Jump to
S2C1
Energy calculated at MP2/6-31G(2df,p)
| | hartrees |
| Energy at 0K | -77.039664 |
| Energy at 298.15K | -77.039118 |
| HF Energy | -76.772805 |
| Nuclear repulsion energy | 23.808136 |
The energy at 298.15K was derived from the energy at 0K
and an integrated heat capacity that used the calculated vibrational frequencies.
Vibrational Frequencies calculated at MP2/6-31G(2df,p)
| Mode Number |
Symmetry |
Frequency (cm-1) |
Scaled Frequency (cm-1) |
IR Intensities (km mol-1) |
Raman Act (Å4/u) |
Dep P |
Dep U |
| 1 |
A1 |
3204 |
3026 |
55.17 |
|
|
|
| 2 |
A1 |
1688 |
1594 |
79.59 |
|
|
|
| 3 |
A1 |
1220 |
1152 |
21.67 |
|
|
|
| 4 |
B1 |
743 |
702 |
76.47 |
|
|
|
| 5 |
B2 |
3304 |
3121 |
28.02 |
|
|
|
| 6 |
B2 |
167 |
158 |
4.43 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 5162.7 cm
-1
Scaled (by 0.9445) Zero Point Vibrational Energy (zpe) 4876.2 cm
-1
See section
III.C.1 List or set vibrational scaling factors
to change the scale factors used here.
See section
III.C.2
Calculate a vibrational scaling factor for a given set of molecules
to determine the least squares best scaling factor.
Geometric Data calculated at MP2/6-31G(2df,p)
Point Group is C2v
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
0.000 |
0.000 |
-0.481 |
| C2 |
0.000 |
0.000 |
0.823 |
| H3 |
0.000 |
0.938 |
-1.026 |
| H4 |
0.000 |
-0.938 |
-1.026 |
Atom - Atom Distances (Å)
| |
C1 |
C2 |
H3 |
H4 |
| C1 | | 1.3039 | 1.0850 | 1.0850 |
C2 | 1.3039 | | 2.0732 | 2.0732 | H3 | 1.0850 | 2.0732 | | 1.8766 | H4 | 1.0850 | 2.0732 | 1.8766 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| C2 |
C1 |
H3 |
120.141 |
|
C2 |
C1 |
H4 |
120.141 |
| H3 |
C1 |
H4 |
119.719 |
|
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Jump to
S1C1
Energy calculated at MP2/6-31G(2df,p)
| | hartrees |
| Energy at 0K | -76.961765 |
| Energy at 298.15K | -76.961889 |
| HF Energy | -76.740285 |
| Nuclear repulsion energy | 23.849101 |
The energy at 298.15K was derived from the energy at 0K
and an integrated heat capacity that used the calculated vibrational frequencies.
Vibrational Frequencies calculated at MP2/6-31G(2df,p)
| Mode Number |
Symmetry |
Frequency (cm-1) |
Scaled Frequency (cm-1) |
IR Intensities (km mol-1) |
Raman Act (Å4/u) |
Dep P |
Dep U |
| 1 |
A1 |
3161 |
2986 |
1.14 |
|
|
|
| 2 |
A1 |
1650 |
1558 |
3.12 |
|
|
|
| 3 |
A1 |
1437 |
1357 |
5.12 |
|
|
|
| 4 |
B1 |
967 |
913 |
29.22 |
|
|
|
| 5 |
B2 |
3251 |
3071 |
1.72 |
|
|
|
| 6 |
B2 |
1022 |
965 |
1.81 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 5743.6 cm
-1
Scaled (by 0.9445) Zero Point Vibrational Energy (zpe) 5424.9 cm
-1
See section
III.C.1 List or set vibrational scaling factors
to change the scale factors used here.
See section
III.C.2
Calculate a vibrational scaling factor for a given set of molecules
to determine the least squares best scaling factor.
Geometric Data calculated at MP2/6-31G(2df,p)
Point Group is C2v
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
0.000 |
0.000 |
-0.476 |
| C2 |
0.000 |
0.000 |
0.823 |
| H3 |
0.000 |
0.928 |
-1.041 |
| H4 |
0.000 |
-0.928 |
-1.041 |
Atom - Atom Distances (Å)
| |
C1 |
C2 |
H3 |
H4 |
| C1 | | 1.2986 | 1.0867 | 1.0867 |
C2 | 1.2986 | | 2.0819 | 2.0819 | H3 | 1.0867 | 2.0819 | | 1.8567 | H4 | 1.0867 | 2.0819 | 1.8567 | |
More geometry information
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability