Jump to
S1C2
Energy calculated at B2PLYP=FULLultrafine/6-311G*
| | hartrees |
| Energy at 0K | -192.960807 |
| Energy at 298.15K | |
| HF Energy | -192.740511 |
| Nuclear repulsion energy | 128.155822 |
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=FULLultrafine/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 |
3106 |
3106 |
31.16 |
|
|
|
| 2 |
A1 |
3061 |
3061 |
3.02 |
|
|
|
| 3 |
A1 |
1580 |
1580 |
0.03 |
|
|
|
| 4 |
A1 |
1527 |
1527 |
4.32 |
|
|
|
| 5 |
A1 |
1407 |
1407 |
2.54 |
|
|
|
| 6 |
A1 |
1060 |
1060 |
5.96 |
|
|
|
| 7 |
A1 |
937 |
937 |
31.78 |
|
|
|
| 8 |
A1 |
823 |
823 |
4.51 |
|
|
|
| 9 |
A2 |
3102 |
3102 |
0.00 |
|
|
|
| 10 |
A2 |
1262 |
1262 |
0.00 |
|
|
|
| 11 |
A2 |
1185 |
1185 |
0.00 |
|
|
|
| 12 |
A2 |
858 |
858 |
0.00 |
|
|
|
| 13 |
B1 |
3164 |
3164 |
48.62 |
|
|
|
| 14 |
B1 |
3099 |
3099 |
86.32 |
|
|
|
| 15 |
B1 |
1219 |
1219 |
0.61 |
|
|
|
| 16 |
B1 |
1171 |
1171 |
2.75 |
|
|
|
| 17 |
B1 |
780 |
780 |
0.11 |
|
|
|
| 18 |
B1 |
68 |
68 |
2.81 |
|
|
|
| 19 |
B2 |
3052 |
3052 |
167.88 |
|
|
|
| 20 |
B2 |
1552 |
1552 |
1.96 |
|
|
|
| 21 |
B2 |
1336 |
1336 |
0.59 |
|
|
|
| 22 |
B2 |
1285 |
1285 |
11.99 |
|
|
|
| 23 |
B2 |
1045 |
1045 |
96.28 |
|
|
|
| 24 |
B2 |
961 |
961 |
6.22 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 19320.0 cm
-1
Scaled (by 1) Zero Point Vibrational Energy (zpe) 19320.0 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=FULLultrafine/6-311G*
Point Group is C2v
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| O1 |
0.000 |
0.000 |
1.072 |
| C2 |
0.000 |
0.000 |
-1.076 |
| C3 |
0.000 |
1.035 |
0.063 |
| C4 |
0.000 |
-1.035 |
0.063 |
| H5 |
0.889 |
0.000 |
-1.705 |
| H6 |
-0.889 |
0.000 |
-1.705 |
| H7 |
0.892 |
1.664 |
0.132 |
| H8 |
-0.892 |
1.664 |
0.132 |
| H9 |
-0.892 |
-1.664 |
0.132 |
| H10 |
0.892 |
-1.664 |
0.132 |
Atom - Atom Distances (Å)
| |
O1 |
C2 |
C3 |
C4 |
H5 |
H6 |
H7 |
H8 |
H9 |
H10 |
| O1 | | 2.1482 | 1.4456 | 1.4456 | 2.9160 | 2.9160 | 2.1088 | 2.1088 | 2.1088 | 2.1088 |
C2 | 2.1482 | | 1.5393 | 1.5393 | 1.0891 | 1.0891 | 2.2415 | 2.2415 | 2.2415 | 2.2415 | C3 | 1.4456 | 1.5393 | | 2.0704 | 2.2335 | 2.2335 | 1.0933 | 1.0933 | 2.8435 | 2.8435 | C4 | 1.4456 | 1.5393 | 2.0704 | | 2.2335 | 2.2335 | 2.8435 | 2.8435 | 1.0933 | 1.0933 | H5 | 2.9160 | 1.0891 | 2.2335 | 2.2335 | | 1.7782 | 2.4789 | 3.0523 | 3.0523 | 2.4789 | H6 | 2.9160 | 1.0891 | 2.2335 | 2.2335 | 1.7782 | | 3.0523 | 2.4789 | 2.4789 | 3.0523 | H7 | 2.1088 | 2.2415 | 1.0933 | 2.8435 | 2.4789 | 3.0523 | | 1.7835 | 3.7758 | 3.3280 | H8 | 2.1088 | 2.2415 | 1.0933 | 2.8435 | 3.0523 | 2.4789 | 1.7835 | | 3.3280 | 3.7758 | H9 | 2.1088 | 2.2415 | 2.8435 | 1.0933 | 3.0523 | 2.4789 | 3.7758 | 3.3280 | | 1.7835 | H10 | 2.1088 | 2.2415 | 2.8435 | 1.0933 | 2.4789 | 3.0523 | 3.3280 | 3.7758 | 1.7835 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| O1 |
C3 |
C2 |
92.003 |
|
O1 |
C3 |
H7 |
111.571 |
| O1 |
C3 |
H8 |
111.571 |
|
O1 |
C4 |
C2 |
92.003 |
| O1 |
C4 |
H9 |
111.571 |
|
O1 |
C4 |
H10 |
111.571 |
| C2 |
C3 |
H7 |
115.700 |
|
C2 |
C3 |
H8 |
115.700 |
| C2 |
C4 |
H9 |
115.700 |
|
C2 |
C4 |
H10 |
115.700 |
| C3 |
O1 |
C4 |
91.470 |
|
C3 |
C2 |
C4 |
84.525 |
| C3 |
C2 |
H5 |
115.305 |
|
C3 |
C2 |
H6 |
115.305 |
| C4 |
C2 |
H5 |
115.305 |
|
C4 |
C2 |
H6 |
115.305 |
| H5 |
C2 |
H6 |
109.442 |
|
H7 |
C3 |
H8 |
109.296 |
| H9 |
C4 |
H10 |
109.296 |
|
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Jump to
S1C1
Energy calculated at B2PLYP=FULLultrafine/6-311G*
| | hartrees |
| Energy at 0K | -192.960807 |
| Energy at 298.15K | |
| HF Energy | -192.740511 |
| Nuclear repulsion energy | 128.157472 |
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=FULLultrafine/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' |
3164 |
3164 |
48.79 |
|
|
|
| 2 |
A' |
3106 |
3106 |
31.18 |
|
|
|
| 3 |
A' |
3099 |
3099 |
86.17 |
|
|
|
| 4 |
A' |
3061 |
3061 |
3.03 |
|
|
|
| 5 |
A' |
1581 |
1581 |
0.03 |
|
|
|
| 6 |
A' |
1527 |
1527 |
4.33 |
|
|
|
| 7 |
A' |
1407 |
1407 |
2.54 |
|
|
|
| 8 |
A' |
1219 |
1219 |
0.62 |
|
|
|
| 9 |
A' |
1171 |
1171 |
2.75 |
|
|
|
| 10 |
A' |
1060 |
1060 |
5.94 |
|
|
|
| 11 |
A' |
937 |
937 |
31.80 |
|
|
|
| 12 |
A' |
823 |
823 |
4.50 |
|
|
|
| 13 |
A' |
780 |
780 |
0.11 |
|
|
|
| 14 |
A' |
68 |
68 |
2.81 |
|
|
|
| 15 |
A" |
3102 |
3102 |
0.00 |
|
|
|
| 16 |
A" |
3052 |
3052 |
167.88 |
|
|
|
| 17 |
A" |
1553 |
1553 |
1.96 |
|
|
|
| 18 |
A" |
1336 |
1336 |
0.59 |
|
|
|
| 19 |
A" |
1286 |
1286 |
11.99 |
|
|
|
| 20 |
A" |
1262 |
1262 |
0.00 |
|
|
|
| 21 |
A" |
1185 |
1185 |
0.00 |
|
|
|
| 22 |
A" |
1045 |
1045 |
96.25 |
|
|
|
| 23 |
A" |
962 |
962 |
6.25 |
|
|
|
| 24 |
A" |
858 |
858 |
0.00 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 19320.2 cm
-1
Scaled (by 1) Zero Point Vibrational Energy (zpe) 19320.2 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 B2PLYP=FULLultrafine/6-311G*
Point Group is Cs
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| O1 |
-0.001 |
-1.072 |
0.000 |
| C2 |
0.000 |
1.076 |
0.000 |
| C3 |
0.000 |
-0.063 |
1.035 |
| C4 |
0.000 |
-0.063 |
-1.035 |
| H5 |
0.889 |
1.705 |
0.000 |
| H6 |
-0.889 |
1.705 |
0.000 |
| H7 |
0.893 |
-0.133 |
1.663 |
| H8 |
-0.891 |
-0.132 |
1.665 |
| H9 |
0.893 |
-0.133 |
-1.663 |
| H10 |
-0.891 |
-0.132 |
-1.665 |
Atom - Atom Distances (Å)
| |
O1 |
C2 |
C3 |
C4 |
H5 |
H6 |
H7 |
H8 |
H9 |
H10 |
| O1 | | 2.1481 | 1.4456 | 1.4456 | 2.9167 | 2.9154 | 2.1089 | 2.1089 | 2.1089 | 2.1089 |
C2 | 2.1481 | | 1.5392 | 1.5392 | 1.0891 | 1.0891 | 2.2413 | 2.2415 | 2.2413 | 2.2415 | C3 | 1.4456 | 1.5392 | | 2.0704 | 2.2337 | 2.2334 | 1.0933 | 1.0933 | 2.8430 | 2.8441 | C4 | 1.4456 | 1.5392 | 2.0704 | | 2.2337 | 2.2334 | 2.8430 | 2.8441 | 1.0933 | 1.0933 | H5 | 2.9167 | 1.0891 | 2.2337 | 2.2337 | | 1.7780 | 2.4790 | 3.0521 | 2.4790 | 3.0521 | H6 | 2.9154 | 1.0891 | 2.2334 | 2.2334 | 1.7780 | | 3.0523 | 2.4788 | 3.0523 | 2.4788 | H7 | 2.1089 | 2.2413 | 1.0933 | 2.8430 | 2.4790 | 3.0523 | | 1.7834 | 3.3266 | 3.7758 | H8 | 2.1089 | 2.2415 | 1.0933 | 2.8441 | 3.0521 | 2.4788 | 1.7834 | | 3.7758 | 3.3296 | H9 | 2.1089 | 2.2413 | 2.8430 | 1.0933 | 2.4790 | 3.0523 | 3.3266 | 3.7758 | | 1.7834 | H10 | 2.1089 | 2.2415 | 2.8441 | 1.0933 | 3.0521 | 2.4788 | 3.7758 | 3.3296 | 1.7834 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| O1 |
C3 |
C2 |
92.000 |
|
O1 |
C3 |
H7 |
111.579 |
| O1 |
C3 |
H8 |
111.577 |
|
O1 |
C4 |
C2 |
92.000 |
| O1 |
C4 |
H9 |
111.579 |
|
O1 |
C4 |
H10 |
111.577 |
| C2 |
C3 |
H7 |
115.687 |
|
C2 |
C3 |
H8 |
115.706 |
| C2 |
C4 |
H9 |
115.687 |
|
C2 |
C4 |
H10 |
115.706 |
| C3 |
O1 |
C4 |
91.470 |
|
C3 |
C2 |
C4 |
84.530 |
| C3 |
C2 |
H5 |
115.324 |
|
C3 |
C2 |
H6 |
115.297 |
| C4 |
C2 |
H5 |
115.324 |
|
C4 |
C2 |
H6 |
115.297 |
| H5 |
C2 |
H6 |
109.423 |
|
H7 |
C3 |
H8 |
109.293 |
| H9 |
C4 |
H10 |
109.293 |
|
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability