Jump to
S1C2
Energy calculated at MP2=FULL/cc-pVDZ
| | hartrees |
| Energy at 0K | -79.542894 |
| Energy at 298.15K | -79.548838 |
| HF Energy | -79.234634 |
| Nuclear repulsion energy | 42.022302 |
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=FULL/cc-pVDZ
| Mode Number |
Symmetry |
Frequency (cm-1) |
Scaled Frequency (cm-1) |
IR Intensities (km mol-1) |
Raman Act (Å4/u) |
Dep P |
Dep U |
| 1 |
A1g |
3095 |
2942 |
0.00 |
242.75 |
0.01 |
0.02 |
| 2 |
A1g |
1433 |
1362 |
0.00 |
2.58 |
0.72 |
0.84 |
| 3 |
A1g |
1044 |
993 |
0.00 |
10.75 |
0.27 |
0.42 |
| 4 |
A1u |
334 |
318 |
0.00 |
0.00 |
0.00 |
0.00 |
| 5 |
A2u |
3092 |
2939 |
51.42 |
0.00 |
0.00 |
0.00 |
| 6 |
A2u |
1400 |
1331 |
0.14 |
0.00 |
0.00 |
0.00 |
| 7 |
Eg |
3179 |
3021 |
0.00 |
140.00 |
0.75 |
0.86 |
| 7 |
Eg |
3179 |
3021 |
0.00 |
140.00 |
0.75 |
0.86 |
| 8 |
Eg |
1506 |
1432 |
0.00 |
28.23 |
0.75 |
0.86 |
| 8 |
Eg |
1506 |
1432 |
0.00 |
28.23 |
0.75 |
0.86 |
| 9 |
Eg |
1225 |
1164 |
0.00 |
0.95 |
0.75 |
0.86 |
| 9 |
Eg |
1225 |
1164 |
0.00 |
0.95 |
0.75 |
0.86 |
| 10 |
Eu |
3199 |
3041 |
50.91 |
0.00 |
0.00 |
0.00 |
| 10 |
Eu |
3199 |
3041 |
50.91 |
0.00 |
0.00 |
0.00 |
| 11 |
Eu |
1507 |
1432 |
7.74 |
0.00 |
0.00 |
0.00 |
| 11 |
Eu |
1507 |
1432 |
7.74 |
0.00 |
0.00 |
0.00 |
| 12 |
Eu |
825 |
784 |
3.64 |
0.00 |
0.00 |
0.00 |
| 12 |
Eu |
825 |
784 |
3.64 |
0.00 |
0.00 |
0.00 |
Unscaled Zero Point Vibrational Energy (zpe) 16640.6 cm
-1
Scaled (by 0.9504) Zero Point Vibrational Energy (zpe) 15815.2 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=FULL/cc-pVDZ
Point Group is D3d
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
0.000 |
0.000 |
0.764 |
| C2 |
0.000 |
0.000 |
-0.764 |
| H3 |
0.000 |
1.027 |
1.164 |
| H4 |
-0.889 |
-0.513 |
1.164 |
| H5 |
0.889 |
-0.513 |
1.164 |
| H6 |
0.000 |
-1.027 |
-1.164 |
| H7 |
-0.889 |
0.513 |
-1.164 |
| H8 |
0.889 |
0.513 |
-1.164 |
Atom - Atom Distances (Å)
| |
C1 |
C2 |
H3 |
H4 |
H5 |
H6 |
H7 |
H8 |
| C1 | | 1.5286 | 1.1016 | 1.1016 | 1.1016 | 2.1845 | 2.1845 | 2.1845 |
C2 | 1.5286 | | 2.1845 | 2.1845 | 2.1845 | 1.1016 | 1.1016 | 1.1016 | H3 | 1.1016 | 2.1845 | | 1.7780 | 1.7780 | 3.1039 | 2.5442 | 2.5442 | H4 | 1.1016 | 2.1845 | 1.7780 | | 1.7780 | 2.5442 | 2.5442 | 3.1039 | H5 | 1.1016 | 2.1845 | 1.7780 | 1.7780 | | 2.5442 | 3.1039 | 2.5442 | H6 | 2.1845 | 1.1016 | 3.1039 | 2.5442 | 2.5442 | | 1.7780 | 1.7780 | H7 | 2.1845 | 1.1016 | 2.5442 | 2.5442 | 3.1039 | 1.7780 | | 1.7780 | H8 | 2.1845 | 1.1016 | 2.5442 | 3.1039 | 2.5442 | 1.7780 | 1.7780 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| C1 |
C2 |
H6 |
111.271 |
|
C1 |
C2 |
H7 |
111.271 |
| C1 |
C2 |
H8 |
111.271 |
|
C2 |
C1 |
H3 |
111.271 |
| C2 |
C1 |
H4 |
111.271 |
|
C2 |
C1 |
H5 |
111.271 |
| H3 |
C1 |
H4 |
107.613 |
|
H3 |
C1 |
H5 |
107.613 |
| H4 |
C1 |
H5 |
107.613 |
|
H6 |
C2 |
H7 |
107.613 |
| H6 |
C2 |
H8 |
107.613 |
|
H7 |
C2 |
H8 |
107.613 |
Electronic energy levels
Electronic state
Charges, Dipole, Quadrupole and Polarizability
Jump to
S1C1
Energy calculated at MP2=FULL/cc-pVDZ
| | hartrees |
| Energy at 0K | -79.537711 |
| Energy at 298.15K | |
| HF Energy | -79.229384 |
| Nuclear repulsion energy | 41.856657 |
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=FULL/cc-pVDZ
| 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' |
3107 |
2952 |
0.00 |
|
|
|
| 2 |
A1' |
1445 |
1374 |
0.00 |
|
|
|
| 3 |
A1' |
1042 |
990 |
0.00 |
|
|
|
| 4 |
A1" |
326i |
310i |
0.00 |
|
|
|
| 5 |
A2" |
3098 |
2944 |
53.53 |
|
|
|
| 6 |
A2" |
1397 |
1328 |
0.06 |
|
|
|
| 7 |
E' |
3203 |
3044 |
41.24 |
|
|
|
| 7 |
E' |
3203 |
3044 |
41.24 |
|
|
|
| 8 |
E' |
1510 |
1435 |
9.73 |
|
|
|
| 8 |
E' |
1510 |
1435 |
9.73 |
|
|
|
| 9 |
E' |
899 |
854 |
3.04 |
|
|
|
| 9 |
E' |
899 |
854 |
3.04 |
|
|
|
| 10 |
E" |
3184 |
3026 |
0.00 |
|
|
|
| 10 |
E" |
3184 |
3026 |
0.00 |
|
|
|
| 11 |
E" |
1503 |
1428 |
0.00 |
|
|
|
| 11 |
E" |
1503 |
1428 |
0.00 |
|
|
|
| 12 |
E" |
1171 |
1113 |
0.00 |
|
|
|
| 12 |
E" |
1171 |
1113 |
0.00 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 16350.3 cm
-1
Scaled (by 0.9504) Zero Point Vibrational Energy (zpe) 15539.3 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=FULL/cc-pVDZ
Point Group is D3h
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
0.000 |
0.000 |
0.771 |
| C2 |
0.000 |
0.000 |
-0.771 |
| H3 |
0.000 |
1.022 |
1.180 |
| H4 |
-0.885 |
-0.511 |
1.180 |
| H5 |
0.885 |
-0.511 |
1.180 |
| H6 |
0.000 |
1.022 |
-1.180 |
| H7 |
0.885 |
-0.511 |
-1.180 |
| H8 |
-0.885 |
-0.511 |
-1.180 |
Atom - Atom Distances (Å)
| |
C1 |
C2 |
H3 |
H4 |
H5 |
H6 |
H7 |
H8 |
| C1 | | 1.5419 | 1.1007 | 1.1007 | 1.1007 | 2.2022 | 2.2022 | 2.2022 |
C2 | 1.5419 | | 2.2022 | 2.2022 | 2.2022 | 1.1007 | 1.1007 | 1.1007 | H3 | 1.1007 | 2.2022 | | 1.7701 | 1.7701 | 2.3595 | 2.9496 | 2.9496 | H4 | 1.1007 | 2.2022 | 1.7701 | | 1.7701 | 2.9496 | 2.9496 | 2.3595 | H5 | 1.1007 | 2.2022 | 1.7701 | 1.7701 | | 2.9496 | 2.3595 | 2.9496 | H6 | 2.2022 | 1.1007 | 2.3595 | 2.9496 | 2.9496 | | 1.7701 | 1.7701 | H7 | 2.2022 | 1.1007 | 2.9496 | 2.9496 | 2.3595 | 1.7701 | | 1.7701 | H8 | 2.2022 | 1.1007 | 2.9496 | 2.3595 | 2.9496 | 1.7701 | 1.7701 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| C1 |
C2 |
H6 |
111.801 |
|
C1 |
C2 |
H7 |
111.801 |
| C1 |
C2 |
H8 |
111.801 |
|
C2 |
C1 |
H3 |
111.801 |
| C2 |
C1 |
H4 |
111.801 |
|
C2 |
C1 |
H5 |
111.801 |
| H3 |
C1 |
H4 |
107.044 |
|
H3 |
C1 |
H5 |
107.044 |
| H4 |
C1 |
H5 |
107.044 |
|
H6 |
C2 |
H7 |
107.044 |
| H6 |
C2 |
H8 |
107.044 |
|
H7 |
C2 |
H8 |
107.044 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability