Jump to
S1C2
Energy calculated at B3PW91/6-311G*
| | hartrees |
| Energy at 0K | -477.975184 |
| Energy at 298.15K | -477.981428 |
| HF Energy | -477.975184 |
| Nuclear repulsion energy | 107.273649 |
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 B3PW91/6-311G*
| 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' |
3118 |
3002 |
28.24 |
|
|
|
| 2 |
A' |
3066 |
2951 |
27.30 |
|
|
|
| 3 |
A' |
3046 |
2932 |
23.19 |
|
|
|
| 4 |
A' |
2640 |
2542 |
14.70 |
|
|
|
| 5 |
A' |
1517 |
1461 |
3.76 |
|
|
|
| 6 |
A' |
1500 |
1444 |
3.05 |
|
|
|
| 7 |
A' |
1424 |
1371 |
6.69 |
|
|
|
| 8 |
A' |
1320 |
1270 |
47.55 |
|
|
|
| 9 |
A' |
1124 |
1082 |
2.38 |
|
|
|
| 10 |
A' |
1006 |
969 |
3.88 |
|
|
|
| 11 |
A' |
867 |
835 |
2.14 |
|
|
|
| 12 |
A' |
680 |
655 |
1.44 |
|
|
|
| 13 |
A' |
302 |
291 |
2.54 |
|
|
|
| 14 |
A" |
3132 |
3016 |
36.54 |
|
|
|
| 15 |
A" |
3107 |
2991 |
0.00 |
|
|
|
| 16 |
A" |
1508 |
1452 |
11.83 |
|
|
|
| 17 |
A" |
1282 |
1234 |
1.88 |
|
|
|
| 18 |
A" |
1060 |
1021 |
1.98 |
|
|
|
| 19 |
A" |
798 |
768 |
7.36 |
|
|
|
| 20 |
A" |
261 |
251 |
1.12 |
|
|
|
| 21 |
A" |
174 |
167 |
23.42 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 16466.2 cm
-1
Scaled (by 0.9627) Zero Point Vibrational Energy (zpe) 15852.0 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 B3PW91/6-311G*
Point Group is Cs
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
1.514 |
0.693 |
0.000 |
| C2 |
0.000 |
0.830 |
0.000 |
| S3 |
-0.755 |
-0.840 |
0.000 |
| H4 |
1.982 |
1.682 |
0.000 |
| H5 |
1.865 |
0.156 |
0.885 |
| H6 |
1.865 |
0.156 |
-0.885 |
| H7 |
-0.333 |
1.374 |
0.886 |
| H8 |
-0.333 |
1.374 |
-0.886 |
| H9 |
-2.045 |
-0.435 |
0.000 |
Atom - Atom Distances (Å)
| |
C1 |
C2 |
S3 |
H4 |
H5 |
H6 |
H7 |
H8 |
H9 |
| C1 | | 1.5204 | 2.7392 | 1.0937 | 1.0931 | 1.0931 | 2.1594 | 2.1594 | 3.7334 |
C2 | 1.5204 | | 1.8332 | 2.1576 | 2.1719 | 2.1719 | 1.0922 | 1.0922 | 2.4043 | S3 | 2.7392 | 1.8332 | | 3.7224 | 2.9402 | 2.9402 | 2.4223 | 2.4223 | 1.3512 | H4 | 1.0937 | 2.1576 | 3.7224 | | 1.7676 | 1.7676 | 2.4986 | 2.4986 | 4.5494 | H5 | 1.0931 | 2.1719 | 2.9402 | 1.7676 | | 1.7696 | 2.5138 | 3.0751 | 4.0522 | H6 | 1.0931 | 2.1719 | 2.9402 | 1.7676 | 1.7696 | | 3.0751 | 2.5138 | 4.0522 | H7 | 2.1594 | 1.0922 | 2.4223 | 2.4986 | 2.5138 | 3.0751 | | 1.7727 | 2.6433 | H8 | 2.1594 | 1.0922 | 2.4223 | 2.4986 | 3.0751 | 2.5138 | 1.7727 | | 2.6433 | H9 | 3.7334 | 2.4043 | 1.3512 | 4.5494 | 4.0522 | 4.0522 | 2.6433 | 2.6433 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| C1 |
C2 |
S3 |
109.175 |
|
C1 |
C2 |
H7 |
110.417 |
| C1 |
C2 |
H8 |
110.417 |
|
C2 |
C1 |
H4 |
110.182 |
| C2 |
C1 |
H5 |
111.360 |
|
C2 |
C1 |
H6 |
111.360 |
| C2 |
S3 |
H9 |
96.888 |
|
S3 |
C2 |
H7 |
109.156 |
| S3 |
C2 |
H8 |
109.156 |
|
H4 |
C1 |
H5 |
107.862 |
| H4 |
C1 |
H6 |
107.862 |
|
H5 |
C1 |
H6 |
108.075 |
| H7 |
C2 |
H8 |
108.494 |
|
Electronic energy levels
Electronic state
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at B3PW91/6-311G*
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
-0.670 |
|
|
|
| 2 |
C |
-0.582 |
|
|
|
| 3 |
S |
-0.117 |
|
|
|
| 4 |
H |
0.232 |
|
|
|
| 5 |
H |
0.240 |
|
|
|
| 6 |
H |
0.240 |
|
|
|
| 7 |
H |
0.252 |
|
|
|
| 8 |
H |
0.252 |
|
|
|
| 9 |
H |
0.153 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
-0.066 |
1.829 |
0.000 |
1.831 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-24.769 |
-0.213 |
0.000 |
| y |
-0.213 |
-28.564 |
0.000 |
| z |
0.000 |
0.000 |
-29.350 |
|
| Traceless |
| | x | y | z |
| x |
4.188 |
-0.213 |
0.000 |
| y |
-0.213 |
-1.505 |
0.000 |
| z |
0.000 |
0.000 |
-2.684 |
|
| Polar |
| 3z2-r2 | -5.367 |
| x2-y2 | 3.795 |
| xy | -0.213 |
| xz | 0.000 |
| yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
6.707 |
0.866 |
0.000 |
| y |
0.866 |
6.410 |
0.000 |
| z |
0.000 |
0.000 |
4.538 |
<r2> (average value of r
2) Å
2
| <r2> |
83.690 |
| (<r2>)1/2 |
9.148 |
Jump to
S1C1
Energy calculated at B3PW91/6-311G*
| | hartrees |
| Energy at 0K | -477.976086 |
| Energy at 298.15K | -477.982405 |
| HF Energy | -477.976086 |
| Nuclear repulsion energy | 106.983351 |
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 B3PW91/6-311G*
| 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 |
3134 |
3017 |
33.72 |
|
|
|
| 2 |
A |
3112 |
2996 |
12.65 |
|
|
|
| 3 |
A |
3102 |
2986 |
24.57 |
|
|
|
| 4 |
A |
3069 |
2955 |
16.31 |
|
|
|
| 5 |
A |
3037 |
2924 |
30.78 |
|
|
|
| 6 |
A |
2638 |
2539 |
13.86 |
|
|
|
| 7 |
A |
1511 |
1455 |
4.77 |
|
|
|
| 8 |
A |
1505 |
1448 |
12.42 |
|
|
|
| 9 |
A |
1489 |
1434 |
2.39 |
|
|
|
| 10 |
A |
1421 |
1368 |
5.61 |
|
|
|
| 11 |
A |
1323 |
1274 |
20.69 |
|
|
|
| 12 |
A |
1294 |
1246 |
6.20 |
|
|
|
| 13 |
A |
1134 |
1092 |
13.01 |
|
|
|
| 14 |
A |
1079 |
1038 |
0.37 |
|
|
|
| 15 |
A |
996 |
959 |
8.81 |
|
|
|
| 16 |
A |
881 |
848 |
8.86 |
|
|
|
| 17 |
A |
742 |
714 |
3.19 |
|
|
|
| 18 |
A |
663 |
639 |
4.31 |
|
|
|
| 19 |
A |
328 |
316 |
1.61 |
|
|
|
| 20 |
A |
269 |
259 |
1.60 |
|
|
|
| 21 |
A |
213 |
205 |
20.62 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 16468.9 cm
-1
Scaled (by 0.9627) Zero Point Vibrational Energy (zpe) 15854.6 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 B3PW91/6-311G*
Point Group is C1
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
1.641 |
-0.349 |
-0.053 |
| C2 |
0.498 |
0.641 |
0.091 |
| S3 |
-1.166 |
-0.100 |
-0.082 |
| H4 |
2.606 |
0.166 |
0.009 |
| H5 |
1.618 |
-1.103 |
0.739 |
| H6 |
1.592 |
-0.871 |
-1.011 |
| H7 |
0.550 |
1.179 |
1.040 |
| H8 |
0.535 |
1.393 |
-0.701 |
| H9 |
-1.086 |
-0.911 |
0.997 |
Atom - Atom Distances (Å)
| |
C1 |
C2 |
S3 |
H4 |
H5 |
H6 |
H7 |
H8 |
H9 |
| C1 | | 1.5187 | 2.8177 | 1.0955 | 1.0938 | 1.0924 | 2.1724 | 2.1629 | 2.9752 |
C2 | 1.5187 | | 1.8300 | 2.1617 | 2.1715 | 2.1671 | 1.0923 | 1.0930 | 2.3958 | S3 | 2.8177 | 1.8300 | | 3.7819 | 3.0703 | 3.0100 | 2.4167 | 2.3471 | 1.3517 | H4 | 1.0955 | 2.1617 | 3.7819 | | 1.7665 | 1.7732 | 2.5130 | 2.5092 | 3.9703 | H5 | 1.0938 | 2.1715 | 3.0703 | 1.7665 | | 1.7658 | 2.5374 | 3.0787 | 2.7224 | H6 | 1.0924 | 2.1671 | 3.0100 | 1.7732 | 1.7658 | | 3.0815 | 2.5177 | 3.3468 | H7 | 2.1724 | 1.0923 | 2.4167 | 2.5130 | 2.5374 | 3.0815 | | 1.7547 | 2.6547 | H8 | 2.1629 | 1.0930 | 2.3471 | 2.5092 | 3.0787 | 2.5177 | 1.7547 | | 3.2897 | H9 | 2.9752 | 2.3958 | 1.3517 | 3.9703 | 2.7224 | 3.3468 | 2.6547 | 3.2897 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| C1 |
C2 |
S3 |
114.262 |
|
C1 |
C2 |
H7 |
111.573 |
| C1 |
C2 |
H8 |
110.766 |
|
C2 |
C1 |
H4 |
110.525 |
| C2 |
C1 |
H5 |
111.407 |
|
C2 |
C1 |
H6 |
111.144 |
| C2 |
S3 |
H9 |
96.541 |
|
S3 |
C2 |
H7 |
108.947 |
| S3 |
C2 |
H8 |
103.959 |
|
H4 |
C1 |
H5 |
107.585 |
| H4 |
C1 |
H6 |
108.290 |
|
H5 |
C1 |
H6 |
107.744 |
| H7 |
C2 |
H8 |
106.825 |
|
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at B3PW91/6-311G*
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
-0.633 |
|
|
|
| 2 |
C |
-0.610 |
|
|
|
| 3 |
S |
-0.112 |
|
|
|
| 4 |
H |
0.223 |
|
|
|
| 5 |
H |
0.223 |
|
|
|
| 6 |
H |
0.244 |
|
|
|
| 7 |
H |
0.255 |
|
|
|
| 8 |
H |
0.257 |
|
|
|
| 9 |
H |
0.152 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
1.654 |
0.072 |
0.848 |
1.860 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-29.510 |
1.522 |
-0.900 |
| y |
1.522 |
-27.412 |
-1.831 |
| z |
-0.900 |
-1.831 |
-27.075 |
|
| Traceless |
| | x | y | z |
| x |
-2.267 |
1.522 |
-0.900 |
| y |
1.522 |
0.880 |
-1.831 |
| z |
-0.900 |
-1.831 |
1.386 |
|
| Polar |
| 3z2-r2 | 2.772 |
| x2-y2 | -2.098 |
| xy | 1.522 |
| xz | -0.900 |
| yz | -1.831 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
7.392 |
0.440 |
0.084 |
| y |
0.440 |
5.381 |
-0.379 |
| z |
0.084 |
-0.379 |
5.182 |
<r2> (average value of r
2) Å
2
| <r2> |
84.415 |
| (<r2>)1/2 |
9.188 |