Jump to
S1C2
Energy calculated at CID/6-31G
| | hartrees |
| Energy at 0K | -79.400419 |
| Energy at 298.15K | -79.406381 |
| HF Energy | -79.196687 |
| Nuclear repulsion energy | 41.919489 |
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 CID/6-31G
| 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 |
3072 |
2873 |
0.00 |
|
|
|
| 2 |
A1g |
1504 |
1407 |
0.00 |
|
|
|
| 3 |
A1g |
1026 |
960 |
0.00 |
|
|
|
| 4 |
A1u |
317 |
297 |
0.00 |
|
|
|
| 5 |
A2u |
3064 |
2865 |
56.43 |
|
|
|
| 6 |
A2u |
1500 |
1403 |
3.34 |
|
|
|
| 7 |
Eg |
3124 |
2921 |
0.00 |
|
|
|
| 7 |
Eg |
3124 |
2921 |
0.00 |
|
|
|
| 8 |
Eg |
1575 |
1473 |
0.00 |
|
|
|
| 8 |
Eg |
1575 |
1473 |
0.00 |
|
|
|
| 9 |
Eg |
1292 |
1208 |
0.00 |
|
|
|
| 9 |
Eg |
1292 |
1208 |
0.00 |
|
|
|
| 10 |
Eu |
3148 |
2944 |
79.90 |
|
|
|
| 10 |
Eu |
3148 |
2944 |
79.90 |
|
|
|
| 11 |
Eu |
1580 |
1478 |
9.05 |
|
|
|
| 11 |
Eu |
1580 |
1478 |
9.05 |
|
|
|
| 12 |
Eu |
866 |
810 |
4.57 |
|
|
|
| 12 |
Eu |
866 |
810 |
4.57 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 16826.5 cm
-1
Scaled (by 0.9352) Zero Point Vibrational Energy (zpe) 15736.1 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 CID/6-31G
Point Group is D3d
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
0.000 |
0.000 |
0.772 |
| C2 |
0.000 |
0.000 |
-0.772 |
| H3 |
0.000 |
1.025 |
1.167 |
| H4 |
-0.887 |
-0.512 |
1.167 |
| H5 |
0.887 |
-0.512 |
1.167 |
| H6 |
0.000 |
-1.025 |
-1.167 |
| H7 |
-0.887 |
0.512 |
-1.167 |
| H8 |
0.887 |
0.512 |
-1.167 |
Atom - Atom Distances (Å)
| |
C1 |
C2 |
H3 |
H4 |
H5 |
H6 |
H7 |
H8 |
| C1 | | 1.5434 | 1.0984 | 1.0984 | 1.0984 | 2.1931 | 2.1931 | 2.1931 |
C2 | 1.5434 | | 2.1931 | 2.1931 | 2.1931 | 1.0984 | 1.0984 | 1.0984 | H3 | 1.0984 | 2.1931 | | 1.7748 | 1.7748 | 3.1064 | 2.5495 | 2.5495 | H4 | 1.0984 | 2.1931 | 1.7748 | | 1.7748 | 2.5495 | 2.5495 | 3.1064 | H5 | 1.0984 | 2.1931 | 1.7748 | 1.7748 | | 2.5495 | 3.1064 | 2.5495 | H6 | 2.1931 | 1.0984 | 3.1064 | 2.5495 | 2.5495 | | 1.7748 | 1.7748 | H7 | 2.1931 | 1.0984 | 2.5495 | 2.5495 | 3.1064 | 1.7748 | | 1.7748 | H8 | 2.1931 | 1.0984 | 2.5495 | 3.1064 | 2.5495 | 1.7748 | 1.7748 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| C1 |
C2 |
H6 |
111.107 |
|
C1 |
C2 |
H7 |
111.107 |
| C1 |
C2 |
H8 |
111.107 |
|
C2 |
C1 |
H3 |
111.107 |
| C2 |
C1 |
H4 |
111.107 |
|
C2 |
C1 |
H5 |
111.107 |
| H3 |
C1 |
H4 |
107.788 |
|
H3 |
C1 |
H5 |
107.788 |
| H4 |
C1 |
H5 |
107.788 |
|
H6 |
C2 |
H7 |
107.788 |
| H6 |
C2 |
H8 |
107.788 |
|
H7 |
C2 |
H8 |
107.788 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Jump to
S1C1
Energy calculated at CID/6-31G
| | hartrees |
| Energy at 0K | -79.395750 |
| Energy at 298.15K | |
| HF Energy | -79.192267 |
| Nuclear repulsion energy | 41.767989 |
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 CID/6-31G
| 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' |
3083 |
2883 |
0.00 |
|
|
|
| 2 |
A1' |
1525 |
1426 |
0.00 |
|
|
|
| 3 |
A1' |
1017 |
951 |
0.00 |
|
|
|
| 4 |
A1" |
310i |
290i |
0.00 |
|
|
|
| 5 |
A2" |
3068 |
2869 |
60.21 |
|
|
|
| 6 |
A2" |
1496 |
1399 |
3.12 |
|
|
|
| 7 |
E' |
3151 |
2947 |
69.79 |
|
|
|
| 7 |
E' |
3151 |
2947 |
69.79 |
|
|
|
| 8 |
E' |
1586 |
1483 |
10.36 |
|
|
|
| 8 |
E' |
1586 |
1483 |
10.36 |
|
|
|
| 9 |
E' |
949 |
888 |
4.58 |
|
|
|
| 9 |
E' |
949 |
888 |
4.58 |
|
|
|
| 10 |
E" |
3129 |
2926 |
0.00 |
|
|
|
| 10 |
E" |
3129 |
2926 |
0.00 |
|
|
|
| 11 |
E" |
1570 |
1469 |
0.00 |
|
|
|
| 11 |
E" |
1570 |
1469 |
0.00 |
|
|
|
| 12 |
E" |
1237 |
1157 |
0.00 |
|
|
|
| 12 |
E" |
1237 |
1157 |
0.00 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 16561.9 cm
-1
Scaled (by 0.9352) Zero Point Vibrational Energy (zpe) 15488.7 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 CID/6-31G
Point Group is D3h
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
0.000 |
0.000 |
0.778 |
| C2 |
0.000 |
0.000 |
-0.778 |
| H3 |
0.000 |
1.021 |
1.181 |
| H4 |
-0.884 |
-0.511 |
1.181 |
| H5 |
0.884 |
-0.511 |
1.181 |
| H6 |
0.000 |
1.021 |
-1.181 |
| H7 |
0.884 |
-0.511 |
-1.181 |
| H8 |
-0.884 |
-0.511 |
-1.181 |
Atom - Atom Distances (Å)
| |
C1 |
C2 |
H3 |
H4 |
H5 |
H6 |
H7 |
H8 |
| C1 | | 1.5558 | 1.0977 | 1.0977 | 1.0977 | 2.2089 | 2.2089 | 2.2089 |
C2 | 1.5558 | | 2.2089 | 2.2089 | 2.2089 | 1.0977 | 1.0977 | 1.0977 | H3 | 1.0977 | 2.2089 | | 1.7685 | 1.7685 | 2.3617 | 2.9505 | 2.9505 | H4 | 1.0977 | 2.2089 | 1.7685 | | 1.7685 | 2.9505 | 2.9505 | 2.3617 | H5 | 1.0977 | 2.2089 | 1.7685 | 1.7685 | | 2.9505 | 2.3617 | 2.9505 | H6 | 2.2089 | 1.0977 | 2.3617 | 2.9505 | 2.9505 | | 1.7685 | 1.7685 | H7 | 2.2089 | 1.0977 | 2.9505 | 2.9505 | 2.3617 | 1.7685 | | 1.7685 | H8 | 2.2089 | 1.0977 | 2.9505 | 2.3617 | 2.9505 | 1.7685 | 1.7685 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| C1 |
C2 |
H6 |
111.538 |
|
C1 |
C2 |
H7 |
111.538 |
| C1 |
C2 |
H8 |
111.538 |
|
C2 |
C1 |
H3 |
111.538 |
| C2 |
C1 |
H4 |
111.538 |
|
C2 |
C1 |
H5 |
111.538 |
| H3 |
C1 |
H4 |
107.328 |
|
H3 |
C1 |
H5 |
107.328 |
| H4 |
C1 |
H5 |
107.328 |
|
H6 |
C2 |
H7 |
107.328 |
| H6 |
C2 |
H8 |
107.328 |
|
H7 |
C2 |
H8 |
107.328 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability