Jump to
S1C2
Energy calculated at PBE1PBE/6-311G**
| | hartrees |
| Energy at 0K | -477.802254 |
| Energy at 298.15K | |
| HF Energy | -477.802254 |
| Nuclear repulsion energy | 107.486871 |
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 PBE1PBE/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' |
3133 |
3005 |
21.66 |
|
|
|
| 2 |
A' |
3079 |
2954 |
22.42 |
|
|
|
| 3 |
A' |
3055 |
2931 |
18.52 |
|
|
|
| 4 |
A' |
2708 |
2598 |
5.14 |
|
|
|
| 5 |
A' |
1500 |
1439 |
3.28 |
|
|
|
| 6 |
A' |
1486 |
1425 |
2.51 |
|
|
|
| 7 |
A' |
1412 |
1355 |
6.32 |
|
|
|
| 8 |
A' |
1311 |
1257 |
43.31 |
|
|
|
| 9 |
A' |
1123 |
1077 |
2.21 |
|
|
|
| 10 |
A' |
1011 |
970 |
3.97 |
|
|
|
| 11 |
A' |
867 |
832 |
2.03 |
|
|
|
| 12 |
A' |
689 |
661 |
1.36 |
|
|
|
| 13 |
A' |
303 |
291 |
2.52 |
|
|
|
| 14 |
A" |
3146 |
3018 |
27.07 |
|
|
|
| 15 |
A" |
3122 |
2995 |
0.17 |
|
|
|
| 16 |
A" |
1489 |
1428 |
10.84 |
|
|
|
| 17 |
A" |
1273 |
1222 |
1.65 |
|
|
|
| 18 |
A" |
1054 |
1011 |
1.50 |
|
|
|
| 19 |
A" |
794 |
762 |
6.80 |
|
|
|
| 20 |
A" |
257 |
247 |
1.05 |
|
|
|
| 21 |
A" |
164 |
157 |
22.68 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 16487.4 cm
-1
Scaled (by 0.9594) Zero Point Vibrational Energy (zpe) 15818.0 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 PBE1PBE/6-311G**
Point Group is Cs
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
1.512 |
0.690 |
0.000 |
| C2 |
0.000 |
0.829 |
0.000 |
| S3 |
-0.754 |
-0.837 |
0.000 |
| H4 |
1.980 |
1.678 |
0.000 |
| H5 |
1.860 |
0.151 |
0.885 |
| H6 |
1.860 |
0.151 |
-0.885 |
| H7 |
-0.334 |
1.370 |
0.887 |
| H8 |
-0.334 |
1.370 |
-0.887 |
| H9 |
-2.040 |
-0.438 |
0.000 |
Atom - Atom Distances (Å)
| |
C1 |
C2 |
S3 |
H4 |
H5 |
H6 |
H7 |
H8 |
H9 |
| C1 | | 1.5179 | 2.7322 | 1.0935 | 1.0932 | 1.0932 | 2.1577 | 2.1577 | 3.7265 |
C2 | 1.5179 | | 1.8288 | 2.1545 | 2.1682 | 2.1682 | 1.0919 | 1.0919 | 2.4016 | S3 | 2.7322 | 1.8288 | | 3.7150 | 2.9311 | 2.9311 | 2.4162 | 2.4162 | 1.3467 | H4 | 1.0935 | 2.1545 | 3.7150 | | 1.7689 | 1.7689 | 2.4972 | 2.4972 | 4.5432 | H5 | 1.0932 | 2.1682 | 2.9311 | 1.7689 | | 1.7704 | 2.5095 | 3.0724 | 4.0422 | H6 | 1.0932 | 2.1682 | 2.9311 | 1.7689 | 1.7704 | | 3.0724 | 2.5095 | 4.0422 | H7 | 2.1577 | 1.0919 | 2.4162 | 2.4972 | 2.5095 | 3.0724 | | 1.7748 | 2.6402 | H8 | 2.1577 | 1.0919 | 2.4162 | 2.4972 | 3.0724 | 2.5095 | 1.7748 | | 2.6402 | H9 | 3.7265 | 2.4016 | 1.3467 | 4.5432 | 4.0422 | 4.0422 | 2.6402 | 2.6402 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| C1 |
C2 |
S3 |
109.097 |
|
C1 |
C2 |
H7 |
110.473 |
| C1 |
C2 |
H8 |
110.473 |
|
C2 |
C1 |
H4 |
110.127 |
| C2 |
C1 |
H5 |
111.237 |
|
C2 |
C1 |
H6 |
111.237 |
| C2 |
S3 |
H9 |
97.109 |
|
S3 |
C2 |
H7 |
109.019 |
| S3 |
C2 |
H8 |
109.019 |
|
H4 |
C1 |
H5 |
107.989 |
| H4 |
C1 |
H6 |
107.989 |
|
H5 |
C1 |
H6 |
108.138 |
| H7 |
C2 |
H8 |
108.729 |
|
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at PBE1PBE/6-311G**
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
-0.367 |
|
|
|
| 2 |
C |
-0.423 |
|
|
|
| 3 |
S |
-0.059 |
|
|
|
| 4 |
H |
0.136 |
|
|
|
| 5 |
H |
0.145 |
|
|
|
| 6 |
H |
0.145 |
|
|
|
| 7 |
H |
0.169 |
|
|
|
| 8 |
H |
0.169 |
|
|
|
| 9 |
H |
0.083 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
-0.047 |
1.813 |
0.000 |
1.814 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-24.754 |
-0.197 |
0.000 |
| y |
-0.197 |
-28.566 |
0.000 |
| z |
0.000 |
0.000 |
-29.330 |
|
| Traceless |
| | x | y | z |
| x |
4.194 |
-0.197 |
0.000 |
| y |
-0.197 |
-1.524 |
0.000 |
| z |
0.000 |
0.000 |
-2.670 |
|
| Polar |
| 3z2-r2 | -5.341 |
| x2-y2 | 3.812 |
| xy | -0.197 |
| xz | 0.000 |
| yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
6.808 |
0.876 |
0.000 |
| y |
0.876 |
6.486 |
0.000 |
| z |
0.000 |
0.000 |
4.660 |
<r2> (average value of r
2) Å
2
| <r2> |
83.379 |
| (<r2>)1/2 |
9.131 |
Jump to
S1C1
Energy calculated at PBE1PBE/6-311G**
| | hartrees |
| Energy at 0K | -477.803245 |
| Energy at 298.15K | -477.809591 |
| HF Energy | -477.803245 |
| Nuclear repulsion energy | 107.229625 |
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 PBE1PBE/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 |
3147 |
3019 |
25.40 |
|
|
|
| 2 |
A |
3126 |
2999 |
11.51 |
|
|
|
| 3 |
A |
3117 |
2990 |
17.79 |
|
|
|
| 4 |
A |
3081 |
2956 |
14.02 |
|
|
|
| 5 |
A |
3048 |
2924 |
23.89 |
|
|
|
| 6 |
A |
2707 |
2597 |
5.09 |
|
|
|
| 7 |
A |
1494 |
1433 |
3.95 |
|
|
|
| 8 |
A |
1487 |
1426 |
11.40 |
|
|
|
| 9 |
A |
1475 |
1415 |
1.94 |
|
|
|
| 10 |
A |
1410 |
1352 |
5.26 |
|
|
|
| 11 |
A |
1315 |
1262 |
20.92 |
|
|
|
| 12 |
A |
1284 |
1232 |
4.89 |
|
|
|
| 13 |
A |
1129 |
1083 |
10.70 |
|
|
|
| 14 |
A |
1079 |
1035 |
0.62 |
|
|
|
| 15 |
A |
1000 |
959 |
8.42 |
|
|
|
| 16 |
A |
878 |
842 |
8.66 |
|
|
|
| 17 |
A |
743 |
713 |
3.18 |
|
|
|
| 18 |
A |
674 |
647 |
3.94 |
|
|
|
| 19 |
A |
330 |
317 |
2.00 |
|
|
|
| 20 |
A |
269 |
258 |
1.50 |
|
|
|
| 21 |
A |
219 |
210 |
19.39 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 16505.1 cm
-1
Scaled (by 0.9594) Zero Point Vibrational Energy (zpe) 15835.0 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 PBE1PBE/6-311G**
Point Group is C1
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
1.636 |
-0.349 |
-0.053 |
| C2 |
0.496 |
0.641 |
0.092 |
| S3 |
-1.162 |
-0.099 |
-0.080 |
| H4 |
2.600 |
0.166 |
0.009 |
| H5 |
1.608 |
-1.102 |
0.739 |
| H6 |
1.583 |
-0.869 |
-1.012 |
| H7 |
0.549 |
1.176 |
1.042 |
| H8 |
0.533 |
1.393 |
-0.701 |
| H9 |
-1.071 |
-0.929 |
0.978 |
Atom - Atom Distances (Å)
| |
C1 |
C2 |
S3 |
H4 |
H5 |
H6 |
H7 |
H8 |
H9 |
| C1 | | 1.5166 | 2.8091 | 1.0951 | 1.0937 | 1.0924 | 2.1699 | 2.1614 | 2.9544 |
C2 | 1.5166 | | 1.8245 | 2.1587 | 2.1670 | 2.1637 | 1.0922 | 1.0930 | 2.3895 | S3 | 2.8091 | 1.8245 | | 3.7728 | 3.0579 | 2.9993 | 2.4112 | 2.3422 | 1.3474 | H4 | 1.0951 | 2.1587 | 3.7728 | | 1.7679 | 1.7748 | 2.5098 | 2.5072 | 3.9521 | H5 | 1.0937 | 2.1670 | 3.0579 | 1.7679 | | 1.7668 | 2.5311 | 3.0754 | 2.6958 | H6 | 1.0924 | 2.1637 | 2.9993 | 1.7748 | 1.7668 | | 3.0783 | 2.5139 | 3.3178 | H7 | 2.1699 | 1.0922 | 2.4112 | 2.5098 | 2.5311 | 3.0783 | | 1.7569 | 2.6572 | H8 | 2.1614 | 1.0930 | 2.3422 | 2.5072 | 3.0754 | 2.5139 | 1.7569 | | 3.2839 | H9 | 2.9544 | 2.3895 | 1.3474 | 3.9521 | 2.6958 | 3.3178 | 2.6572 | 3.2839 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| C1 |
C2 |
S3 |
114.126 |
|
C1 |
C2 |
H7 |
111.529 |
| C1 |
C2 |
H8 |
110.790 |
|
C2 |
C1 |
H4 |
110.454 |
| C2 |
C1 |
H5 |
111.199 |
|
C2 |
C1 |
H6 |
111.013 |
| C2 |
S3 |
H9 |
96.604 |
|
S3 |
C2 |
H7 |
108.919 |
| S3 |
C2 |
H8 |
103.962 |
|
H4 |
C1 |
H5 |
107.746 |
| H4 |
C1 |
H6 |
108.462 |
|
H5 |
C1 |
H6 |
107.845 |
| H7 |
C2 |
H8 |
107.031 |
|
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at PBE1PBE/6-311G**
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
-0.329 |
|
|
|
| 2 |
C |
-0.444 |
|
|
|
| 3 |
S |
-0.053 |
|
|
|
| 4 |
H |
0.127 |
|
|
|
| 5 |
H |
0.129 |
|
|
|
| 6 |
H |
0.148 |
|
|
|
| 7 |
H |
0.172 |
|
|
|
| 8 |
H |
0.170 |
|
|
|
| 9 |
H |
0.081 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
1.654 |
0.071 |
0.817 |
1.846 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-29.445 |
1.452 |
-0.846 |
| y |
1.452 |
-27.316 |
-1.805 |
| z |
-0.846 |
-1.805 |
-27.179 |
|
| Traceless |
| | x | y | z |
| x |
-2.198 |
1.452 |
-0.846 |
| y |
1.452 |
0.995 |
-1.805 |
| z |
-0.846 |
-1.805 |
1.202 |
|
| Polar |
| 3z2-r2 | 2.404 |
| x2-y2 | -2.129 |
| xy | 1.452 |
| xz | -0.846 |
| yz | -1.805 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
7.474 |
0.420 |
0.074 |
| y |
0.420 |
5.505 |
-0.366 |
| z |
0.074 |
-0.366 |
5.254 |
<r2> (average value of r
2) Å
2
| <r2> |
84.020 |
| (<r2>)1/2 |
9.166 |