Jump to
S1C2
Energy calculated at HF/6-31+G**
| hartrees |
Energy at 0K | -191.923474 |
Energy at 298.15K | -191.930904 |
HF Energy | -191.923474 |
Nuclear repulsion energy | 129.356287 |
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/6-31+G**
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 |
3235 |
2925 |
29.97 |
|
|
|
2 |
A1 |
3208 |
2901 |
8.00 |
|
|
|
3 |
A1 |
1680 |
1519 |
0.08 |
|
|
|
4 |
A1 |
1621 |
1466 |
3.34 |
|
|
|
5 |
A1 |
1518 |
1372 |
10.03 |
|
|
|
6 |
A1 |
1138 |
1029 |
23.41 |
|
|
|
7 |
A1 |
1023 |
925 |
36.13 |
|
|
|
8 |
A1 |
896 |
810 |
5.33 |
|
|
|
9 |
A2 |
3248 |
2937 |
0.00 |
|
|
|
10 |
A2 |
1337 |
1209 |
0.00 |
|
|
|
11 |
A2 |
1263 |
1142 |
0.00 |
|
|
|
12 |
A2 |
900 |
813 |
0.00 |
|
|
|
13 |
B1 |
3287 |
2972 |
77.26 |
|
|
|
14 |
B1 |
3244 |
2933 |
59.96 |
|
|
|
15 |
B1 |
1312 |
1186 |
0.06 |
|
|
|
16 |
B1 |
1263 |
1142 |
6.85 |
|
|
|
17 |
B1 |
825 |
746 |
0.03 |
|
|
|
18 |
B1 |
81 |
73 |
6.21 |
|
|
|
19 |
B2 |
3201 |
2894 |
173.45 |
|
|
|
20 |
B2 |
1651 |
1493 |
3.46 |
|
|
|
21 |
B2 |
1439 |
1301 |
0.07 |
|
|
|
22 |
B2 |
1392 |
1258 |
8.89 |
|
|
|
23 |
B2 |
1164 |
1052 |
136.22 |
|
|
|
24 |
B2 |
1005 |
909 |
1.54 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 20463.5 cm
-1
Scaled (by 0.9042) Zero Point Vibrational Energy (zpe) 18503.1 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 HF/6-31+G**
Point Group is C2v
Cartesians (Å)
Atom |
x (Å) |
y (Å) |
z (Å) |
O1 |
0.000 |
0.000 |
1.050 |
C2 |
0.000 |
0.000 |
-1.071 |
C3 |
0.000 |
1.029 |
0.070 |
C4 |
0.000 |
-1.029 |
0.070 |
H5 |
0.883 |
0.000 |
-1.697 |
H6 |
-0.883 |
0.000 |
-1.697 |
H7 |
0.884 |
1.653 |
0.145 |
H8 |
-0.884 |
1.653 |
0.145 |
H9 |
-0.884 |
-1.653 |
0.145 |
H10 |
0.884 |
-1.653 |
0.145 |
Atom - Atom Distances (Å)
|
O1 |
C2 |
C3 |
C4 |
H5 |
H6 |
H7 |
H8 |
H9 |
H10 |
O1 | | 2.1208 | 1.4207 | 1.4207 | 2.8854 | 2.8854 | 2.0814 | 2.0814 | 2.0814 | 2.0814 |
C2 | 2.1208 | | 1.5370 | 1.5370 | 1.0826 | 1.0826 | 2.2343 | 2.2343 | 2.2343 | 2.2343 | C3 | 1.4207 | 1.5370 | | 2.0586 | 2.2280 | 2.2280 | 1.0845 | 1.0845 | 2.8250 | 2.8250 | C4 | 1.4207 | 1.5370 | 2.0586 | | 2.2280 | 2.2280 | 2.8250 | 2.8250 | 1.0845 | 1.0845 | H5 | 2.8854 | 1.0826 | 2.2280 | 2.2280 | | 1.7662 | 2.4748 | 3.0411 | 3.0411 | 2.4748 | H6 | 2.8854 | 1.0826 | 2.2280 | 2.2280 | 1.7662 | | 3.0411 | 2.4748 | 2.4748 | 3.0411 | H7 | 2.0814 | 2.2343 | 1.0845 | 2.8250 | 2.4748 | 3.0411 | | 1.7685 | 3.7488 | 3.3055 | H8 | 2.0814 | 2.2343 | 1.0845 | 2.8250 | 3.0411 | 2.4748 | 1.7685 | | 3.3055 | 3.7488 | H9 | 2.0814 | 2.2343 | 2.8250 | 1.0845 | 3.0411 | 2.4748 | 3.7488 | 3.3055 | | 1.7685 | H10 | 2.0814 | 2.2343 | 2.8250 | 1.0845 | 2.4748 | 3.0411 | 3.3055 | 3.7488 | 1.7685 | |
More geometry information
Calculated Bond Angles
atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
O1 |
C3 |
C2 |
91.534 |
|
O1 |
C3 |
H7 |
111.667 |
O1 |
C3 |
H8 |
111.667 |
|
O1 |
C4 |
C2 |
91.534 |
O1 |
C4 |
H9 |
111.667 |
|
O1 |
C4 |
H10 |
111.667 |
C2 |
C3 |
H7 |
115.843 |
|
C2 |
C3 |
H8 |
115.843 |
C2 |
C4 |
H9 |
115.843 |
|
C2 |
C4 |
H10 |
115.843 |
C3 |
O1 |
C4 |
92.853 |
|
C3 |
C2 |
C4 |
84.080 |
C3 |
C2 |
H5 |
115.440 |
|
C3 |
C2 |
H6 |
115.440 |
C4 |
C2 |
H5 |
115.440 |
|
C4 |
C2 |
H6 |
115.440 |
H5 |
C2 |
H6 |
109.325 |
|
H7 |
C3 |
H8 |
109.245 |
H9 |
C4 |
H10 |
109.245 |
|
Electronic energy levels
Electronic state
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at HF/6-31+G**
Charges (e)
Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
1 |
O |
-0.533 |
|
|
|
2 |
C |
-0.210 |
|
|
|
3 |
C |
0.000 |
|
|
|
4 |
C |
0.000 |
|
|
|
5 |
H |
0.140 |
|
|
|
6 |
H |
0.140 |
|
|
|
7 |
H |
0.115 |
|
|
|
8 |
H |
0.115 |
|
|
|
9 |
H |
0.115 |
|
|
|
10 |
H |
0.115 |
|
|
|
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 |
-2.327 |
2.327 |
CHELPG |
|
|
|
|
AIM |
|
|
|
|
ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
Primitive |
| x | y | z |
x |
-24.315 |
0.000 |
0.000 |
y |
0.000 |
-22.753 |
0.000 |
z |
0.000 |
0.000 |
-28.561 |
|
Traceless |
| x | y | z |
x |
1.342 |
0.000 |
0.000 |
y |
0.000 |
3.685 |
0.000 |
z |
0.000 |
0.000 |
-5.027 |
|
Polar |
3z2-r2 | -10.055 |
x2-y2 | -1.562 |
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 |
4.728 |
0.000 |
0.000 |
y |
0.000 |
5.597 |
0.000 |
z |
0.000 |
0.000 |
4.823 |
<r2> (average value of r
2) Å
2
<r2> |
65.675 |
(<r2>)1/2 |
8.104 |
Jump to
S1C1
Energy calculated at HF/6-31+G**
| hartrees |
Energy at 0K | -191.923474 |
Energy at 298.15K | -191.930904 |
HF Energy | -191.923474 |
Nuclear repulsion energy | 129.355534 |
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/6-31+G**
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' |
3287 |
2972 |
77.30 |
|
|
|
2 |
A' |
3244 |
2933 |
59.89 |
|
|
|
3 |
A' |
3235 |
2925 |
29.95 |
|
|
|
4 |
A' |
3208 |
2901 |
8.02 |
|
|
|
5 |
A' |
1680 |
1519 |
0.08 |
|
|
|
6 |
A' |
1621 |
1466 |
3.34 |
|
|
|
7 |
A' |
1518 |
1372 |
10.03 |
|
|
|
8 |
A' |
1312 |
1186 |
0.06 |
|
|
|
9 |
A' |
1263 |
1142 |
6.85 |
|
|
|
10 |
A' |
1138 |
1029 |
23.39 |
|
|
|
11 |
A' |
1023 |
925 |
36.16 |
|
|
|
12 |
A' |
896 |
810 |
5.34 |
|
|
|
13 |
A' |
825 |
746 |
0.03 |
|
|
|
14 |
A' |
81 |
73 |
6.21 |
|
|
|
15 |
A" |
3248 |
2937 |
0.00 |
|
|
|
16 |
A" |
3201 |
2894 |
173.43 |
|
|
|
17 |
A" |
1651 |
1493 |
3.46 |
|
|
|
18 |
A" |
1439 |
1301 |
0.07 |
|
|
|
19 |
A" |
1392 |
1258 |
8.89 |
|
|
|
20 |
A" |
1337 |
1209 |
0.00 |
|
|
|
21 |
A" |
1263 |
1142 |
0.00 |
|
|
|
22 |
A" |
1164 |
1052 |
136.20 |
|
|
|
23 |
A" |
1005 |
909 |
1.55 |
|
|
|
24 |
A" |
900 |
813 |
0.00 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 20463.5 cm
-1
Scaled (by 0.9042) Zero Point Vibrational Energy (zpe) 18503.1 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 HF/6-31+G**
Point Group is Cs
Cartesians (Å)
Atom |
x (Å) |
y (Å) |
z (Å) |
O1 |
0.000 |
-1.050 |
0.000 |
C2 |
-0.000 |
1.071 |
0.000 |
C3 |
-0.000 |
-0.070 |
1.029 |
C4 |
-0.000 |
-0.070 |
-1.029 |
H5 |
0.883 |
1.697 |
0.000 |
H6 |
-0.883 |
1.697 |
0.000 |
H7 |
0.884 |
-0.145 |
1.653 |
H8 |
-0.884 |
-0.145 |
1.653 |
H9 |
0.884 |
-0.145 |
-1.653 |
H10 |
-0.884 |
-0.145 |
-1.653 |
Atom - Atom Distances (Å)
|
O1 |
C2 |
C3 |
C4 |
H5 |
H6 |
H7 |
H8 |
H9 |
H10 |
O1 | | 2.1208 | 1.4207 | 1.4207 | 2.8854 | 2.8855 | 2.0814 | 2.0814 | 2.0814 | 2.0814 |
C2 | 2.1208 | | 1.5370 | 1.5370 | 1.0826 | 1.0826 | 2.2342 | 2.2342 | 2.2342 | 2.2342 | C3 | 1.4207 | 1.5370 | | 2.0585 | 2.2280 | 2.2280 | 1.0845 | 1.0845 | 2.8250 | 2.8249 | C4 | 1.4207 | 1.5370 | 2.0585 | | 2.2280 | 2.2280 | 2.8250 | 2.8249 | 1.0845 | 1.0845 | H5 | 2.8854 | 1.0826 | 2.2280 | 2.2280 | | 1.7662 | 2.4748 | 3.0411 | 2.4748 | 3.0411 | H6 | 2.8855 | 1.0826 | 2.2280 | 2.2280 | 1.7662 | | 3.0411 | 2.4748 | 3.0411 | 2.4748 | H7 | 2.0814 | 2.2342 | 1.0845 | 2.8250 | 2.4748 | 3.0411 | | 1.7685 | 3.3056 | 3.7488 | H8 | 2.0814 | 2.2342 | 1.0845 | 2.8249 | 3.0411 | 2.4748 | 1.7685 | | 3.7488 | 3.3052 | H9 | 2.0814 | 2.2342 | 2.8250 | 1.0845 | 2.4748 | 3.0411 | 3.3056 | 3.7488 | | 1.7685 | H10 | 2.0814 | 2.2342 | 2.8249 | 1.0845 | 3.0411 | 2.4748 | 3.7488 | 3.3052 | 1.7685 | |
More geometry information
Calculated Bond Angles
atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
O1 |
C3 |
C2 |
91.536 |
|
O1 |
C3 |
H7 |
111.666 |
O1 |
C3 |
H8 |
111.666 |
|
O1 |
C4 |
C2 |
91.536 |
O1 |
C4 |
H9 |
111.666 |
|
O1 |
C4 |
H10 |
111.666 |
C2 |
C3 |
H7 |
115.843 |
|
C2 |
C3 |
H8 |
115.842 |
C2 |
C4 |
H9 |
115.843 |
|
C2 |
C4 |
H10 |
115.842 |
C3 |
O1 |
C4 |
92.849 |
|
C3 |
C2 |
C4 |
84.080 |
C3 |
C2 |
H5 |
115.438 |
|
C3 |
C2 |
H6 |
115.440 |
C4 |
C2 |
H5 |
115.438 |
|
C4 |
C2 |
H6 |
115.440 |
H5 |
C2 |
H6 |
109.328 |
|
H7 |
C3 |
H8 |
109.247 |
H9 |
C4 |
H10 |
109.247 |
|
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at HF/6-31+G**
Charges (e)
Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
1 |
O |
-0.533 |
|
|
|
2 |
C |
-0.210 |
|
|
|
3 |
C |
0.000 |
|
|
|
4 |
C |
0.000 |
|
|
|
5 |
H |
0.140 |
|
|
|
6 |
H |
0.140 |
|
|
|
7 |
H |
0.115 |
|
|
|
8 |
H |
0.115 |
|
|
|
9 |
H |
0.115 |
|
|
|
10 |
H |
0.115 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
|
x |
y |
z |
Total |
|
-0.000 |
2.327 |
0.000 |
2.327 |
CHELPG |
|
|
|
|
AIM |
|
|
|
|
ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
Primitive |
| x | y | z |
x |
-24.315 |
0.001 |
0.000 |
y |
0.001 |
-28.562 |
0.000 |
z |
0.000 |
0.000 |
-22.753 |
|
Traceless |
| x | y | z |
x |
1.343 |
0.001 |
0.000 |
y |
0.001 |
-5.028 |
0.000 |
z |
0.000 |
0.000 |
3.685 |
|
Polar |
3z2-r2 | 7.371 |
x2-y2 | 4.247 |
xy | 0.001 |
xz | 0.000 |
yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
|
x |
y |
z |
x |
4.728 |
0.000 |
0.000 |
y |
0.000 |
4.823 |
0.000 |
z |
0.000 |
0.000 |
5.597 |
<r2> (average value of r
2) Å
2
<r2> |
65.675 |
(<r2>)1/2 |
8.104 |