Jump to
S1C2
Energy calculated at B2PLYP=FULLultrafine/6-31G**
| | hartrees |
| Energy at 0K | -192.909835 |
| Energy at 298.15K | |
| HF Energy | -192.707240 |
| Nuclear repulsion energy | 128.112576 |
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/6-31G**
| 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 |
3131 |
3131 |
24.80 |
|
|
|
| 2 |
A1 |
3075 |
3075 |
1.83 |
|
|
|
| 3 |
A1 |
1586 |
1586 |
0.01 |
|
|
|
| 4 |
A1 |
1529 |
1529 |
1.52 |
|
|
|
| 5 |
A1 |
1409 |
1409 |
5.12 |
|
|
|
| 6 |
A1 |
1064 |
1064 |
5.23 |
|
|
|
| 7 |
A1 |
941 |
941 |
27.50 |
|
|
|
| 8 |
A1 |
818 |
818 |
4.04 |
|
|
|
| 9 |
A2 |
3117 |
3117 |
0.00 |
|
|
|
| 10 |
A2 |
1258 |
1258 |
0.00 |
|
|
|
| 11 |
A2 |
1181 |
1181 |
0.00 |
|
|
|
| 12 |
A2 |
856 |
856 |
0.00 |
|
|
|
| 13 |
B1 |
3191 |
3191 |
32.91 |
|
|
|
| 14 |
B1 |
3117 |
3117 |
87.48 |
|
|
|
| 15 |
B1 |
1217 |
1217 |
1.23 |
|
|
|
| 16 |
B1 |
1164 |
1164 |
1.82 |
|
|
|
| 17 |
B1 |
779 |
779 |
0.14 |
|
|
|
| 18 |
B1 |
4i |
4i |
2.89 |
|
|
|
| 19 |
B2 |
3066 |
3066 |
152.30 |
|
|
|
| 20 |
B2 |
1557 |
1557 |
5.92 |
|
|
|
| 21 |
B2 |
1333 |
1333 |
0.54 |
|
|
|
| 22 |
B2 |
1288 |
1288 |
7.09 |
|
|
|
| 23 |
B2 |
1055 |
1055 |
97.21 |
|
|
|
| 24 |
B2 |
965 |
965 |
6.74 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 19347.1 cm
-1
Scaled (by 1) Zero Point Vibrational Energy (zpe) 19347.1 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 B2PLYP=FULLultrafine/6-31G**
Point Group is C2v
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| O1 |
0.000 |
0.000 |
1.073 |
| C2 |
0.000 |
0.000 |
-1.075 |
| C3 |
0.000 |
1.036 |
0.063 |
| C4 |
0.000 |
-1.036 |
0.063 |
| H5 |
0.888 |
0.000 |
-1.705 |
| H6 |
-0.888 |
0.000 |
-1.705 |
| H7 |
0.890 |
1.668 |
0.129 |
| H8 |
-0.890 |
1.668 |
0.129 |
| H9 |
-0.890 |
-1.668 |
0.129 |
| H10 |
0.890 |
-1.668 |
0.129 |
Atom - Atom Distances (Å)
| |
O1 |
C2 |
C3 |
C4 |
H5 |
H6 |
H7 |
H8 |
H9 |
H10 |
| O1 | | 2.1479 | 1.4469 | 1.4469 | 2.9164 | 2.9164 | 2.1135 | 2.1135 | 2.1135 | 2.1135 |
C2 | 2.1479 | | 1.5384 | 1.5384 | 1.0888 | 1.0888 | 2.2413 | 2.2413 | 2.2413 | 2.2413 | C3 | 1.4469 | 1.5384 | | 2.0714 | 2.2328 | 2.2328 | 1.0938 | 1.0938 | 2.8474 | 2.8474 | C4 | 1.4469 | 1.5384 | 2.0714 | | 2.2328 | 2.2328 | 2.8474 | 2.8474 | 1.0938 | 1.0938 | H5 | 2.9164 | 1.0888 | 2.2328 | 2.2328 | | 1.7758 | 2.4789 | 3.0505 | 3.0505 | 2.4789 | H6 | 2.9164 | 1.0888 | 2.2328 | 2.2328 | 1.7758 | | 3.0505 | 2.4789 | 2.4789 | 3.0505 | H7 | 2.1135 | 2.2413 | 1.0938 | 2.8474 | 2.4789 | 3.0505 | | 1.7797 | 3.7815 | 3.3366 | H8 | 2.1135 | 2.2413 | 1.0938 | 2.8474 | 3.0505 | 2.4789 | 1.7797 | | 3.3366 | 3.7815 | H9 | 2.1135 | 2.2413 | 2.8474 | 1.0938 | 3.0505 | 2.4789 | 3.7815 | 3.3366 | | 1.7797 | H10 | 2.1135 | 2.2413 | 2.8474 | 1.0938 | 2.4789 | 3.0505 | 3.3366 | 3.7815 | 1.7797 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| O1 |
C3 |
C2 |
91.974 |
|
O1 |
C3 |
H7 |
111.834 |
| O1 |
C3 |
H8 |
111.834 |
|
O1 |
C4 |
C2 |
91.974 |
| O1 |
C4 |
H9 |
111.834 |
|
O1 |
C4 |
H10 |
111.834 |
| C2 |
C3 |
H7 |
115.718 |
|
C2 |
C3 |
H8 |
115.718 |
| C2 |
C4 |
H9 |
115.718 |
|
C2 |
C4 |
H10 |
115.718 |
| C3 |
O1 |
C4 |
91.419 |
|
C3 |
C2 |
C4 |
84.634 |
| C3 |
C2 |
H5 |
115.337 |
|
C3 |
C2 |
H6 |
115.337 |
| C4 |
C2 |
H5 |
115.337 |
|
C4 |
C2 |
H6 |
115.337 |
| H5 |
C2 |
H6 |
109.274 |
|
H7 |
C3 |
H8 |
108.887 |
| H9 |
C4 |
H10 |
108.887 |
|
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Jump to
S1C1
Energy calculated at B2PLYP=FULLultrafine/6-31G**
| | hartrees |
| Energy at 0K | -192.909835 |
| Energy at 298.15K | |
| HF Energy | -192.707241 |
| Nuclear repulsion energy | 128.115765 |
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/6-31G**
| Mode Number |
Symmetry |
Frequency (cm-1) |
Scaled Frequency (cm-1) |
IR Intensities (km mol-1) |
Raman Act (Å4/u) |
Dep P |
Dep U |
| 1 |
A' |
3191 |
3191 |
33.02 |
|
|
|
| 2 |
A' |
3131 |
3131 |
24.85 |
|
|
|
| 3 |
A' |
3117 |
3117 |
87.22 |
|
|
|
| 4 |
A' |
3075 |
3075 |
2.01 |
|
|
|
| 5 |
A' |
1586 |
1586 |
0.01 |
|
|
|
| 6 |
A' |
1530 |
1530 |
1.52 |
|
|
|
| 7 |
A' |
1409 |
1409 |
5.12 |
|
|
|
| 8 |
A' |
1217 |
1217 |
1.23 |
|
|
|
| 9 |
A' |
1164 |
1164 |
1.82 |
|
|
|
| 10 |
A' |
1064 |
1064 |
5.23 |
|
|
|
| 11 |
A' |
942 |
942 |
27.49 |
|
|
|
| 12 |
A' |
818 |
818 |
4.03 |
|
|
|
| 13 |
A' |
779 |
779 |
0.16 |
|
|
|
| 14 |
A' |
7 |
7 |
2.89 |
|
|
|
| 15 |
A" |
3117 |
3117 |
0.13 |
|
|
|
| 16 |
A" |
3066 |
3066 |
152.15 |
|
|
|
| 17 |
A" |
1557 |
1557 |
5.92 |
|
|
|
| 18 |
A" |
1333 |
1333 |
0.54 |
|
|
|
| 19 |
A" |
1288 |
1288 |
7.07 |
|
|
|
| 20 |
A" |
1258 |
1258 |
0.01 |
|
|
|
| 21 |
A" |
1181 |
1181 |
0.00 |
|
|
|
| 22 |
A" |
1055 |
1055 |
97.20 |
|
|
|
| 23 |
A" |
965 |
965 |
6.74 |
|
|
|
| 24 |
A" |
856 |
856 |
0.01 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 19352.6 cm
-1
Scaled (by 1) Zero Point Vibrational Energy (zpe) 19352.6 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/6-31G**
Point Group is Cs
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| O1 |
0.013 |
-1.073 |
0.000 |
| C2 |
-0.004 |
1.074 |
0.000 |
| C3 |
-0.004 |
-0.063 |
1.036 |
| C4 |
-0.004 |
-0.063 |
-1.036 |
| H5 |
0.886 |
1.702 |
0.000 |
| H6 |
-0.889 |
1.708 |
0.000 |
| H7 |
0.880 |
-0.123 |
1.677 |
| H8 |
-0.899 |
-0.135 |
1.659 |
| H9 |
0.880 |
-0.123 |
-1.677 |
| H10 |
-0.899 |
-0.135 |
-1.659 |
Atom - Atom Distances (Å)
| |
O1 |
C2 |
C3 |
C4 |
H5 |
H6 |
H7 |
H8 |
H9 |
H10 |
| O1 | | 2.1477 | 1.4468 | 1.4468 | 2.9092 | 2.9235 | 2.1136 | 2.1135 | 2.1136 | 2.1135 |
C2 | 2.1477 | | 1.5383 | 1.5383 | 1.0888 | 1.0888 | 2.2423 | 2.2400 | 2.2423 | 2.2400 | C3 | 1.4468 | 1.5383 | | 2.0713 | 2.2314 | 2.2343 | 1.0937 | 1.0939 | 2.8538 | 2.8409 | C4 | 1.4468 | 1.5383 | 2.0713 | | 2.2314 | 2.2343 | 2.8538 | 2.8409 | 1.0937 | 1.0939 | H5 | 2.9092 | 1.0888 | 2.2314 | 2.2314 | | 1.7756 | 2.4787 | 3.0520 | 2.4787 | 3.0520 | H6 | 2.9235 | 1.0888 | 2.2343 | 2.2343 | 1.7756 | | 3.0488 | 2.4793 | 3.0488 | 2.4793 | H7 | 2.1136 | 2.2423 | 1.0937 | 2.8538 | 2.4787 | 3.0488 | | 1.7797 | 3.3544 | 3.7814 | H8 | 2.1135 | 2.2400 | 1.0939 | 2.8409 | 3.0520 | 2.4793 | 1.7797 | | 3.7814 | 3.3186 | H9 | 2.1136 | 2.2423 | 2.8538 | 1.0937 | 2.4787 | 3.0488 | 3.3544 | 3.7814 | | 1.7797 | H10 | 2.1135 | 2.2400 | 2.8409 | 1.0939 | 3.0520 | 2.4793 | 3.7814 | 3.3186 | 1.7797 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| O1 |
C3 |
C2 |
91.968 |
|
O1 |
C3 |
H7 |
111.848 |
| O1 |
C3 |
H8 |
111.831 |
|
O1 |
C4 |
C2 |
91.968 |
| O1 |
C4 |
H9 |
111.848 |
|
O1 |
C4 |
H10 |
111.831 |
| C2 |
C3 |
H7 |
115.819 |
|
C2 |
C3 |
H8 |
115.613 |
| C2 |
C4 |
H9 |
115.819 |
|
C2 |
C4 |
H10 |
115.613 |
| C3 |
O1 |
C4 |
91.419 |
|
C3 |
C2 |
C4 |
84.636 |
| C3 |
C2 |
H5 |
115.224 |
|
C3 |
C2 |
H6 |
115.463 |
| C4 |
C2 |
H5 |
115.224 |
|
C4 |
C2 |
H6 |
115.463 |
| H5 |
C2 |
H6 |
109.255 |
|
H7 |
C3 |
H8 |
108.886 |
| H9 |
C4 |
H10 |
108.886 |
|
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability