00000 14 5XX 0.00757 -0.01669 0.00002 0.00000 0.00000 15 5YY 0.00757 -0.01669 0.00002 0.00000 0.00000 16 5ZZ 0.00765 -0.01573 -0.00228 0.00000 0.00000 17 5XY 0.00000 0.00000 0.00000 0.00000 0.00000 18 5XZ 0.00000 0.00000 0.00000 -0.00048 0.00000 19 5YZ 0.00000 0.00000 0.00000 0.00000 -0.00048 20 2 H 1S 0.00005 -0.00124 0.00256 0.00000 0.00000 21 2S -0.00022 0.00300 -0.00359 0.00000 0.00000 22 3PX 0.00000 0.00000 0.00000 -0.00039 0.00000 23 3PY 0.00000 0.00000 0.00000 0.00000 -0.00039 24 3PZ -0.00014 -0.00052 0.00180 0.00000 0.00000 6 7 8 9 10 O O O O V Eigenvalues -- -0.84773 -0.47433 -0.33163 -0.33163 0.01366 1 1 Cl 1S 0.08094 0.02733 0.00000 0.00000 -0.02450 2 2S -0.36382 -0.12619 0.00000 0.00000 0.10936 3 2PX 0.00000 0.00000 -0.28537 0.00000 0.00000 4 2PY 0.00000 0.00000 0.00000 -0.28537 0.00000 5 2PZ 0.04545 -0.23220 0.00000 0.00000 -0.16897 6 3S 0.73327 0.26260 0.00000 0.00000 -0.26941 7 3PX 0.00000 0.00000 0.73004 0.00000 0.00000 8 3PY 0.00000 0.00000 0.00000 0.73004 0.00000 9 3PZ -0.10755 0.57863 0.00000 0.00000 0.46375 10 4S 0.27021 0.24735 0.00000 0.00000 -0.72409 11 4PX 0.00000 0.00000 0.40430 0.00000 0.00000 12 4PY 0.00000 0.00000 0.00000 0.40430 0.00000 13 4PZ -0.01216 0.16969 0.00000 0.00000 0.87011 14 5XX -0.02029 0.01824 0.00000 0.00000 -0.04398 15 5YY -0.02029 0.01824 0.00000 0.00000 -0.04398 16 5ZZ 0.02127 -0.05761 0.00000 0.00000 0.10073 17 5XY 0.00000 0.00000 0.00000 0.00000 0.00000 18 5XZ 0.00000 0.00000 -0.01866 0.00000 0.00000 19 5YZ 0.00000 0.00000 0.00000 -0.01866 0.00000 20 2 H 1S 0.15662 -0.28655 0.00000 0.00000 0.24914 21 2S 0.04977 -0.24977 0.00000 0.00000 1.50879 22 3PX 0.00000 0.00000 0.01771 0.00000 0.00000 23 3PY 0.00000 0.00000 0.00000 0.01771 0.00000 24 3PZ 0.01666 -0.01719 0.00000 0.00000 -0.01235 11 12 13 14 15 V V V V V Eigenvalues -- 0.36800 0.40255 0.43685 0.43685 0.68586 1 1 Cl 1S -0.05961 -0.02916 0.00000 0.00000 0.03175 2 2S 0.04945 0.06099 0.00000 0.00000 -0.03265 3 2PX 0.00000 0.00000 0.30181 0.00000 0.00000 4 2PY 0.00000 0.00000 0.00000 0.30181 0.00000 5 2PZ -0.01321 0.23797 0.00000 0.00000 0.18170 6 3S -1.26542 -0.52542 0.00000 0.00000 0.69879 7 3PX 0.00000 0.00000 -1.16096 0.00000 0.00000 8 3PY 0.00000 0.00000 0.00000 -1.16096 0.00000 9 3PZ 0.11244 -0.94335 0.00000 0.00000 -0.68364 10 4S 1.96653 0.54265 0.00000 0.00000 -1.77015 11 4PX 0.00000 0.00000 1.23592 0.00000 0.00000 12 4PY 0.00000 0.00000 0.00000 1.23592 0.00000 13 4PZ -0.65815 1.18628 0.00000 0.00000 1.39906 14 5XX 0.01785 -0.10153 0.00000 0.00000 0.22144 15 5YY 0.01785 -0.10153 0.00000 0.00000 0.22144 16 5ZZ -0.34080 0.11877 0.00000 0.00000 -0.36870 17 5XY 0.00000 0.00000 0.00000 0.00000 0.00000 18 5XZ 0.00000 0.00000 0.01458 0.00000 0.00000 19 5YZ 0.00000 0.00000 0.00000 0.01458 0.00000 20 2 H 1S -0.37113 0.25587 0.00000 0.00000 -0.86140 21 2S -0.41553 -0.05089 0.00000 0.00000 2.18749 22 3PX 0.00000 0.00000 -0.00153 0.00000 0.00000 23 3PY 0.00000 0.00000 0.00000 -0.00153 0.00000 24 3PZ -0.04561 0.04911 0.00000 0.00000 0.01578 16 17 18 19 20 V V V V V Eigenvalues -- 0.80005 0.80005 0.86468 0.86468 1.16034 1 1 Cl 1S 0.00000 0.00000 0.00000 0.00000 0.00066 2 2S 0.00000 0.00000 0.00000 0.00000 0.03128 3 2PX 0.00000 -0.01332 0.00000 0.00000 0.00000 4 2PY -0.01332 0.00000 0.00000 0.00000 0.00000 5 2PZ 0.00000 0.00000 0.00000 0.00000 -0.01614 6 3S 0.00000 0.00000 0.00000 0.00000 0.07339 7 3PX 0.00000 0.03860 0.00000 0.00000 0.00000 8 3PY 0.03860 0.00000 0.00000 0.00000 0.00000 9 3PZ 0.00000 0.00000 0.00000 0.00000 -0.00125 10 4S 0.00000 0.00000 0.00000 0.00000 -0.17360 11 4PX 0.00000 0.01600 0.00000 0.00000 0.00000 12 4PY 0.01600 0.00000 0.00000 0.00000 0.00000 13 4PZ 0.00000 0.00000 0.00000 0.00000 0.24726 14 5XX 0.00000 0.00000 0.86603 0.00000 0.46825 15 5YY 0.00000 0.00000 -0.86603 0.00000 0.46825 16 5ZZ 0.00000 0.00000 0.00000 0.00000 -0.82390 17 5XY 0.00000 0.00000 0.00000 1.00000 0.00000 18 5XZ 0.00000 0.95574 0.00000 0.00000 0.00000 19 5YZ 0.95574 0.00000 0.00000 0.00000 0.00000 20 2 H 1S 0.00000 0.00000 0.00000 0.00000 0.92285 21 2S 0.00000 0.00000 0.00000 0.00000 -0.40892 22 3PX 0.00000 -0.17261 0.00000 0.00000 0.00000 23 3PY -0.17261 0.00000 0.00000 0.00000 0.00000 24 3PZ 0.00000 0.00000 0.00000 0.00000 -0.15003 21 22 23 24 V V V V Eigenvalues -- 2.05856 2.05856 2.75279 4.27800 1 1 Cl 1S 0.00000 0.00000 -0.02965 0.16933 2 2S 0.00000 0.00000 0.15175 -0.79433 3 2PX 0.00000 0.01699 0.00000 0.00000 4 2PY 0.01699 0.00000 0.00000 0.00000 5 2PZ 0.00000 0.00000 -0.14494 -0.03702 6 3S 0.00000 0.00000 -0.56866 5.51631 7 3PX 0.00000 -0.02940 0.00000 0.00000 8 3PY -0.02940 0.00000 0.00000 0.00000 9 3PZ 0.00000 0.00000 0.58914 0.15492 10 4S 0.00000 0.00000 -0.52879 0.10829 11 4PX 0.00000 -0.15059 0.00000 0.00000 12 4PY -0.15059 0.00000 0.00000 0.00000 13 4PZ 0.00000 0.00000 0.26345 -0.05395 14 5XX 0.00000 0.00000 0.47810 -2.41449 15 5YY 0.00000 0.00000 0.47810 -2.41449 16 5ZZ 0.00000 0.00000 -0.47857 -2.60306 17 5XY 0.00000 0.00000 0.00000 0.00000 18 5XZ 0.00000 0.34228 0.00000 0.00000 19 5YZ 0.34228 0.00000 0.00000 0.00000 20 2 H 1S 0.00000 0.00000 0.27323 0.13310 21 2S 0.00000 0.00000 0.64729 -0.07000 22 3PX 0.00000 1.01311 0.00000 0.00000 23 3PY 1.01311 0.00000 0.00000 0.00000 24 3PZ 0.00000 0.00000 1.23461 0.27943 Density Matrix: 1 2 3 4 5 1 1 Cl 1S 2.16070 2 2S -0.61758 2.38693 3 2PX 0.00000 0.00000 2.12770 4 2PY 0.00000 0.00000 0.00000 2.12770 5 2PZ -0.00558 0.02626 0.00000 0.00000 2.07410 6 3S 0.04903 -0.44960 0.00000 0.00000 -0.05556 7 3PX 0.00000 0.00000 -0.36119 0.00000 0.00000 8 3PY 0.00000 0.00000 0.00000 -0.36119 0.00000 9 3PZ 0.01475 -0.06982 0.00000 0.00000 -0.21815 10 4S 0.06840 -0.28673 0.00000 0.00000 -0.08588 11 4PX 0.00000 0.00000 -0.24535 0.00000 0.00000 12 4PY 0.00000 0.00000 0.00000 -0.24535 0.00000 13 4PZ 0.00613 -0.03048 0.00000 0.00000 -0.09866 14 5XX 0.02229 -0.02373 0.00000 0.00000 -0.01006 15 5YY 0.02229 -0.02373 0.00000 0.00000 -0.01006 16 5ZZ 0.02449 -0.03288 0.00000 0.00000 0.02438 17 5XY 0.00000 0.00000 0.00000 0.00000 0.00000 18 5XZ 0.00000 0.00000 0.00970 0.00000 0.00000 19 5YZ 0.00000 0.00000 0.00000 0.00970 0.00000 20 2 H 1S 0.01049 -0.04413 0.00000 0.00000 0.15240 21 2S -0.00772 0.03290 0.00000 0.00000 0.11337 22 3PX 0.00000 0.00000 -0.01088 0.00000 0.00000 23 3PY 0.00000 0.00000 0.00000 -0.01088 0.00000 24 3PZ 0.00176 -0.00884 0.00000 0.00000 0.01307 6 7 8 9 10 6 3S 1.22508 7 3PX 0.00000 1.06750 8 3PY 0.00000 0.00000 1.06750 9 3PZ 0.14602 0.00000 0.00000 0.69461 10 4S 0.52411 0.00000 0.00000 0.22828 0.26877 11 4PX 0.00000 0.58991 0.00000 0.00000 0.00000 12 4PY 0.00000 0.00000 0.58991 0.00000 0.00000 13 4PZ 0.07155 0.00000 0.00000 0.19841 0.07728 14 5XX -0.02296 0.00000 0.00000 0.02551 -0.00146 15 5YY -0.02296 0.00000 0.00000 0.02551 -0.00146 16 5ZZ -0.00172 0.00000 0.00000 -0.07134 -0.01656 17 5XY 0.00000 0.00000 0.00000 0.00000 0.00000 18 5XZ 0.00000 -0.02727 0.00000 0.00000 0.00000 19 5YZ 0.00000 0.00000 -0.02727 0.00000 0.00000 20 2 H 1S 0.07901 0.00000 0.00000 -0.36515 -0.05707 21 2S -0.05774 0.00000 0.00000 -0.29997 -0.09676 22 3PX 0.00000 0.02584 0.00000 0.00000 0.00000 23 3PY 0.00000 0.00000 0.02584 0.00000 0.00000 24 3PZ 0.01534 0.00000 0.00000 -0.02336 0.00052 11 12 13 14 15 11 4PX 0.32703 12 4PY 0.00000 0.32703 13 4PZ 0.00000 0.00000 0.05807 14 5XX 0.00000 0.00000 0.00662 0.00216 15 5YY 0.00000 0.00000 0.00662 0.00216 0.00216 16 5ZZ 0.00000 0.00000 -0.02008 -0.00232 -0.00232 17 5XY 0.00000 0.00000 0.00000 0.00000 0.00000 18 5XZ -0.01508 0.00000 0.00000 0.00000 0.00000 19 5YZ 0.00000 -0.01508 0.00000 0.00000 0.00000 20 2 H 1S 0.00000 0.00000 -0.10111 -0.01677 -0.01677 21 2S 0.00000 0.00000 -0.08590 -0.01123 -0.01123 22 3PX 0.01433 0.00000 0.00000 0.00000 0.00000 23 3PY 0.00000 0.01433 0.00000 0.00000 0.00000 24 3PZ 0.00000 0.00000 -0.00627 -0.00129 -0.00129 16 17 18 19 20 16 5ZZ 0.00816 17 5XY 0.00000 0.00000 18 5XZ 0.00000 0.00000 0.00070 19 5YZ 0.00000 0.00000 0.00000 0.00070 20 2 H 1S 0.03971 0.00000 0.00000 0.00000 0.21331 21 2S 0.03081 0.00000 0.00000 0.00000 0.15871 22 3PX 0.00000 0.00000 -0.00066 0.00000 0.00000 23 3PY 0.00000 0.00000 0.00000 -0.00066 0.00000 24 3PZ 0.00270 0.00000 0.00000 0.00000 0.01508 21 22 23 24 21 2S 0.12976 22 3PX 0.00000 0.00063 23 3PY 0.00000 0.00000 0.00063 24 3PZ 0.01023 0.00000 0.00000 0.00115
CH3OH
test molecule |
Calculation Method | RB3LYP |
Basis Set | 6-31G(d.p) |
Final Energy | -115.72396437 a.u. |
RMS Gradient Norm | 0.00001494 a.u. |
Point Group | C1 |
Optimisation Table
Item Value Threshold Converged? Maximum Force 0.000038 0.000450 YES RMS Force 0.000020 0.000300 YES Maximum Displacement 0.000497 0.001800 YES RMS Displacement 0.000240 0.001200 YES Predicted change in Energy=-1.610243D-08 Optimization completed. -- Stationary point found. ---------------------------- ! Optimized Parameters ! ! (Angstroms and Degrees) ! -------------------------- -------------------------- ! Name Definition Value Derivative Info. ! -------------------------------------------------------------------------------- ! R1 R(1,2) 1.1006 -DE/DX = 0.0 ! ! R2 R(1,3) 1.1006 -DE/DX = 0.0 ! ! R3 R(1,4) 1.093 -DE/DX = 0.0 ! ! R4 R(1,5) 1.4181 -DE/DX = 0.0 ! ! R5 R(5,6) 0.9652 -DE/DX = 0.0 ! ! A1 A(2,1,3) 108.2583 -DE/DX = 0.0 ! ! A2 A(2,1,4) 107.8992 -DE/DX = 0.0 ! ! A3 A(2,1,5) 112.8281 -DE/DX = 0.0 ! ! A4 A(3,1,4) 107.8997 -DE/DX = 0.0 ! ! A5 A(3,1,5) 112.8274 -DE/DX = 0.0 ! ! A6 A(4,1,5) 106.9041 -DE/DX = 0.0 ! ! A7 A(1,5,6) 107.7375 -DE/DX = 0.0 ! ! D1 D(2,1,5,6) 61.5104 -DE/DX = 0.0 ! ! D2 D(3,1,5,6) -61.5824 -DE/DX = 0.0 ! ! D3 D(4,1,5,6) 179.9638 -DE/DX = 0.0 ! --------------------------------------------------------------------------------
Vibrational Modes of CH3OH
CH3OH is a non-linear molecule, using the rule 3N-6 where N = 6, we would expect it to have 12 vibrational modes.
The oxygen atom is more electronegative than carbon and hydrogen. Therefore, it is most negatively charged.
IR Spectrum of CH3OH
Molecular Orbital Analysis of CH3OH
Molecular Coefficient Table of CH3OH
1 2 3 4 5 O O O O O Eigenvalues -- -19.13323 -10.21741 -1.00348 -0.68461 -0.49746 1 1 C 1S 0.00001 0.99288 -0.07451 -0.18213 0.02296 2 2S 0.00021 0.04924 0.14082 0.36746 -0.04378 3 2PX -0.00033 -0.00049 -0.10035 0.06600 -0.22267 4 2PY 0.00010 0.00001 0.00321 0.00812 0.22340 5 2PZ 0.00000 0.00000 0.00000 -0.00001 0.00006 6 3S -0.00162 -0.01419 0.04858 0.31204 -0.04524 7 3PX 0.00074 -0.00029 0.00250 0.02863 -0.07688 8 3PY -0.00050 0.00010 -0.00814 -0.00520 0.09766 9 3PZ 0.00000 0.00000 0.00001 0.00001 -0.00001 10 4XX 0.00032 -0.00902 0.01802 -0.01507 0.02270 11 4YY 0.00006 -0.00907 -0.01070 -0.00605 -0.00255 12 4ZZ 0.00010 -0.00910 -0.01132 -0.00767 -0.01465 13 4XY -0.00006 0.00003 -0.00064 -0.00132 -0.00965 14 4XZ 0.00000 0.00000 0.00000 0.00000 0.00000 15 4YZ 0.00000 0.00000 0.00000 0.00000 -0.00004 16 2 H 1S 0.00000 -0.00017 0.02933 0.13947 -0.11858 17 2S -0.00004 0.00278 0.00343 0.04344 -0.07603 18 3PX 0.00005 0.00004 -0.00227 -0.00251 -0.00111 19 3PY -0.00001 -0.00004 0.00252 0.00644 0.00032 20 3PZ -0.00006 -0.00005 0.00361 0.01031 -0.00567 21 3 H 1S 0.00000 -0.00017 0.02933 0.13947 -0.11817 22 2S -0.00004 0.00278 0.00342 0.04343 -0.07571 23 3PX 0.00005 0.00004 -0.00227 -0.00251 -0.00112 24 3PY -0.00001 -0.00004 0.00251 0.00640 0.00035 25 3PZ 0.00006 0.00005 -0.00362 -0.01034 0.00567 26 4 H 1S 0.00012 -0.00020 0.02757 0.14807 0.03097 27 2S 0.00024 0.00271 0.00894 0.05050 0.01704 28 3PX 0.00005 0.00005 -0.00324 -0.00427 -0.00428 29 3PY 0.00003 0.00008 -0.00363 -0.01207 0.00174 30 3PZ 0.00000 0.00000 0.00001 0.00002 0.00001 31 5 O 1S 0.99282 -0.00011 -0.20324 0.06132 -0.04071 32 2S 0.02609 -0.00019 0.44780 -0.14040 0.09438 33 2PX 0.00039 -0.00010 0.05685 0.17576 0.28950 34 2PY -0.00105 0.00002 -0.09528 0.08703 0.31404 35 2PZ 0.00000 0.00000 0.00000 0.00000 0.00002 36 3S 0.01107 0.00199 0.42747 -0.16902 0.15384 37 3PX 0.00020 0.00021 0.03906 0.07928 0.13067 38 3PY -0.00005 0.00024 -0.03356 0.03331 0.16062 39 3PZ 0.00000 0.00000 0.00000 0.00000 0.00002 40 4XX 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