Jump to
S1C2
Energy calculated at PBEPBE/6-311G*
| | hartrees |
| Energy at 0K | -477.742563 |
| Energy at 298.15K | -477.748726 |
| HF Energy | -477.742563 |
| Nuclear repulsion energy | 106.628726 |
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 PBEPBE/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' |
3045 |
3013 |
26.41 |
|
|
|
| 2 |
A' |
2990 |
2959 |
27.73 |
|
|
|
| 3 |
A' |
2975 |
2944 |
21.93 |
|
|
|
| 4 |
A' |
2556 |
2529 |
16.06 |
|
|
|
| 5 |
A' |
1475 |
1460 |
3.85 |
|
|
|
| 6 |
A' |
1454 |
1439 |
2.67 |
|
|
|
| 7 |
A' |
1380 |
1366 |
7.20 |
|
|
|
| 8 |
A' |
1274 |
1261 |
48.25 |
|
|
|
| 9 |
A' |
1092 |
1080 |
2.01 |
|
|
|
| 10 |
A' |
981 |
970 |
4.70 |
|
|
|
| 11 |
A' |
837 |
828 |
1.72 |
|
|
|
| 12 |
A' |
653 |
646 |
1.57 |
|
|
|
| 13 |
A' |
294 |
291 |
2.56 |
|
|
|
| 14 |
A" |
3058 |
3026 |
35.39 |
|
|
|
| 15 |
A" |
3031 |
3000 |
0.19 |
|
|
|
| 16 |
A" |
1465 |
1450 |
12.12 |
|
|
|
| 17 |
A" |
1244 |
1231 |
1.91 |
|
|
|
| 18 |
A" |
1026 |
1016 |
2.09 |
|
|
|
| 19 |
A" |
777 |
769 |
7.77 |
|
|
|
| 20 |
A" |
258 |
256 |
0.96 |
|
|
|
| 21 |
A" |
167 |
165 |
22.34 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 16015.5 cm
-1
Scaled (by 0.9896) Zero Point Vibrational Energy (zpe) 15849.0 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 PBEPBE/6-311G*
Point Group is Cs
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
1.519 |
0.699 |
0.000 |
| C2 |
0.000 |
0.837 |
0.000 |
| S3 |
-0.757 |
-0.848 |
0.000 |
| H4 |
1.991 |
1.694 |
0.000 |
| H5 |
1.873 |
0.158 |
0.891 |
| H6 |
1.873 |
0.158 |
-0.891 |
| H7 |
-0.338 |
1.383 |
0.893 |
| H8 |
-0.338 |
1.383 |
-0.893 |
| H9 |
-2.057 |
-0.435 |
0.000 |
Atom - Atom Distances (Å)
| |
C1 |
C2 |
S3 |
H4 |
H5 |
H6 |
H7 |
H8 |
H9 |
| C1 | | 1.5250 | 2.7518 | 1.1012 | 1.1007 | 1.1007 | 2.1712 | 2.1712 | 3.7509 |
C2 | 1.5250 | | 1.8473 | 2.1673 | 2.1827 | 2.1827 | 1.0999 | 1.0999 | 2.4183 | S3 | 2.7518 | 1.8473 | | 3.7433 | 2.9539 | 2.9539 | 2.4390 | 2.4390 | 1.3635 | H4 | 1.1012 | 2.1673 | 3.7433 | | 1.7791 | 1.7791 | 2.5139 | 2.5139 | 4.5732 | H5 | 1.1007 | 2.1827 | 2.9539 | 1.7791 | | 1.7814 | 2.5282 | 3.0941 | 4.0732 | H6 | 1.1007 | 2.1827 | 2.9539 | 1.7791 | 1.7814 | | 3.0941 | 2.5282 | 4.0732 | H7 | 2.1712 | 1.0999 | 2.4390 | 2.5139 | 2.5282 | 3.0941 | | 1.7862 | 2.6560 | H8 | 2.1712 | 1.0999 | 2.4390 | 2.5139 | 3.0941 | 2.5282 | 1.7862 | | 2.6560 | H9 | 3.7509 | 2.4183 | 1.3635 | 4.5732 | 4.0732 | 4.0732 | 2.6560 | 2.6560 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| C1 |
C2 |
S3 |
109.001 |
|
C1 |
C2 |
H7 |
110.569 |
| C1 |
C2 |
H8 |
110.569 |
|
C2 |
C1 |
H4 |
110.190 |
| C2 |
C1 |
H5 |
111.435 |
|
C2 |
C1 |
H6 |
111.435 |
| C2 |
S3 |
H9 |
96.573 |
|
S3 |
C2 |
H7 |
109.049 |
| S3 |
C2 |
H8 |
109.049 |
|
H4 |
C1 |
H5 |
107.798 |
| H4 |
C1 |
H6 |
107.798 |
|
H5 |
C1 |
H6 |
108.035 |
| H7 |
C2 |
H8 |
108.573 |
|
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at PBEPBE/6-311G*
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
-0.657 |
|
|
|
| 2 |
C |
-0.574 |
|
|
|
| 3 |
S |
-0.119 |
|
|
|
| 4 |
H |
0.228 |
|
|
|
| 5 |
H |
0.235 |
|
|
|
| 6 |
H |
0.235 |
|
|
|
| 7 |
H |
0.249 |
|
|
|
| 8 |
H |
0.249 |
|
|
|
| 9 |
H |
0.155 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
-0.055 |
1.827 |
0.000 |
1.827 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-25.016 |
-0.213 |
0.000 |
| y |
-0.213 |
-28.808 |
0.000 |
| z |
0.000 |
0.000 |
-29.668 |
|
| Traceless |
| | x | y | z |
| x |
4.222 |
-0.213 |
0.000 |
| y |
-0.213 |
-1.466 |
0.000 |
| z |
0.000 |
0.000 |
-2.755 |
|
| Polar |
| 3z2-r2 | -5.511 |
| x2-y2 | 3.792 |
| xy | -0.213 |
| xz | 0.000 |
| yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
6.978 |
0.911 |
0.000 |
| y |
0.911 |
6.640 |
0.000 |
| z |
0.000 |
0.000 |
4.679 |
<r2> (average value of r
2) Å
2
| <r2> |
84.588 |
| (<r2>)1/2 |
9.197 |
Jump to
S1C1
Energy calculated at PBEPBE/6-311G*
| | hartrees |
| Energy at 0K | -477.743634 |
| Energy at 298.15K | -477.749876 |
| HF Energy | -477.743634 |
| Nuclear repulsion energy | 106.346248 |
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 PBEPBE/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 |
3061 |
3029 |
32.28 |
|
|
|
| 2 |
A |
3038 |
3007 |
16.25 |
|
|
|
| 3 |
A |
3028 |
2997 |
20.11 |
|
|
|
| 4 |
A |
2995 |
2964 |
16.45 |
|
|
|
| 5 |
A |
2966 |
2935 |
31.14 |
|
|
|
| 6 |
A |
2553 |
2526 |
15.28 |
|
|
|
| 7 |
A |
1469 |
1453 |
4.60 |
|
|
|
| 8 |
A |
1460 |
1445 |
12.80 |
|
|
|
| 9 |
A |
1444 |
1429 |
2.21 |
|
|
|
| 10 |
A |
1376 |
1361 |
5.81 |
|
|
|
| 11 |
A |
1278 |
1264 |
20.12 |
|
|
|
| 12 |
A |
1254 |
1241 |
7.43 |
|
|
|
| 13 |
A |
1099 |
1088 |
11.85 |
|
|
|
| 14 |
A |
1047 |
1036 |
0.59 |
|
|
|
| 15 |
A |
967 |
957 |
9.86 |
|
|
|
| 16 |
A |
854 |
845 |
8.35 |
|
|
|
| 17 |
A |
722 |
714 |
3.43 |
|
|
|
| 18 |
A |
637 |
631 |
4.38 |
|
|
|
| 19 |
A |
319 |
316 |
1.70 |
|
|
|
| 20 |
A |
264 |
262 |
1.34 |
|
|
|
| 21 |
A |
209 |
207 |
20.14 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 16020.3 cm
-1
Scaled (by 0.9896) Zero Point Vibrational Energy (zpe) 15853.6 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 PBEPBE/6-311G*
Point Group is C1
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
1.649 |
-0.351 |
-0.054 |
| C2 |
0.504 |
0.644 |
0.092 |
| S3 |
-1.173 |
-0.100 |
-0.082 |
| H4 |
2.621 |
0.166 |
0.005 |
| H5 |
1.626 |
-1.109 |
0.745 |
| H6 |
1.596 |
-0.878 |
-1.017 |
| H7 |
0.555 |
1.186 |
1.048 |
| H8 |
0.537 |
1.401 |
-0.706 |
| H9 |
-1.082 |
-0.922 |
1.003 |
Atom - Atom Distances (Å)
| |
C1 |
C2 |
S3 |
H4 |
H5 |
H6 |
H7 |
H8 |
H9 |
| C1 | | 1.5242 | 2.8327 | 1.1030 | 1.1013 | 1.0997 | 2.1845 | 2.1751 | 2.9837 |
C2 | 1.5242 | | 1.8426 | 2.1724 | 2.1816 | 2.1778 | 1.1000 | 1.1007 | 2.4078 | S3 | 2.8327 | 1.8426 | | 3.8042 | 3.0878 | 3.0243 | 2.4330 | 2.3599 | 1.3639 | H4 | 1.1030 | 2.1724 | 3.8042 | | 1.7785 | 1.7857 | 2.5286 | 2.5245 | 3.9869 | H5 | 1.1013 | 2.1816 | 3.0878 | 1.7785 | | 1.7775 | 2.5505 | 3.0970 | 2.7273 | H6 | 1.0997 | 2.1778 | 3.0243 | 1.7857 | 1.7775 | | 3.1002 | 2.5326 | 3.3554 | H7 | 2.1845 | 1.1000 | 2.4330 | 2.5286 | 2.5505 | 3.1002 | | 1.7676 | 2.6696 | H8 | 2.1751 | 1.1007 | 2.3599 | 2.5245 | 3.0970 | 2.5326 | 1.7676 | | 3.3077 | H9 | 2.9837 | 2.4078 | 1.3639 | 3.9869 | 2.7273 | 3.3554 | 2.6696 | 3.3077 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| C1 |
C2 |
S3 |
114.237 |
|
C1 |
C2 |
H7 |
111.686 |
| C1 |
C2 |
H8 |
110.885 |
|
C2 |
C1 |
H4 |
110.537 |
| C2 |
C1 |
H5 |
111.373 |
|
C2 |
C1 |
H6 |
111.169 |
| C2 |
S3 |
H9 |
96.190 |
|
S3 |
C2 |
H7 |
108.912 |
| S3 |
C2 |
H8 |
103.719 |
|
H4 |
C1 |
H5 |
107.571 |
| H4 |
C1 |
H6 |
108.320 |
|
H5 |
C1 |
H6 |
107.727 |
| H7 |
C2 |
H8 |
106.874 |
|
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at PBEPBE/6-311G*
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
-0.619 |
|
|
|
| 2 |
C |
-0.603 |
|
|
|
| 3 |
S |
-0.112 |
|
|
|
| 4 |
H |
0.218 |
|
|
|
| 5 |
H |
0.218 |
|
|
|
| 6 |
H |
0.240 |
|
|
|
| 7 |
H |
0.252 |
|
|
|
| 8 |
H |
0.253 |
|
|
|
| 9 |
H |
0.154 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
1.645 |
0.076 |
0.834 |
1.846 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-29.751 |
1.503 |
-0.864 |
| y |
1.503 |
-27.691 |
-1.850 |
| z |
-0.864 |
-1.850 |
-27.369 |
|
| Traceless |
| | x | y | z |
| x |
-2.220 |
1.503 |
-0.864 |
| y |
1.503 |
0.869 |
-1.850 |
| z |
-0.864 |
-1.850 |
1.352 |
|
| Polar |
| 3z2-r2 | 2.704 |
| x2-y2 | -2.059 |
| xy | 1.503 |
| xz | -0.864 |
| yz | -1.850 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
7.759 |
0.430 |
0.087 |
| y |
0.430 |
5.563 |
-0.388 |
| z |
0.087 |
-0.388 |
5.350 |
<r2> (average value of r
2) Å
2
| <r2> |
85.335 |
| (<r2>)1/2 |
9.238 |