Jump to
S1C2
Energy calculated at B3PW91/6-311+G(3df,2p)
| | hartrees |
| Energy at 0K | -477.998248 |
| Energy at 298.15K | |
| HF Energy | -477.998248 |
| Nuclear repulsion energy | 107.658792 |
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 B3PW91/6-311+G(3df,2p)
| 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' |
3111 |
2978 |
20.38 |
|
|
|
| 2 |
A' |
3058 |
2927 |
18.47 |
|
|
|
| 3 |
A' |
3038 |
2908 |
18.96 |
|
|
|
| 4 |
A' |
2691 |
2576 |
2.37 |
|
|
|
| 5 |
A' |
1497 |
1433 |
3.44 |
|
|
|
| 6 |
A' |
1483 |
1420 |
3.24 |
|
|
|
| 7 |
A' |
1407 |
1347 |
4.10 |
|
|
|
| 8 |
A' |
1291 |
1236 |
27.79 |
|
|
|
| 9 |
A' |
1112 |
1064 |
1.20 |
|
|
|
| 10 |
A' |
998 |
955 |
3.96 |
|
|
|
| 11 |
A' |
860 |
824 |
0.86 |
|
|
|
| 12 |
A' |
683 |
654 |
1.11 |
|
|
|
| 13 |
A' |
299 |
287 |
2.00 |
|
|
|
| 14 |
A" |
3122 |
2989 |
21.48 |
|
|
|
| 15 |
A" |
3098 |
2965 |
0.27 |
|
|
|
| 16 |
A" |
1487 |
1424 |
10.12 |
|
|
|
| 17 |
A" |
1263 |
1209 |
0.44 |
|
|
|
| 18 |
A" |
1041 |
996 |
0.34 |
|
|
|
| 19 |
A" |
786 |
752 |
3.61 |
|
|
|
| 20 |
A" |
248 |
238 |
0.79 |
|
|
|
| 21 |
A" |
166 |
159 |
13.85 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 16369.6 cm
-1
Scaled (by 0.9573) Zero Point Vibrational Energy (zpe) 15670.6 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 B3PW91/6-311+G(3df,2p)
Point Group is Cs
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
1.512 |
0.684 |
0.000 |
| C2 |
0.000 |
0.828 |
0.000 |
| S3 |
-0.754 |
-0.833 |
0.000 |
| H4 |
1.983 |
1.669 |
0.000 |
| H5 |
1.858 |
0.145 |
0.883 |
| H6 |
1.858 |
0.145 |
-0.883 |
| H7 |
-0.334 |
1.369 |
0.885 |
| H8 |
-0.334 |
1.369 |
-0.885 |
| H9 |
-2.038 |
-0.439 |
0.000 |
Atom - Atom Distances (Å)
| |
C1 |
C2 |
S3 |
H4 |
H5 |
H6 |
H7 |
H8 |
H9 |
| C1 | | 1.5193 | 2.7277 | 1.0914 | 1.0912 | 1.0912 | 2.1590 | 2.1590 | 3.7235 |
C2 | 1.5193 | | 1.8241 | 2.1540 | 2.1678 | 2.1678 | 1.0899 | 1.0899 | 2.3994 | S3 | 2.7277 | 1.8241 | | 3.7085 | 2.9259 | 2.9259 | 2.4104 | 2.4104 | 1.3424 | H4 | 1.0914 | 2.1540 | 3.7085 | | 1.7660 | 1.7660 | 2.4982 | 2.4982 | 4.5397 | H5 | 1.0912 | 2.1678 | 2.9259 | 1.7660 | | 1.7667 | 2.5106 | 3.0710 | 4.0370 | H6 | 1.0912 | 2.1678 | 2.9259 | 1.7660 | 1.7667 | | 3.0710 | 2.5106 | 4.0370 | H7 | 2.1590 | 1.0899 | 2.4104 | 2.4982 | 2.5106 | 3.0710 | | 1.7704 | 2.6375 | H8 | 2.1590 | 1.0899 | 2.4104 | 2.4982 | 3.0710 | 2.5106 | 1.7704 | | 2.6375 | H9 | 3.7235 | 2.3994 | 1.3424 | 4.5397 | 4.0370 | 4.0370 | 2.6375 | 2.6375 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| C1 |
C2 |
S3 |
109.000 |
|
C1 |
C2 |
H7 |
110.599 |
| C1 |
C2 |
H8 |
110.599 |
|
C2 |
C1 |
H4 |
110.112 |
| C2 |
C1 |
H5 |
111.227 |
|
C2 |
C1 |
H6 |
111.227 |
| C2 |
S3 |
H9 |
97.362 |
|
S3 |
C2 |
H7 |
108.997 |
| S3 |
C2 |
H8 |
108.997 |
|
H4 |
C1 |
H5 |
108.027 |
| H4 |
C1 |
H6 |
108.027 |
|
H5 |
C1 |
H6 |
108.098 |
| H7 |
C2 |
H8 |
108.615 |
|
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at B3PW91/6-311+G(3df,2p)
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
-0.344 |
|
|
|
| 2 |
C |
-0.252 |
|
|
|
| 3 |
S |
-0.316 |
|
|
|
| 4 |
H |
0.137 |
|
|
|
| 5 |
H |
0.157 |
|
|
|
| 6 |
H |
0.157 |
|
|
|
| 7 |
H |
0.154 |
|
|
|
| 8 |
H |
0.154 |
|
|
|
| 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 |
| |
0.112 |
1.667 |
0.000 |
1.670 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-24.941 |
-0.280 |
0.000 |
| y |
-0.280 |
-28.156 |
0.000 |
| z |
0.000 |
0.000 |
-28.986 |
|
| Traceless |
| | x | y | z |
| x |
3.630 |
-0.280 |
0.000 |
| y |
-0.280 |
-1.192 |
0.000 |
| z |
0.000 |
0.000 |
-2.438 |
|
| Polar |
| 3z2-r2 | -4.877 |
| x2-y2 | 3.215 |
| xy | -0.280 |
| xz | 0.000 |
| yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
7.678 |
0.919 |
0.000 |
| y |
0.919 |
7.319 |
0.000 |
| z |
0.000 |
0.000 |
6.312 |
<r2> (average value of r
2) Å
2
| <r2> |
83.051 |
| (<r2>)1/2 |
9.113 |
Jump to
S1C1
Energy calculated at B3PW91/6-311+G(3df,2p)
| | hartrees |
| Energy at 0K | -477.999150 |
| Energy at 298.15K | |
| HF Energy | -477.999150 |
| Nuclear repulsion energy | 107.359376 |
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 B3PW91/6-311+G(3df,2p)
| 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 |
3124 |
2991 |
21.87 |
11.89 |
0.75 |
0.86 |
| 2 |
A |
3101 |
2969 |
15.24 |
70.45 |
0.72 |
0.83 |
| 3 |
A |
3094 |
2962 |
11.58 |
103.23 |
0.70 |
0.82 |
| 4 |
A |
3057 |
2927 |
11.17 |
125.16 |
0.08 |
0.15 |
| 5 |
A |
3030 |
2901 |
25.26 |
176.27 |
0.04 |
0.08 |
| 6 |
A |
2692 |
2577 |
2.18 |
107.66 |
0.22 |
0.36 |
| 7 |
A |
1492 |
1429 |
3.36 |
3.05 |
0.75 |
0.86 |
| 8 |
A |
1485 |
1421 |
10.93 |
4.99 |
0.74 |
0.85 |
| 9 |
A |
1471 |
1408 |
2.06 |
7.51 |
0.72 |
0.84 |
| 10 |
A |
1405 |
1345 |
4.67 |
0.45 |
0.74 |
0.85 |
| 11 |
A |
1301 |
1245 |
16.38 |
1.83 |
0.33 |
0.49 |
| 12 |
A |
1276 |
1221 |
3.67 |
1.69 |
0.75 |
0.86 |
| 13 |
A |
1119 |
1072 |
6.27 |
3.12 |
0.34 |
0.51 |
| 14 |
A |
1065 |
1020 |
0.31 |
3.75 |
0.18 |
0.31 |
| 15 |
A |
989 |
947 |
7.05 |
3.35 |
0.75 |
0.86 |
| 16 |
A |
874 |
837 |
5.64 |
1.61 |
0.31 |
0.47 |
| 17 |
A |
734 |
703 |
1.95 |
2.86 |
0.20 |
0.34 |
| 18 |
A |
665 |
637 |
2.74 |
10.99 |
0.20 |
0.33 |
| 19 |
A |
327 |
313 |
1.22 |
1.26 |
0.22 |
0.36 |
| 20 |
A |
256 |
245 |
1.82 |
0.16 |
0.40 |
0.58 |
| 21 |
A |
213 |
204 |
12.30 |
0.58 |
0.66 |
0.79 |
Unscaled Zero Point Vibrational Energy (zpe) 16384.8 cm
-1
Scaled (by 0.9573) Zero Point Vibrational Energy (zpe) 15685.2 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 B3PW91/6-311+G(3df,2p)
Point Group is C1
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
1.637 |
-0.347 |
-0.052 |
| C2 |
0.493 |
0.639 |
0.091 |
| S3 |
-1.161 |
-0.100 |
-0.081 |
| H4 |
2.598 |
0.169 |
0.015 |
| H5 |
1.608 |
-1.101 |
0.737 |
| H6 |
1.591 |
-0.865 |
-1.011 |
| H7 |
0.544 |
1.174 |
1.040 |
| H8 |
0.528 |
1.391 |
-0.700 |
| H9 |
-1.085 |
-0.918 |
0.982 |
Atom - Atom Distances (Å)
| |
C1 |
C2 |
S3 |
H4 |
H5 |
H6 |
H7 |
H8 |
H9 |
| C1 | | 1.5174 | 2.8088 | 1.0933 | 1.0914 | 1.0903 | 2.1689 | 2.1614 | 2.9675 |
C2 | 1.5174 | | 1.8199 | 2.1581 | 2.1652 | 2.1638 | 1.0904 | 1.0915 | 2.3896 | S3 | 2.8088 | 1.8199 | | 3.7697 | 3.0554 | 3.0035 | 2.4050 | 2.3360 | 1.3427 | H4 | 1.0933 | 2.1581 | 3.7697 | | 1.7649 | 1.7710 | 2.5065 | 2.5080 | 3.9604 | H5 | 1.0914 | 2.1652 | 3.0554 | 1.7649 | | 1.7632 | 2.5301 | 3.0724 | 2.7107 | H6 | 1.0903 | 2.1638 | 3.0035 | 1.7710 | 1.7632 | | 3.0759 | 2.5134 | 3.3368 | H7 | 2.1689 | 1.0904 | 2.4050 | 2.5065 | 2.5301 | 3.0759 | | 1.7532 | 2.6520 | H8 | 2.1614 | 1.0915 | 2.3360 | 2.5080 | 3.0724 | 2.5134 | 1.7532 | | 3.2801 | H9 | 2.9675 | 2.3896 | 1.3427 | 3.9604 | 2.7107 | 3.3368 | 2.6520 | 3.2801 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| C1 |
C2 |
S3 |
114.322 |
|
C1 |
C2 |
H7 |
111.501 |
| C1 |
C2 |
H8 |
110.828 |
|
C2 |
C1 |
H4 |
110.455 |
| C2 |
C1 |
H5 |
111.139 |
|
C2 |
C1 |
H6 |
111.097 |
| C2 |
S3 |
H9 |
96.996 |
|
S3 |
C2 |
H7 |
108.862 |
| S3 |
C2 |
H8 |
103.886 |
|
H4 |
C1 |
H5 |
107.778 |
| H4 |
C1 |
H6 |
108.405 |
|
H5 |
C1 |
H6 |
107.843 |
| H7 |
C2 |
H8 |
106.939 |
|
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at B3PW91/6-311+G(3df,2p)
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
-0.269 |
|
|
|
| 2 |
C |
-0.303 |
|
|
|
| 3 |
S |
-0.289 |
|
|
|
| 4 |
H |
0.134 |
|
|
|
| 5 |
H |
0.141 |
|
|
|
| 6 |
H |
0.151 |
|
|
|
| 7 |
H |
0.150 |
|
|
|
| 8 |
H |
0.146 |
|
|
|
| 9 |
H |
0.138 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
1.559 |
0.166 |
0.660 |
1.701 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-29.073 |
1.261 |
-0.643 |
| y |
1.261 |
-27.178 |
-1.693 |
| z |
-0.643 |
-1.693 |
-26.924 |
|
| Traceless |
| | x | y | z |
| x |
-2.021 |
1.261 |
-0.643 |
| y |
1.261 |
0.820 |
-1.693 |
| z |
-0.643 |
-1.693 |
1.201 |
|
| Polar |
| 3z2-r2 | 2.403 |
| x2-y2 | -1.894 |
| xy | 1.261 |
| xz | -0.643 |
| yz | -1.693 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
8.452 |
0.218 |
-0.063 |
| y |
0.218 |
6.703 |
0.038 |
| z |
-0.063 |
0.038 |
6.286 |
<r2> (average value of r
2) Å
2
| <r2> |
83.783 |
| (<r2>)1/2 |
9.153 |