Jump to
S1C2
Energy calculated at HF/6-31G**
| | hartrees |
| Energy at 0K | -79.238235 |
| Energy at 298.15K | -79.244236 |
| HF Energy | -79.238235 |
| Nuclear repulsion energy | 42.388459 |
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 HF/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 |
3184 |
2874 |
0.00 |
227.89 |
0.02 |
0.03 |
| 2 |
A1g |
1565 |
1412 |
0.00 |
3.75 |
0.72 |
0.84 |
| 3 |
A1g |
1058 |
955 |
0.00 |
13.99 |
0.30 |
0.46 |
| 4 |
A1u |
328 |
296 |
0.00 |
0.00 |
0.00 |
0.00 |
| 5 |
A2u |
3178 |
2869 |
72.30 |
0.00 |
0.00 |
0.00 |
| 6 |
A2u |
1532 |
1382 |
0.18 |
0.00 |
0.00 |
0.00 |
| 7 |
Eg |
3232 |
2917 |
0.00 |
147.71 |
0.75 |
0.86 |
| 7 |
Eg |
3232 |
2917 |
0.00 |
147.71 |
0.75 |
0.86 |
| 8 |
Eg |
1627 |
1469 |
0.00 |
37.09 |
0.75 |
0.86 |
| 8 |
Eg |
1627 |
1469 |
0.00 |
37.09 |
0.75 |
0.86 |
| 9 |
Eg |
1329 |
1200 |
0.00 |
2.67 |
0.75 |
0.86 |
| 9 |
Eg |
1329 |
1200 |
0.00 |
2.67 |
0.75 |
0.86 |
| 10 |
Eu |
3257 |
2940 |
100.11 |
0.00 |
0.00 |
0.00 |
| 10 |
Eu |
3257 |
2940 |
100.11 |
0.00 |
0.00 |
0.00 |
| 11 |
Eu |
1633 |
1474 |
5.85 |
0.00 |
0.00 |
0.00 |
| 11 |
Eu |
1633 |
1474 |
5.85 |
0.00 |
0.00 |
0.00 |
| 12 |
Eu |
885 |
799 |
2.61 |
0.00 |
0.00 |
0.00 |
| 12 |
Eu |
885 |
799 |
2.61 |
0.00 |
0.00 |
0.00 |
Unscaled Zero Point Vibrational Energy (zpe) 17385.2 cm
-1
Scaled (by 0.9026) Zero Point Vibrational Energy (zpe) 15691.9 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 HF/6-31G**
Point Group is D3d
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
0.000 |
0.000 |
0.763 |
| C2 |
0.000 |
0.000 |
-0.763 |
| H3 |
0.000 |
1.012 |
1.156 |
| H4 |
-0.877 |
-0.506 |
1.156 |
| H5 |
0.877 |
-0.506 |
1.156 |
| H6 |
0.000 |
-1.012 |
-1.156 |
| H7 |
-0.877 |
0.506 |
-1.156 |
| H8 |
0.877 |
0.506 |
-1.156 |
Atom - Atom Distances (Å)
| |
C1 |
C2 |
H3 |
H4 |
H5 |
H6 |
H7 |
H8 |
| C1 | | 1.5266 | 1.0858 | 1.0858 | 1.0858 | 2.1701 | 2.1701 | 2.1701 |
C2 | 1.5266 | | 2.1701 | 2.1701 | 2.1701 | 1.0858 | 1.0858 | 1.0858 | H3 | 1.0858 | 2.1701 | | 1.7531 | 1.7531 | 3.0734 | 2.5244 | 2.5244 | H4 | 1.0858 | 2.1701 | 1.7531 | | 1.7531 | 2.5244 | 2.5244 | 3.0734 | H5 | 1.0858 | 2.1701 | 1.7531 | 1.7531 | | 2.5244 | 3.0734 | 2.5244 | H6 | 2.1701 | 1.0858 | 3.0734 | 2.5244 | 2.5244 | | 1.7531 | 1.7531 | H7 | 2.1701 | 1.0858 | 2.5244 | 2.5244 | 3.0734 | 1.7531 | | 1.7531 | H8 | 2.1701 | 1.0858 | 2.5244 | 3.0734 | 2.5244 | 1.7531 | 1.7531 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| C1 |
C2 |
H6 |
111.220 |
|
C1 |
C2 |
H7 |
111.220 |
| C1 |
C2 |
H8 |
111.220 |
|
C2 |
C1 |
H3 |
111.220 |
| C2 |
C1 |
H4 |
111.220 |
|
C2 |
C1 |
H5 |
111.220 |
| H3 |
C1 |
H4 |
107.667 |
|
H3 |
C1 |
H5 |
107.667 |
| H4 |
C1 |
H5 |
107.667 |
|
H6 |
C2 |
H7 |
107.667 |
| H6 |
C2 |
H8 |
107.667 |
|
H7 |
C2 |
H8 |
107.667 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at HF/6-31G**
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
-0.335 |
|
|
|
| 2 |
C |
-0.335 |
|
|
|
| 3 |
H |
0.112 |
|
|
|
| 4 |
H |
0.112 |
|
|
|
| 5 |
H |
0.112 |
|
|
|
| 6 |
H |
0.112 |
|
|
|
| 7 |
H |
0.112 |
|
|
|
| 8 |
H |
0.112 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
0.000 |
0.000 |
0.000 |
0.000 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-14.906 |
0.000 |
0.000 |
| y |
0.000 |
-14.906 |
0.000 |
| z |
0.000 |
0.000 |
-15.485 |
|
| Traceless |
| | x | y | z |
| x |
0.289 |
0.000 |
0.000 |
| y |
0.000 |
0.289 |
0.000 |
| z |
0.000 |
0.000 |
-0.579 |
|
| Polar |
| 3z2-r2 | -1.157 |
| x2-y2 | 0.000 |
| xy | 0.000 |
| xz | 0.000 |
| yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
3.322 |
0.000 |
0.000 |
| y |
0.000 |
3.322 |
0.000 |
| z |
0.000 |
0.000 |
3.507 |
<r2> (average value of r
2) Å
2
| <r2> |
30.591 |
| (<r2>)1/2 |
5.531 |
Jump to
S1C1
Energy calculated at HF/6-31G**
| | hartrees |
| Energy at 0K | -79.233423 |
| Energy at 298.15K | |
| HF Energy | -79.233423 |
| Nuclear repulsion energy | 42.221012 |
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 HF/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' |
3198 |
2887 |
0.00 |
|
|
|
| 2 |
A1' |
1582 |
1428 |
0.00 |
|
|
|
| 3 |
A1' |
1056 |
953 |
0.00 |
|
|
|
| 4 |
A1" |
317i |
286i |
0.00 |
|
|
|
| 5 |
A2" |
3185 |
2875 |
76.38 |
|
|
|
| 6 |
A2" |
1530 |
1381 |
0.04 |
|
|
|
| 7 |
E' |
3264 |
2946 |
87.14 |
|
|
|
| 7 |
E' |
3264 |
2946 |
87.14 |
|
|
|
| 8 |
E' |
1638 |
1479 |
7.02 |
|
|
|
| 8 |
E' |
1638 |
1479 |
7.02 |
|
|
|
| 9 |
E' |
966 |
872 |
2.33 |
|
|
|
| 9 |
E' |
966 |
872 |
2.33 |
|
|
|
| 10 |
E" |
3241 |
2925 |
0.00 |
|
|
|
| 10 |
E" |
3241 |
2925 |
0.00 |
|
|
|
| 11 |
E" |
1626 |
1468 |
0.00 |
|
|
|
| 11 |
E" |
1626 |
1468 |
0.00 |
|
|
|
| 12 |
E" |
1285 |
1160 |
0.00 |
|
|
|
| 12 |
E" |
1285 |
1160 |
0.00 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 17138.0 cm
-1
Scaled (by 0.9026) Zero Point Vibrational Energy (zpe) 15468.7 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 HF/6-31G**
Point Group is D3h
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
0.000 |
0.000 |
0.770 |
| C2 |
0.000 |
0.000 |
-0.770 |
| H3 |
0.000 |
1.008 |
1.171 |
| H4 |
-0.873 |
-0.504 |
1.171 |
| H5 |
0.873 |
-0.504 |
1.171 |
| H6 |
0.000 |
1.008 |
-1.171 |
| H7 |
0.873 |
-0.504 |
-1.171 |
| H8 |
-0.873 |
-0.504 |
-1.171 |
Atom - Atom Distances (Å)
| |
C1 |
C2 |
H3 |
H4 |
H5 |
H6 |
H7 |
H8 |
| C1 | | 1.5405 | 1.0848 | 1.0848 | 1.0848 | 2.1872 | 2.1872 | 2.1872 |
C2 | 1.5405 | | 2.1872 | 2.1872 | 2.1872 | 1.0848 | 1.0848 | 1.0848 | H3 | 1.0848 | 2.1872 | | 1.7462 | 1.7462 | 2.3414 | 2.9208 | 2.9208 | H4 | 1.0848 | 2.1872 | 1.7462 | | 1.7462 | 2.9208 | 2.9208 | 2.3414 | H5 | 1.0848 | 2.1872 | 1.7462 | 1.7462 | | 2.9208 | 2.3414 | 2.9208 | H6 | 2.1872 | 1.0848 | 2.3414 | 2.9208 | 2.9208 | | 1.7462 | 1.7462 | H7 | 2.1872 | 1.0848 | 2.9208 | 2.9208 | 2.3414 | 1.7462 | | 1.7462 | H8 | 2.1872 | 1.0848 | 2.9208 | 2.3414 | 2.9208 | 1.7462 | 1.7462 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| C1 |
C2 |
H6 |
111.661 |
|
C1 |
C2 |
H7 |
111.661 |
| C1 |
C2 |
H8 |
111.661 |
|
C2 |
C1 |
H3 |
111.661 |
| C2 |
C1 |
H4 |
111.661 |
|
C2 |
C1 |
H5 |
111.661 |
| H3 |
C1 |
H4 |
107.195 |
|
H3 |
C1 |
H5 |
107.195 |
| H4 |
C1 |
H5 |
107.195 |
|
H6 |
C2 |
H7 |
107.195 |
| H6 |
C2 |
H8 |
107.195 |
|
H7 |
C2 |
H8 |
107.195 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at HF/6-31G**
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
-0.348 |
|
|
|
| 2 |
C |
-0.348 |
|
|
|
| 3 |
H |
0.116 |
|
|
|
| 4 |
H |
0.116 |
|
|
|
| 5 |
H |
0.116 |
|
|
|
| 6 |
H |
0.116 |
|
|
|
| 7 |
H |
0.116 |
|
|
|
| 8 |
H |
0.116 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
0.000 |
0.000 |
0.000 |
0.000 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-14.880 |
0.000 |
0.000 |
| y |
0.000 |
-14.880 |
0.000 |
| z |
0.000 |
0.000 |
-15.416 |
|
| Traceless |
| | x | y | z |
| x |
0.268 |
0.000 |
0.000 |
| y |
0.000 |
0.268 |
0.000 |
| z |
0.000 |
0.000 |
-0.536 |
|
| Polar |
| 3z2-r2 | -1.073 |
| x2-y2 | 0.000 |
| xy | 0.000 |
| xz | 0.000 |
| yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
3.260 |
0.000 |
0.000 |
| y |
0.000 |
3.260 |
0.000 |
| z |
0.000 |
0.000 |
3.456 |
<r2> (average value of r
2) Å
2
| <r2> |
30.847 |
| (<r2>)1/2 |
5.554 |