Jump to
S1C2
Energy calculated at HSEh1PBE/6-311G**
| | hartrees |
| Energy at 0K | -477.825323 |
| Energy at 298.15K | |
| HF Energy | -477.825323 |
| Nuclear repulsion energy | 107.464247 |
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 HSEh1PBE/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' |
3130 |
3006 |
22.59 |
|
|
|
| 2 |
A' |
3077 |
2955 |
22.97 |
|
|
|
| 3 |
A' |
3053 |
2933 |
19.02 |
|
|
|
| 4 |
A' |
2703 |
2596 |
5.55 |
|
|
|
| 5 |
A' |
1501 |
1441 |
3.25 |
|
|
|
| 6 |
A' |
1486 |
1427 |
2.51 |
|
|
|
| 7 |
A' |
1413 |
1357 |
6.22 |
|
|
|
| 8 |
A' |
1311 |
1259 |
43.89 |
|
|
|
| 9 |
A' |
1122 |
1078 |
2.22 |
|
|
|
| 10 |
A' |
1010 |
970 |
4.01 |
|
|
|
| 11 |
A' |
865 |
831 |
2.01 |
|
|
|
| 12 |
A' |
687 |
660 |
1.45 |
|
|
|
| 13 |
A' |
303 |
291 |
2.52 |
|
|
|
| 14 |
A" |
3144 |
3019 |
28.30 |
|
|
|
| 15 |
A" |
3120 |
2996 |
0.20 |
|
|
|
| 16 |
A" |
1489 |
1430 |
10.82 |
|
|
|
| 17 |
A" |
1274 |
1223 |
1.63 |
|
|
|
| 18 |
A" |
1054 |
1013 |
1.56 |
|
|
|
| 19 |
A" |
795 |
764 |
6.80 |
|
|
|
| 20 |
A" |
258 |
248 |
0.84 |
|
|
|
| 21 |
A" |
150 |
144 |
22.61 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 16472.6 cm
-1
Scaled (by 0.9604) Zero Point Vibrational Energy (zpe) 15820.3 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 HSEh1PBE/6-311G**
Point Group is Cs
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
1.512 |
0.691 |
0.000 |
| C2 |
0.000 |
0.830 |
0.000 |
| S3 |
-0.754 |
-0.838 |
0.000 |
| H4 |
1.980 |
1.678 |
0.000 |
| H5 |
1.860 |
0.152 |
0.885 |
| H6 |
1.860 |
0.152 |
-0.885 |
| H7 |
-0.334 |
1.371 |
0.887 |
| H8 |
-0.334 |
1.371 |
-0.887 |
| H9 |
-2.040 |
-0.439 |
0.000 |
Atom - Atom Distances (Å)
| |
C1 |
C2 |
S3 |
H4 |
H5 |
H6 |
H7 |
H8 |
H9 |
| C1 | | 1.5179 | 2.7328 | 1.0933 | 1.0930 | 1.0930 | 2.1577 | 2.1577 | 3.7272 |
C2 | 1.5179 | | 1.8299 | 2.1545 | 2.1681 | 2.1681 | 1.0917 | 1.0917 | 2.4026 | S3 | 2.7328 | 1.8299 | | 3.7157 | 2.9314 | 2.9314 | 2.4169 | 2.4169 | 1.3468 | H4 | 1.0933 | 2.1545 | 3.7157 | | 1.7686 | 1.7686 | 2.4975 | 2.4975 | 4.5441 | H5 | 1.0930 | 2.1681 | 2.9314 | 1.7686 | | 1.7701 | 2.5096 | 3.0723 | 4.0426 | H6 | 1.0930 | 2.1681 | 2.9314 | 1.7686 | 1.7701 | | 3.0723 | 2.5096 | 4.0426 | H7 | 2.1577 | 1.0917 | 2.4169 | 2.4975 | 2.5096 | 3.0723 | | 1.7745 | 2.6410 | H8 | 2.1577 | 1.0917 | 2.4169 | 2.4975 | 3.0723 | 2.5096 | 1.7745 | | 2.6410 | H9 | 3.7272 | 2.4026 | 1.3468 | 4.5441 | 4.0426 | 4.0426 | 2.6410 | 2.6410 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| C1 |
C2 |
S3 |
109.079 |
|
C1 |
C2 |
H7 |
110.491 |
| C1 |
C2 |
H8 |
110.491 |
|
C2 |
C1 |
H4 |
110.136 |
| C2 |
C1 |
H5 |
111.239 |
|
C2 |
C1 |
H6 |
111.239 |
| C2 |
S3 |
H9 |
97.114 |
|
S3 |
C2 |
H7 |
109.010 |
| S3 |
C2 |
H8 |
109.010 |
|
H4 |
C1 |
H5 |
107.983 |
| H4 |
C1 |
H6 |
107.983 |
|
H5 |
C1 |
H6 |
108.135 |
| H7 |
C2 |
H8 |
108.730 |
|
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at HSEh1PBE/6-311G**
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
-0.366 |
|
|
|
| 2 |
C |
-0.420 |
|
|
|
| 3 |
S |
-0.059 |
|
|
|
| 4 |
H |
0.135 |
|
|
|
| 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 |
| |
-0.042 |
1.811 |
0.000 |
1.812 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-24.782 |
-0.194 |
0.000 |
| y |
-0.194 |
-28.576 |
0.000 |
| z |
0.000 |
0.000 |
-29.352 |
|
| Traceless |
| | x | y | z |
| x |
4.182 |
-0.194 |
0.000 |
| y |
-0.194 |
-1.508 |
0.000 |
| z |
0.000 |
0.000 |
-2.673 |
|
| Polar |
| 3z2-r2 | -5.347 |
| x2-y2 | 3.793 |
| xy | -0.194 |
| xz | 0.000 |
| yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
6.824 |
0.882 |
0.000 |
| y |
0.882 |
6.501 |
0.000 |
| z |
0.000 |
0.000 |
4.665 |
<r2> (average value of r
2) Å
2
| <r2> |
83.422 |
| (<r2>)1/2 |
9.134 |
Jump to
S1C1
Energy calculated at HSEh1PBE/6-311G**
| | hartrees |
| Energy at 0K | -477.826317 |
| Energy at 298.15K | -477.832672 |
| HF Energy | -477.826317 |
| Nuclear repulsion energy | 107.207064 |
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 HSEh1PBE/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 |
3145 |
3021 |
26.59 |
|
|
|
| 2 |
A |
3124 |
3000 |
10.88 |
|
|
|
| 3 |
A |
3115 |
2991 |
19.76 |
|
|
|
| 4 |
A |
3080 |
2958 |
14.18 |
|
|
|
| 5 |
A |
3046 |
2925 |
24.81 |
|
|
|
| 6 |
A |
2706 |
2598 |
5.47 |
|
|
|
| 7 |
A |
1494 |
1435 |
3.92 |
|
|
|
| 8 |
A |
1487 |
1428 |
11.39 |
|
|
|
| 9 |
A |
1476 |
1417 |
1.87 |
|
|
|
| 10 |
A |
1410 |
1354 |
5.15 |
|
|
|
| 11 |
A |
1315 |
1263 |
21.22 |
|
|
|
| 12 |
A |
1284 |
1233 |
4.92 |
|
|
|
| 13 |
A |
1129 |
1084 |
10.74 |
|
|
|
| 14 |
A |
1078 |
1035 |
0.61 |
|
|
|
| 15 |
A |
999 |
959 |
8.45 |
|
|
|
| 16 |
A |
877 |
842 |
8.66 |
|
|
|
| 17 |
A |
743 |
714 |
3.13 |
|
|
|
| 18 |
A |
671 |
645 |
4.06 |
|
|
|
| 19 |
A |
331 |
318 |
2.08 |
|
|
|
| 20 |
A |
270 |
259 |
1.88 |
|
|
|
| 21 |
A |
226 |
217 |
18.64 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 16502.6 cm
-1
Scaled (by 0.9604) Zero Point Vibrational Energy (zpe) 15849.1 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 HSEh1PBE/6-311G**
Point Group is C1
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
1.636 |
-0.349 |
-0.054 |
| C2 |
0.497 |
0.642 |
0.092 |
| S3 |
-1.163 |
-0.099 |
-0.080 |
| H4 |
2.601 |
0.164 |
0.009 |
| H5 |
1.607 |
-1.103 |
0.738 |
| H6 |
1.582 |
-0.869 |
-1.013 |
| H7 |
0.549 |
1.176 |
1.043 |
| H8 |
0.533 |
1.394 |
-0.701 |
| H9 |
-1.070 |
-0.932 |
0.975 |
Atom - Atom Distances (Å)
| |
C1 |
C2 |
S3 |
H4 |
H5 |
H6 |
H7 |
H8 |
H9 |
| C1 | | 1.5165 | 2.8096 | 1.0949 | 1.0935 | 1.0922 | 2.1699 | 2.1615 | 2.9524 |
C2 | 1.5165 | | 1.8258 | 2.1588 | 2.1667 | 2.1635 | 1.0919 | 1.0927 | 2.3903 | S3 | 2.8096 | 1.8258 | | 3.7736 | 3.0574 | 2.9996 | 2.4119 | 2.3431 | 1.3475 | H4 | 1.0949 | 2.1588 | 3.7736 | | 1.7676 | 1.7745 | 2.5101 | 2.5080 | 3.9505 | H5 | 1.0935 | 2.1667 | 3.0574 | 1.7676 | | 1.7665 | 2.5308 | 3.0751 | 2.6926 | H6 | 1.0922 | 2.1635 | 2.9996 | 1.7745 | 1.7665 | | 3.0780 | 2.5137 | 3.3149 | H7 | 2.1699 | 1.0919 | 2.4119 | 2.5101 | 2.5308 | 3.0780 | | 1.7569 | 2.6588 | H8 | 2.1615 | 1.0927 | 2.3431 | 2.5080 | 3.0751 | 2.5137 | 1.7569 | | 3.2844 | H9 | 2.9524 | 2.3903 | 1.3475 | 3.9505 | 2.6926 | 3.3149 | 2.6588 | 3.2844 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| C1 |
C2 |
S3 |
114.084 |
|
C1 |
C2 |
H7 |
111.547 |
| C1 |
C2 |
H8 |
110.817 |
|
C2 |
C1 |
H4 |
110.470 |
| C2 |
C1 |
H5 |
111.189 |
|
C2 |
C1 |
H6 |
111.014 |
| C2 |
S3 |
H9 |
96.580 |
|
S3 |
C2 |
H7 |
108.891 |
| S3 |
C2 |
H8 |
103.955 |
|
H4 |
C1 |
H5 |
107.740 |
| H4 |
C1 |
H6 |
108.459 |
|
H5 |
C1 |
H6 |
107.847 |
| H7 |
C2 |
H8 |
107.067 |
|
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at HSEh1PBE/6-311G**
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
-0.328 |
|
|
|
| 2 |
C |
-0.441 |
|
|
|
| 3 |
S |
-0.053 |
|
|
|
| 4 |
H |
0.126 |
|
|
|
| 5 |
H |
0.128 |
|
|
|
| 6 |
H |
0.148 |
|
|
|
| 7 |
H |
0.171 |
|
|
|
| 8 |
H |
0.169 |
|
|
|
| 9 |
H |
0.080 |
|
|
|
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 |
0.810 |
1.843 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-29.459 |
1.448 |
-0.832 |
| y |
1.448 |
-27.330 |
-1.806 |
| z |
-0.832 |
-1.806 |
-27.209 |
|
| Traceless |
| | x | y | z |
| x |
-2.190 |
1.448 |
-0.832 |
| y |
1.448 |
1.005 |
-1.806 |
| z |
-0.832 |
-1.806 |
1.185 |
|
| Polar |
| 3z2-r2 | 2.371 |
| x2-y2 | -2.130 |
| xy | 1.448 |
| xz | -0.832 |
| yz | -1.806 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
7.498 |
0.422 |
0.075 |
| y |
0.422 |
5.516 |
-0.368 |
| z |
0.075 |
-0.368 |
5.259 |
<r2> (average value of r
2) Å
2
| <r2> |
84.055 |
| (<r2>)1/2 |
9.168 |