Jump to
S1C2
Energy calculated at HF/6-311G*
| | hartrees |
| Energy at 0K | -476.772259 |
| Energy at 298.15K | -476.778697 |
| HF Energy | -476.772259 |
| Nuclear repulsion energy | 107.595038 |
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/6-311G*
| 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' |
3250 |
2940 |
60.62 |
|
|
|
| 2 |
A' |
3224 |
2916 |
21.37 |
|
|
|
| 3 |
A' |
3187 |
2883 |
33.40 |
|
|
|
| 4 |
A' |
2827 |
2557 |
16.92 |
|
|
|
| 5 |
A' |
1637 |
1481 |
1.54 |
|
|
|
| 6 |
A' |
1629 |
1473 |
3.51 |
|
|
|
| 7 |
A' |
1551 |
1403 |
2.41 |
|
|
|
| 8 |
A' |
1444 |
1306 |
58.56 |
|
|
|
| 9 |
A' |
1211 |
1095 |
3.17 |
|
|
|
| 10 |
A' |
1059 |
958 |
2.62 |
|
|
|
| 11 |
A' |
946 |
855 |
3.53 |
|
|
|
| 12 |
A' |
721 |
652 |
3.73 |
|
|
|
| 13 |
A' |
327 |
296 |
2.51 |
|
|
|
| 14 |
A" |
3280 |
2966 |
50.92 |
|
|
|
| 15 |
A" |
3249 |
2938 |
9.16 |
|
|
|
| 16 |
A" |
1628 |
1473 |
7.98 |
|
|
|
| 17 |
A" |
1389 |
1256 |
1.09 |
|
|
|
| 18 |
A" |
1151 |
1041 |
2.24 |
|
|
|
| 19 |
A" |
854 |
772 |
4.17 |
|
|
|
| 20 |
A" |
272 |
246 |
2.33 |
|
|
|
| 21 |
A" |
199 |
180 |
23.57 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 17517.9 cm
-1
Scaled (by 0.9044) Zero Point Vibrational Energy (zpe) 15843.1 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/6-311G*
Point Group is Cs
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
1.518 |
0.697 |
0.000 |
| C2 |
0.000 |
0.825 |
0.000 |
| S3 |
-0.757 |
-0.838 |
0.000 |
| H4 |
1.973 |
1.682 |
0.000 |
| H5 |
1.867 |
0.166 |
0.878 |
| H6 |
1.867 |
0.166 |
-0.878 |
| H7 |
-0.333 |
1.362 |
0.878 |
| H8 |
-0.333 |
1.362 |
-0.878 |
| H9 |
-2.034 |
-0.458 |
0.000 |
Atom - Atom Distances (Å)
| |
C1 |
C2 |
S3 |
H4 |
H5 |
H6 |
H7 |
H8 |
H9 |
| C1 | | 1.5233 | 2.7446 | 1.0847 | 1.0840 | 1.0840 | 2.1535 | 2.1535 | 3.7346 |
C2 | 1.5233 | | 1.8279 | 2.1506 | 2.1664 | 2.1664 | 1.0813 | 1.0813 | 2.4049 | S3 | 2.7446 | 1.8279 | | 3.7152 | 2.9443 | 2.9443 | 2.4069 | 2.4069 | 1.3317 | H4 | 1.0847 | 2.1506 | 3.7152 | | 1.7547 | 1.7547 | 2.4876 | 2.4876 | 4.5422 | H5 | 1.0840 | 2.1664 | 2.9443 | 1.7547 | | 1.7560 | 2.5045 | 3.0585 | 4.0471 | H6 | 1.0840 | 2.1664 | 2.9443 | 1.7547 | 1.7560 | | 3.0585 | 2.5045 | 4.0471 | H7 | 2.1535 | 1.0813 | 2.4069 | 2.4876 | 2.5045 | 3.0585 | | 1.7551 | 2.6416 | H8 | 2.1535 | 1.0813 | 2.4069 | 2.4876 | 3.0585 | 2.5045 | 1.7551 | | 2.6416 | H9 | 3.7346 | 2.4049 | 1.3317 | 4.5422 | 4.0471 | 4.0471 | 2.6416 | 2.6416 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| C1 |
C2 |
S3 |
109.636 |
|
C1 |
C2 |
H7 |
110.398 |
| C1 |
C2 |
H8 |
110.398 |
|
C2 |
C1 |
H4 |
109.965 |
| C2 |
C1 |
H5 |
111.267 |
|
C2 |
C1 |
H6 |
111.267 |
| C2 |
S3 |
H9 |
97.900 |
|
S3 |
C2 |
H7 |
108.933 |
| S3 |
C2 |
H8 |
108.933 |
|
H4 |
C1 |
H5 |
108.017 |
| H4 |
C1 |
H6 |
108.017 |
|
H5 |
C1 |
H6 |
108.187 |
| H7 |
C2 |
H8 |
108.505 |
|
Electronic energy levels
Electronic state
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at HF/6-311G*
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
-0.624 |
|
|
|
| 2 |
C |
-0.534 |
|
|
|
| 3 |
S |
-0.117 |
|
|
|
| 4 |
H |
0.218 |
|
|
|
| 5 |
H |
0.225 |
|
|
|
| 6 |
H |
0.225 |
|
|
|
| 7 |
H |
0.237 |
|
|
|
| 8 |
H |
0.237 |
|
|
|
| 9 |
H |
0.134 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
-0.050 |
1.922 |
0.000 |
1.923 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
-0.030 |
1.910 |
0.000 |
1.911 |
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-25.165 |
-0.221 |
0.000 |
| y |
-0.221 |
-29.036 |
0.000 |
| z |
0.000 |
0.000 |
-29.666 |
|
| Traceless |
| | x | y | z |
| x |
4.185 |
-0.221 |
0.000 |
| y |
-0.221 |
-1.620 |
0.000 |
| z |
0.000 |
0.000 |
-2.565 |
|
| Polar |
| 3z2-r2 | -5.130 |
| x2-y2 | 3.871 |
| xy | -0.221 |
| xz | 0.000 |
| yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
6.355 |
0.842 |
0.000 |
| y |
0.842 |
6.145 |
0.000 |
| z |
0.000 |
0.000 |
4.375 |
<r2> (average value of r
2) Å
2
| <r2> |
83.814 |
| (<r2>)1/2 |
9.155 |
Jump to
S1C1
Energy calculated at HF/6-311G*
| | hartrees |
| Energy at 0K | -476.772793 |
| Energy at 298.15K | -476.779280 |
| HF Energy | -476.772793 |
| Nuclear repulsion energy | 107.343338 |
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/6-311G*
| 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 |
3278 |
2964 |
50.39 |
|
|
|
| 2 |
A |
3252 |
2941 |
15.07 |
|
|
|
| 3 |
A |
3238 |
2928 |
65.87 |
|
|
|
| 4 |
A |
3222 |
2914 |
6.31 |
|
|
|
| 5 |
A |
3180 |
2876 |
39.98 |
|
|
|
| 6 |
A |
2822 |
2552 |
15.33 |
|
|
|
| 7 |
A |
1631 |
1475 |
2.88 |
|
|
|
| 8 |
A |
1626 |
1471 |
8.40 |
|
|
|
| 9 |
A |
1615 |
1461 |
1.37 |
|
|
|
| 10 |
A |
1550 |
1402 |
2.14 |
|
|
|
| 11 |
A |
1448 |
1309 |
28.98 |
|
|
|
| 12 |
A |
1402 |
1268 |
4.28 |
|
|
|
| 13 |
A |
1231 |
1114 |
16.78 |
|
|
|
| 14 |
A |
1159 |
1048 |
0.53 |
|
|
|
| 15 |
A |
1053 |
952 |
5.83 |
|
|
|
| 16 |
A |
950 |
859 |
8.81 |
|
|
|
| 17 |
A |
792 |
716 |
1.68 |
|
|
|
| 18 |
A |
711 |
643 |
7.52 |
|
|
|
| 19 |
A |
352 |
318 |
1.35 |
|
|
|
| 20 |
A |
278 |
251 |
2.05 |
|
|
|
| 21 |
A |
225 |
203 |
21.51 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 17507.1 cm
-1
Scaled (by 0.9044) Zero Point Vibrational Energy (zpe) 15833.4 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/6-311G*
Point Group is C1
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
1.642 |
-0.350 |
-0.050 |
| C2 |
0.495 |
0.642 |
0.089 |
| S3 |
-1.162 |
-0.101 |
-0.082 |
| H4 |
2.595 |
0.165 |
0.024 |
| H5 |
1.611 |
-1.101 |
0.732 |
| H6 |
1.603 |
-0.860 |
-1.004 |
| H7 |
0.545 |
1.170 |
1.031 |
| H8 |
0.538 |
1.386 |
-0.697 |
| H9 |
-1.119 |
-0.888 |
0.993 |
Atom - Atom Distances (Å)
| |
C1 |
C2 |
S3 |
H4 |
H5 |
H6 |
H7 |
H8 |
H9 |
| C1 | | 1.5222 | 2.8155 | 1.0861 | 1.0848 | 1.0831 | 2.1637 | 2.1563 | 3.0002 |
C2 | 1.5222 | | 1.8246 | 2.1541 | 2.1670 | 2.1626 | 1.0815 | 1.0825 | 2.4009 | S3 | 2.8155 | 1.8246 | | 3.7685 | 3.0582 | 3.0121 | 2.4022 | 2.3409 | 1.3322 | H4 | 1.0861 | 2.1541 | 3.7685 | | 1.7535 | 1.7592 | 2.4951 | 2.4982 | 3.9807 | H5 | 1.0848 | 2.1670 | 3.0582 | 1.7535 | | 1.7530 | 2.5268 | 3.0622 | 2.7509 | H6 | 1.0831 | 2.1626 | 3.0121 | 1.7592 | 1.7530 | | 3.0633 | 2.5047 | 3.3762 | H7 | 2.1637 | 1.0815 | 2.4022 | 2.4951 | 2.5268 | 3.0633 | | 1.7407 | 2.6474 | H8 | 2.1563 | 1.0825 | 2.3409 | 2.4982 | 3.0622 | 2.5047 | 1.7407 | | 3.2816 | H9 | 3.0002 | 2.4009 | 1.3322 | 3.9807 | 2.7509 | 3.3762 | 2.6474 | 3.2816 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| C1 |
C2 |
S3 |
114.240 |
|
C1 |
C2 |
H7 |
111.281 |
| C1 |
C2 |
H8 |
110.624 |
|
C2 |
C1 |
H4 |
110.231 |
| C2 |
C1 |
H5 |
111.347 |
|
C2 |
C1 |
H6 |
111.093 |
| C2 |
S3 |
H9 |
97.805 |
|
S3 |
C2 |
H7 |
108.800 |
| S3 |
C2 |
H8 |
104.345 |
|
H4 |
C1 |
H5 |
107.750 |
| H4 |
C1 |
H6 |
108.378 |
|
H5 |
C1 |
H6 |
107.918 |
| H7 |
C2 |
H8 |
107.107 |
|
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at HF/6-311G*
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
-0.589 |
|
|
|
| 2 |
C |
-0.557 |
|
|
|
| 3 |
S |
-0.115 |
|
|
|
| 4 |
H |
0.210 |
|
|
|
| 5 |
H |
0.208 |
|
|
|
| 6 |
H |
0.229 |
|
|
|
| 7 |
H |
0.240 |
|
|
|
| 8 |
H |
0.241 |
|
|
|
| 9 |
H |
0.132 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
1.736 |
0.107 |
0.883 |
1.951 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-30.029 |
1.602 |
-1.019 |
| y |
1.602 |
-27.797 |
-1.811 |
| z |
-1.019 |
-1.811 |
-27.373 |
|
| Traceless |
| | x | y | z |
| x |
-2.444 |
1.602 |
-1.019 |
| y |
1.602 |
0.903 |
-1.811 |
| z |
-1.019 |
-1.811 |
1.540 |
|
| Polar |
| 3z2-r2 | 3.081 |
| x2-y2 | -2.231 |
| xy | 1.602 |
| xz | -1.019 |
| yz | -1.811 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
6.922 |
0.504 |
0.063 |
| y |
0.504 |
5.142 |
-0.383 |
| z |
0.063 |
-0.383 |
4.998 |
<r2> (average value of r
2) Å
2
| <r2> |
84.417 |
| (<r2>)1/2 |
9.188 |