Jump to
S1C2
Energy calculated at B2PLYP=FULL/6-311G**
| | hartrees |
| Energy at 0K | -117.168111 |
| Energy at 298.15K | -117.172388 |
| HF Energy | -117.019203 |
| Nuclear repulsion energy | 65.013427 |
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 B2PLYP=FULL/6-311G**
| 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 |
3270 |
3270 |
18.55 |
|
|
|
| 2 |
A1 |
3172 |
3172 |
1.01 |
|
|
|
| 3 |
A1 |
3165 |
3165 |
17.36 |
|
|
|
| 4 |
A1 |
1533 |
1533 |
2.93 |
|
|
|
| 5 |
A1 |
1284 |
1284 |
0.92 |
|
|
|
| 6 |
A1 |
1047 |
1047 |
0.05 |
|
|
|
| 7 |
A1 |
430 |
430 |
0.07 |
|
|
|
| 8 |
A2 |
783 |
783 |
0.00 |
|
|
|
| 9 |
A2 |
561 |
561 |
0.00 |
|
|
|
| 10 |
B1 |
1021 |
1021 |
24.38 |
|
|
|
| 11 |
B1 |
804 |
804 |
77.12 |
|
|
|
| 12 |
B1 |
535 |
535 |
16.03 |
|
|
|
| 13 |
B2 |
3268 |
3268 |
5.26 |
|
|
|
| 14 |
B2 |
3164 |
3164 |
8.26 |
|
|
|
| 15 |
B2 |
1516 |
1516 |
0.92 |
|
|
|
| 16 |
B2 |
1429 |
1429 |
6.46 |
|
|
|
| 17 |
B2 |
1189 |
1189 |
0.08 |
|
|
|
| 18 |
B2 |
941 |
941 |
0.04 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 14556.0 cm
-1
Scaled (by 1) Zero Point Vibrational Energy (zpe) 14556.0 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 B2PLYP=FULL/6-311G**
Point Group is C2v
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
0.000 |
0.000 |
0.444 |
| H2 |
0.000 |
0.000 |
1.531 |
| C3 |
0.000 |
1.225 |
-0.197 |
| C4 |
0.000 |
-1.225 |
-0.197 |
| H5 |
0.000 |
2.153 |
0.359 |
| H6 |
0.000 |
-2.153 |
0.359 |
| H7 |
0.000 |
1.287 |
-1.278 |
| H8 |
0.000 |
-1.287 |
-1.278 |
Atom - Atom Distances (Å)
| |
C1 |
H2 |
C3 |
C4 |
H5 |
H6 |
H7 |
H8 |
| C1 | | 1.0868 | 1.3826 | 1.3826 | 2.1547 | 2.1547 | 2.1506 | 2.1506 |
H2 | 1.0868 | | 2.1180 | 2.1180 | 2.4516 | 2.4516 | 3.0904 | 3.0904 | C3 | 1.3826 | 2.1180 | | 2.4501 | 1.0813 | 3.4234 | 1.0835 | 2.7355 | C4 | 1.3826 | 2.1180 | 2.4501 | | 3.4234 | 1.0813 | 2.7355 | 1.0835 | H5 | 2.1547 | 2.4516 | 1.0813 | 3.4234 | | 4.3059 | 1.8516 | 3.8100 | H6 | 2.1547 | 2.4516 | 3.4234 | 1.0813 | 4.3059 | | 3.8100 | 1.8516 | H7 | 2.1506 | 3.0904 | 1.0835 | 2.7355 | 1.8516 | 3.8100 | | 2.5750 | H8 | 2.1506 | 3.0904 | 2.7355 | 1.0835 | 3.8100 | 1.8516 | 2.5750 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| C1 |
C3 |
H5 |
121.492 |
|
C1 |
C3 |
H7 |
120.921 |
| C1 |
C4 |
H6 |
121.492 |
|
C1 |
C4 |
H8 |
120.921 |
| H2 |
C1 |
C3 |
117.619 |
|
H2 |
C1 |
C4 |
117.619 |
| C3 |
C1 |
C4 |
124.763 |
|
H5 |
C3 |
H7 |
117.587 |
| H6 |
C4 |
H8 |
117.587 |
|
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Jump to
S1C1
Energy calculated at B2PLYP=FULL/6-311G**
| | hartrees |
| Energy at 0K | -117.168111 |
| Energy at 298.15K | -117.172389 |
| HF Energy | -117.019201 |
| Nuclear repulsion energy | 65.015570 |
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 B2PLYP=FULL/6-311G**
| Mode Number |
Symmetry |
Frequency (cm-1) |
Scaled Frequency (cm-1) |
IR Intensities (km mol-1) |
Raman Act (Å4/u) |
Dep P |
Dep U |
| 1 |
A' |
3270 |
3270 |
18.46 |
|
|
|
| 2 |
A' |
3268 |
3268 |
5.29 |
|
|
|
| 3 |
A' |
3171 |
3171 |
0.94 |
|
|
|
| 4 |
A' |
3164 |
3164 |
17.23 |
|
|
|
| 5 |
A' |
3164 |
3164 |
8.45 |
|
|
|
| 6 |
A' |
1533 |
1533 |
2.96 |
|
|
|
| 7 |
A' |
1516 |
1516 |
0.91 |
|
|
|
| 8 |
A' |
1429 |
1429 |
6.47 |
|
|
|
| 9 |
A' |
1285 |
1285 |
0.93 |
|
|
|
| 10 |
A' |
1189 |
1189 |
0.08 |
|
|
|
| 11 |
A' |
1047 |
1047 |
0.05 |
|
|
|
| 12 |
A' |
942 |
942 |
0.04 |
|
|
|
| 13 |
A' |
431 |
431 |
0.08 |
|
|
|
| 14 |
A" |
1021 |
1021 |
24.37 |
|
|
|
| 15 |
A" |
804 |
804 |
77.10 |
|
|
|
| 16 |
A" |
783 |
783 |
0.01 |
|
|
|
| 17 |
A" |
561 |
561 |
0.00 |
|
|
|
| 18 |
A" |
536 |
536 |
16.09 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 14556.0 cm
-1
Scaled (by 1) Zero Point Vibrational Energy (zpe) 14556.0 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 B2PLYP=FULL/6-311G**
Point Group is Cs
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
0.000 |
0.445 |
0.000 |
| H2 |
0.000 |
1.532 |
0.000 |
| C3 |
-1.225 |
-0.197 |
0.000 |
| C4 |
1.225 |
-0.196 |
0.000 |
| H5 |
-2.153 |
0.358 |
0.000 |
| H6 |
2.153 |
0.358 |
0.000 |
| H7 |
-1.286 |
-1.279 |
0.000 |
| H8 |
1.286 |
-1.278 |
0.000 |
Atom - Atom Distances (Å)
| |
C1 |
H2 |
C3 |
C4 |
H5 |
H6 |
H7 |
H8 |
| C1 | | 1.0868 | 1.3828 | 1.3825 | 2.1548 | 2.1546 | 2.1502 | 2.1503 |
H2 | 1.0868 | | 2.1185 | 2.1180 | 2.4522 | 2.4516 | 3.0904 | 3.0903 | C3 | 1.3828 | 2.1185 | | 2.4497 | 1.0814 | 3.4231 | 1.0835 | 2.7343 | C4 | 1.3825 | 2.1180 | 2.4497 | | 3.4231 | 1.0813 | 2.7339 | 1.0836 | H5 | 2.1548 | 2.4522 | 1.0814 | 3.4231 | | 4.3059 | 1.8522 | 3.8088 | H6 | 2.1546 | 2.4516 | 3.4231 | 1.0813 | 4.3059 | | 3.8084 | 1.8519 | H7 | 2.1502 | 3.0904 | 1.0835 | 2.7339 | 1.8522 | 3.8084 | | 2.5721 | H8 | 2.1503 | 3.0903 | 2.7343 | 1.0836 | 3.8088 | 1.8519 | 2.5721 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| C1 |
C3 |
H5 |
121.488 |
|
C1 |
C3 |
H7 |
120.864 |
| C1 |
C4 |
H6 |
121.490 |
|
C1 |
C4 |
H8 |
120.889 |
| H2 |
C1 |
C3 |
117.648 |
|
H2 |
C1 |
C4 |
117.629 |
| C3 |
C1 |
C4 |
124.723 |
|
H5 |
C3 |
H7 |
117.648 |
| H6 |
C4 |
H8 |
117.621 |
|
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability