Jump to
S1C2
Energy calculated at LSDA/cc-pVTZ
| | hartrees |
| Energy at 0K | -476.590227 |
| Energy at 298.15K | -476.596418 |
| HF Energy | -476.590227 |
| Nuclear repulsion energy | 108.261897 |
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 LSDA/cc-pVTZ
| 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' |
3054 |
3020 |
9.45 |
|
|
|
| 2 |
A' |
2986 |
2954 |
17.82 |
|
|
|
| 3 |
A' |
2969 |
2937 |
12.08 |
|
|
|
| 4 |
A' |
2619 |
2591 |
1.81 |
|
|
|
| 5 |
A' |
1426 |
1410 |
4.81 |
|
|
|
| 6 |
A' |
1413 |
1397 |
3.24 |
|
|
|
| 7 |
A' |
1342 |
1328 |
11.42 |
|
|
|
| 8 |
A' |
1232 |
1218 |
22.26 |
|
|
|
| 9 |
A' |
1095 |
1083 |
1.74 |
|
|
|
| 10 |
A' |
987 |
976 |
5.18 |
|
|
|
| 11 |
A' |
826 |
817 |
0.62 |
|
|
|
| 12 |
A' |
689 |
682 |
0.49 |
|
|
|
| 13 |
A' |
293 |
290 |
2.24 |
|
|
|
| 14 |
A" |
3055 |
3022 |
12.32 |
|
|
|
| 15 |
A" |
3029 |
2996 |
0.01 |
|
|
|
| 16 |
A" |
1413 |
1397 |
13.38 |
|
|
|
| 17 |
A" |
1213 |
1199 |
0.90 |
|
|
|
| 18 |
A" |
997 |
986 |
0.24 |
|
|
|
| 19 |
A" |
763 |
754 |
5.22 |
|
|
|
| 20 |
A" |
252 |
250 |
1.62 |
|
|
|
| 21 |
A" |
185 |
183 |
16.07 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 15918.3 cm
-1
Scaled (by 0.9891) Zero Point Vibrational Energy (zpe) 15744.8 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 LSDA/cc-pVTZ
Point Group is Cs
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
1.493 |
0.664 |
0.000 |
| C2 |
0.000 |
0.830 |
0.000 |
| S3 |
-0.744 |
-0.822 |
0.000 |
| H4 |
1.994 |
1.642 |
0.000 |
| H5 |
1.829 |
0.110 |
0.888 |
| H6 |
1.829 |
0.110 |
-0.888 |
| H7 |
-0.334 |
1.378 |
0.892 |
| H8 |
-0.334 |
1.378 |
-0.892 |
| H9 |
-2.040 |
-0.427 |
0.000 |
Atom - Atom Distances (Å)
| |
C1 |
C2 |
S3 |
H4 |
H5 |
H6 |
H7 |
H8 |
H9 |
| C1 | | 1.5017 | 2.6853 | 1.0990 | 1.0998 | 1.0998 | 2.1540 | 2.1540 | 3.6977 |
C2 | 1.5017 | | 1.8114 | 2.1533 | 2.1567 | 2.1567 | 1.0988 | 1.0988 | 2.3962 | S3 | 2.6853 | 1.8114 | | 3.6836 | 2.8767 | 2.8767 | 2.4091 | 2.4091 | 1.3555 | H4 | 1.0990 | 2.1533 | 3.6836 | | 1.7790 | 1.7790 | 2.5067 | 2.5067 | 4.5341 | H5 | 1.0998 | 2.1567 | 2.8767 | 1.7790 | | 1.7765 | 2.5068 | 3.0745 | 4.0059 | H6 | 1.0998 | 2.1567 | 2.8767 | 1.7790 | 1.7765 | | 3.0745 | 2.5068 | 4.0059 | H7 | 2.1540 | 1.0988 | 2.4091 | 2.5067 | 2.5068 | 3.0745 | | 1.7837 | 2.6392 | H8 | 2.1540 | 1.0988 | 2.4091 | 2.5067 | 3.0745 | 2.5068 | 1.7837 | | 2.6392 | H9 | 3.6977 | 2.3962 | 1.3555 | 4.5341 | 4.0059 | 4.0059 | 2.6392 | 2.6392 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| C1 |
C2 |
S3 |
107.926 |
|
C1 |
C2 |
H7 |
110.898 |
| C1 |
C2 |
H8 |
110.898 |
|
C2 |
C1 |
H4 |
110.833 |
| C2 |
C1 |
H5 |
111.054 |
|
C2 |
C1 |
H6 |
111.054 |
| C2 |
S3 |
H9 |
97.289 |
|
S3 |
C2 |
H7 |
109.289 |
| S3 |
C2 |
H8 |
109.289 |
|
H4 |
C1 |
H5 |
108.012 |
| H4 |
C1 |
H6 |
108.012 |
|
H5 |
C1 |
H6 |
107.739 |
| H7 |
C2 |
H8 |
108.517 |
|
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at LSDA/cc-pVTZ
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
-0.349 |
|
|
|
| 2 |
C |
-0.251 |
|
|
|
| 3 |
S |
-0.153 |
|
|
|
| 4 |
H |
0.122 |
|
|
|
| 5 |
H |
0.126 |
|
|
|
| 6 |
H |
0.126 |
|
|
|
| 7 |
H |
0.138 |
|
|
|
| 8 |
H |
0.138 |
|
|
|
| 9 |
H |
0.104 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
0.015 |
1.634 |
0.000 |
1.635 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-25.022 |
-0.172 |
0.000 |
| y |
-0.172 |
-28.305 |
0.000 |
| z |
0.000 |
0.000 |
-29.039 |
|
| Traceless |
| | x | y | z |
| x |
3.650 |
-0.172 |
0.000 |
| y |
-0.172 |
-1.274 |
0.000 |
| z |
0.000 |
0.000 |
-2.376 |
|
| Polar |
| 3z2-r2 | -4.752 |
| x2-y2 | 3.283 |
| xy | -0.172 |
| xz | 0.000 |
| yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
7.637 |
0.896 |
0.000 |
| y |
0.896 |
7.067 |
0.000 |
| z |
0.000 |
0.000 |
5.396 |
<r2> (average value of r
2) Å
2
| <r2> |
81.877 |
| (<r2>)1/2 |
9.049 |
Jump to
S1C1
Energy calculated at LSDA/cc-pVTZ
| | hartrees |
| Energy at 0K | -476.591314 |
| Energy at 298.15K | -476.597564 |
| HF Energy | -476.591314 |
| Nuclear repulsion energy | 107.927640 |
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 LSDA/cc-pVTZ
| 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 |
3059 |
3026 |
11.33 |
|
|
|
| 2 |
A |
3041 |
3008 |
12.23 |
|
|
|
| 3 |
A |
3027 |
2994 |
5.71 |
|
|
|
| 4 |
A |
2987 |
2955 |
10.40 |
|
|
|
| 5 |
A |
2962 |
2930 |
17.61 |
|
|
|
| 6 |
A |
2615 |
2586 |
1.95 |
|
|
|
| 7 |
A |
1420 |
1404 |
4.92 |
|
|
|
| 8 |
A |
1409 |
1394 |
14.36 |
|
|
|
| 9 |
A |
1401 |
1386 |
3.03 |
|
|
|
| 10 |
A |
1338 |
1324 |
10.24 |
|
|
|
| 11 |
A |
1241 |
1227 |
11.59 |
|
|
|
| 12 |
A |
1222 |
1209 |
3.80 |
|
|
|
| 13 |
A |
1087 |
1075 |
2.75 |
|
|
|
| 14 |
A |
1047 |
1035 |
3.06 |
|
|
|
| 15 |
A |
968 |
957 |
6.78 |
|
|
|
| 16 |
A |
839 |
829 |
7.24 |
|
|
|
| 17 |
A |
717 |
709 |
2.95 |
|
|
|
| 18 |
A |
664 |
657 |
2.35 |
|
|
|
| 19 |
A |
324 |
320 |
2.46 |
|
|
|
| 20 |
A |
257 |
254 |
1.10 |
|
|
|
| 21 |
A |
211 |
208 |
14.55 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 15917.2 cm
-1
Scaled (by 0.9891) Zero Point Vibrational Energy (zpe) 15743.7 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 LSDA/cc-pVTZ
Point Group is C1
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
1.612 |
-0.347 |
-0.056 |
| C2 |
0.492 |
0.641 |
0.093 |
| S3 |
-1.149 |
-0.097 |
-0.078 |
| H4 |
2.591 |
0.152 |
0.002 |
| H5 |
1.575 |
-1.105 |
0.740 |
| H6 |
1.544 |
-0.874 |
-1.017 |
| H7 |
0.548 |
1.181 |
1.049 |
| H8 |
0.525 |
1.401 |
-0.702 |
| H9 |
-1.026 |
-0.963 |
0.959 |
Atom - Atom Distances (Å)
| |
C1 |
C2 |
S3 |
H4 |
H5 |
H6 |
H7 |
H8 |
H9 |
| C1 | | 1.5000 | 2.7718 | 1.1010 | 1.1000 | 1.0986 | 2.1645 | 2.1568 | 2.8924 |
C2 | 1.5000 | | 1.8075 | 2.1573 | 2.1536 | 2.1526 | 1.0992 | 1.1002 | 2.3719 | S3 | 2.7718 | 1.8075 | | 3.7494 | 3.0172 | 2.9559 | 2.4046 | 2.3310 | 1.3565 | H4 | 1.1010 | 2.1573 | 3.7494 | | 1.7772 | 1.7856 | 2.5160 | 2.5151 | 3.9043 | H5 | 1.1000 | 2.1536 | 3.0172 | 1.7772 | | 1.7729 | 2.5248 | 3.0757 | 2.6138 | H6 | 1.0986 | 2.1526 | 2.9559 | 1.7856 | 1.7729 | | 3.0795 | 2.5126 | 3.2432 | H7 | 2.1645 | 1.0992 | 2.4046 | 2.5160 | 2.5248 | 3.0795 | | 1.7644 | 2.6610 | H8 | 2.1568 | 1.1002 | 2.3310 | 2.5151 | 3.0757 | 2.5126 | 1.7644 | | 3.2787 | H9 | 2.8924 | 2.3719 | 1.3565 | 3.9043 | 2.6138 | 3.2432 | 2.6610 | 3.2787 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| C1 |
C2 |
S3 |
113.540 |
|
C1 |
C2 |
H7 |
111.843 |
| C1 |
C2 |
H8 |
111.156 |
|
C2 |
C1 |
H4 |
111.145 |
| C2 |
C1 |
H5 |
110.912 |
|
C2 |
C1 |
H6 |
110.916 |
| C2 |
S3 |
H9 |
96.075 |
|
S3 |
C2 |
H7 |
109.208 |
| S3 |
C2 |
H8 |
103.914 |
|
H4 |
C1 |
H5 |
107.695 |
| H4 |
C1 |
H6 |
108.543 |
|
H5 |
C1 |
H6 |
107.486 |
| H7 |
C2 |
H8 |
106.682 |
|
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at LSDA/cc-pVTZ
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
-0.340 |
|
|
|
| 2 |
C |
-0.258 |
|
|
|
| 3 |
S |
-0.145 |
|
|
|
| 4 |
H |
0.118 |
|
|
|
| 5 |
H |
0.118 |
|
|
|
| 6 |
H |
0.130 |
|
|
|
| 7 |
H |
0.143 |
|
|
|
| 8 |
H |
0.135 |
|
|
|
| 9 |
H |
0.100 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
1.519 |
0.108 |
0.672 |
1.665 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-29.222 |
1.267 |
-0.602 |
| y |
1.267 |
-27.177 |
-1.676 |
| z |
-0.602 |
-1.676 |
-27.195 |
|
| Traceless |
| | x | y | z |
| x |
-2.036 |
1.267 |
-0.602 |
| y |
1.267 |
1.032 |
-1.676 |
| z |
-0.602 |
-1.676 |
1.004 |
|
| Polar |
| 3z2-r2 | 2.008 |
| x2-y2 | -2.045 |
| xy | 1.267 |
| xz | -0.602 |
| yz | -1.676 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
8.194 |
0.354 |
0.031 |
| y |
0.354 |
6.262 |
-0.288 |
| z |
0.031 |
-0.288 |
5.879 |
<r2> (average value of r
2) Å
2
| <r2> |
82.656 |
| (<r2>)1/2 |
9.092 |