Jump to
S1C2
Energy calculated at B3LYP/LANL2DZ
| | hartrees |
| Energy at 0K | -89.908048 |
| Energy at 298.15K | -89.914224 |
| HF Energy | -89.908048 |
| Nuclear repulsion energy | 63.973542 |
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 B3LYP/LANL2DZ
| 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' |
3135 |
3013 |
39.00 |
|
|
|
| 2 |
A' |
3094 |
2974 |
25.07 |
|
|
|
| 3 |
A' |
3047 |
2929 |
28.17 |
|
|
|
| 4 |
A' |
2494 |
2398 |
42.84 |
|
|
|
| 5 |
A' |
1527 |
1468 |
7.03 |
|
|
|
| 6 |
A' |
1507 |
1449 |
3.25 |
|
|
|
| 7 |
A' |
1445 |
1389 |
16.05 |
|
|
|
| 8 |
A' |
1324 |
1273 |
36.45 |
|
|
|
| 9 |
A' |
1119 |
1076 |
2.68 |
|
|
|
| 10 |
A' |
1014 |
974 |
9.80 |
|
|
|
| 11 |
A' |
840 |
807 |
2.92 |
|
|
|
| 12 |
A' |
620 |
596 |
3.17 |
|
|
|
| 13 |
A' |
301 |
289 |
4.58 |
|
|
|
| 14 |
A" |
3172 |
3049 |
55.90 |
|
|
|
| 15 |
A" |
3140 |
3018 |
6.54 |
|
|
|
| 16 |
A" |
1516 |
1457 |
13.40 |
|
|
|
| 17 |
A" |
1281 |
1231 |
1.95 |
|
|
|
| 18 |
A" |
1060 |
1019 |
0.00 |
|
|
|
| 19 |
A" |
807 |
776 |
10.71 |
|
|
|
| 20 |
A" |
250 |
240 |
1.22 |
|
|
|
| 21 |
A" |
171 |
165 |
28.13 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 16431.5 cm
-1
Scaled (by 0.9612) Zero Point Vibrational Energy (zpe) 15794.0 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 B3LYP/LANL2DZ
Point Group is Cs
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
1.530 |
0.743 |
0.000 |
| C2 |
0.000 |
0.872 |
0.000 |
| S3 |
-0.759 |
-0.883 |
0.000 |
| H4 |
1.989 |
1.740 |
0.000 |
| H5 |
1.882 |
0.206 |
0.889 |
| H6 |
1.882 |
0.206 |
-0.889 |
| H7 |
-0.353 |
1.396 |
0.893 |
| H8 |
-0.353 |
1.396 |
-0.893 |
| H9 |
-2.085 |
-0.498 |
0.000 |
Atom - Atom Distances (Å)
| |
C1 |
C2 |
S3 |
H4 |
H5 |
H6 |
H7 |
H8 |
H9 |
| C1 | | 1.5351 | 2.8072 | 1.0981 | 1.0965 | 1.0965 | 2.1837 | 2.1837 | 3.8214 |
C2 | 1.5351 | | 1.9119 | 2.1705 | 2.1852 | 2.1852 | 1.0939 | 1.0939 | 2.4945 | S3 | 2.8072 | 1.9119 | | 3.7990 | 2.9916 | 2.9916 | 2.4811 | 2.4811 | 1.3807 | H4 | 1.0981 | 2.1705 | 3.7990 | | 1.7762 | 1.7762 | 2.5302 | 2.5302 | 4.6482 | H5 | 1.0965 | 2.1852 | 2.9916 | 1.7762 | | 1.7777 | 2.5321 | 3.0961 | 4.1255 | H6 | 1.0965 | 2.1852 | 2.9916 | 1.7762 | 1.7777 | | 3.0961 | 2.5321 | 4.1255 | H7 | 2.1837 | 1.0939 | 2.4811 | 2.5302 | 2.5321 | 3.0961 | | 1.7857 | 2.7171 | H8 | 2.1837 | 1.0939 | 2.4811 | 2.5302 | 3.0961 | 2.5321 | 1.7857 | | 2.7171 | H9 | 3.8214 | 2.4945 | 1.3807 | 4.6482 | 4.1255 | 4.1255 | 2.7171 | 2.7171 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| C1 |
C2 |
S3 |
108.561 |
|
C1 |
C2 |
H7 |
111.216 |
| C1 |
C2 |
H8 |
111.216 |
|
C2 |
C1 |
H4 |
109.923 |
| C2 |
C1 |
H5 |
111.179 |
|
C2 |
C1 |
H6 |
111.179 |
| C2 |
S3 |
H9 |
97.187 |
|
S3 |
C2 |
H7 |
108.162 |
| S3 |
C2 |
H8 |
108.162 |
|
H4 |
C1 |
H5 |
108.068 |
| H4 |
C1 |
H6 |
108.068 |
|
H5 |
C1 |
H6 |
108.312 |
| H7 |
C2 |
H8 |
109.420 |
|
Electronic energy levels
Electronic state
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at B3LYP/LANL2DZ
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
-0.578 |
|
|
|
| 2 |
C |
-0.565 |
|
|
|
| 3 |
S |
-0.051 |
|
|
|
| 4 |
H |
0.206 |
|
|
|
| 5 |
H |
0.218 |
|
|
|
| 6 |
H |
0.218 |
|
|
|
| 7 |
H |
0.239 |
|
|
|
| 8 |
H |
0.239 |
|
|
|
| 9 |
H |
0.074 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
-0.070 |
2.004 |
0.000 |
2.005 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-23.764 |
-0.109 |
0.000 |
| y |
-0.109 |
-27.723 |
0.000 |
| z |
0.000 |
0.000 |
-28.072 |
|
| Traceless |
| | x | y | z |
| x |
4.134 |
-0.109 |
0.000 |
| y |
-0.109 |
-1.805 |
0.000 |
| z |
0.000 |
0.000 |
-2.329 |
|
| Polar |
| 3z2-r2 | -4.658 |
| x2-y2 | 3.959 |
| xy | -0.109 |
| xz | 0.000 |
| yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
6.329 |
1.008 |
0.000 |
| y |
1.008 |
6.180 |
0.000 |
| z |
0.000 |
0.000 |
3.375 |
<r2> (average value of r
2) Å
2
| <r2> |
72.674 |
| (<r2>)1/2 |
8.525 |
Jump to
S1C1
Energy calculated at B3LYP/LANL2DZ
| | hartrees |
| Energy at 0K | -89.908876 |
| Energy at 298.15K | -89.915124 |
| HF Energy | -89.908876 |
| Nuclear repulsion energy | 64.053929 |
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 B3LYP/LANL2DZ
| 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 |
3173 |
3050 |
41.31 |
|
|
|
| 2 |
A |
3141 |
3020 |
10.96 |
|
|
|
| 3 |
A |
3123 |
3002 |
48.60 |
|
|
|
| 4 |
A |
3097 |
2976 |
16.70 |
|
|
|
| 5 |
A |
3038 |
2920 |
31.39 |
|
|
|
| 6 |
A |
2499 |
2402 |
36.68 |
|
|
|
| 7 |
A |
1523 |
1464 |
7.75 |
|
|
|
| 8 |
A |
1513 |
1454 |
15.73 |
|
|
|
| 9 |
A |
1502 |
1444 |
4.34 |
|
|
|
| 10 |
A |
1442 |
1386 |
11.58 |
|
|
|
| 11 |
A |
1325 |
1274 |
15.42 |
|
|
|
| 12 |
A |
1286 |
1236 |
4.24 |
|
|
|
| 13 |
A |
1129 |
1085 |
9.96 |
|
|
|
| 14 |
A |
1080 |
1038 |
1.02 |
|
|
|
| 15 |
A |
1005 |
966 |
15.40 |
|
|
|
| 16 |
A |
865 |
831 |
13.09 |
|
|
|
| 17 |
A |
747 |
718 |
3.63 |
|
|
|
| 18 |
A |
611 |
588 |
6.17 |
|
|
|
| 19 |
A |
322 |
309 |
1.82 |
|
|
|
| 20 |
A |
255 |
245 |
1.37 |
|
|
|
| 21 |
A |
210 |
201 |
25.21 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 16441.3 cm
-1
Scaled (by 0.9612) Zero Point Vibrational Energy (zpe) 15803.3 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 B3LYP/LANL2DZ
Point Group is C1
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
1.671 |
-0.366 |
-0.056 |
| C2 |
0.541 |
0.662 |
0.094 |
| S3 |
-1.201 |
-0.096 |
-0.082 |
| H4 |
2.649 |
0.134 |
-0.002 |
| H5 |
1.634 |
-1.119 |
0.742 |
| H6 |
1.602 |
-0.886 |
-1.018 |
| H7 |
0.588 |
1.179 |
1.057 |
| H8 |
0.576 |
1.413 |
-0.701 |
| H9 |
-1.110 |
-0.951 |
0.998 |
Atom - Atom Distances (Å)
| |
C1 |
C2 |
S3 |
H4 |
H5 |
H6 |
H7 |
H8 |
H9 |
| C1 | | 1.5348 | 2.8846 | 1.0996 | 1.0975 | 1.0958 | 2.1907 | 2.1861 | 3.0310 |
C2 | 1.5348 | | 1.9080 | 2.1750 | 2.1873 | 2.1814 | 1.0940 | 1.0944 | 2.4789 | S3 | 2.8846 | 1.9080 | | 3.8574 | 3.1237 | 3.0588 | 2.4742 | 2.4123 | 1.3801 | H4 | 1.0996 | 2.1750 | 3.8574 | | 1.7761 | 1.7798 | 2.5423 | 2.5337 | 4.0382 | H5 | 1.0975 | 2.1873 | 3.1237 | 1.7761 | | 1.7754 | 2.5442 | 3.1000 | 2.7606 | H6 | 1.0958 | 2.1814 | 3.0588 | 1.7798 | 1.7754 | | 3.0982 | 2.5371 | 3.3800 | H7 | 2.1907 | 1.0940 | 2.4742 | 2.5423 | 2.5442 | 3.0982 | | 1.7741 | 2.7241 | H8 | 2.1861 | 1.0944 | 2.4123 | 2.5337 | 3.1000 | 2.5371 | 1.7741 | | 3.3643 | H9 | 3.0310 | 2.4789 | 1.3801 | 4.0382 | 2.7606 | 3.3800 | 2.7241 | 3.3643 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| C1 |
C2 |
S3 |
113.383 |
|
C1 |
C2 |
H7 |
111.791 |
| C1 |
C2 |
H8 |
111.399 |
|
C2 |
C1 |
H4 |
110.202 |
| C2 |
C1 |
H5 |
111.303 |
|
C2 |
C1 |
H6 |
110.934 |
| C2 |
S3 |
H9 |
96.538 |
|
S3 |
C2 |
H7 |
107.916 |
| S3 |
C2 |
H8 |
103.586 |
|
H4 |
C1 |
H5 |
107.873 |
| H4 |
C1 |
H6 |
108.329 |
|
H5 |
C1 |
H6 |
108.088 |
| H7 |
C2 |
H8 |
108.327 |
|
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at B3LYP/LANL2DZ
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
-0.564 |
|
|
|
| 2 |
C |
-0.581 |
|
|
|
| 3 |
S |
-0.037 |
|
|
|
| 4 |
H |
0.202 |
|
|
|
| 5 |
H |
0.202 |
|
|
|
| 6 |
H |
0.221 |
|
|
|
| 7 |
H |
0.242 |
|
|
|
| 8 |
H |
0.245 |
|
|
|
| 9 |
H |
0.069 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
1.882 |
0.017 |
0.908 |
2.089 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-28.586 |
1.518 |
-1.049 |
| y |
1.518 |
-26.201 |
-1.600 |
| z |
-1.049 |
-1.600 |
-26.252 |
|
| Traceless |
| | x | y | z |
| x |
-2.359 |
1.518 |
-1.049 |
| y |
1.518 |
1.218 |
-1.600 |
| z |
-1.049 |
-1.600 |
1.141 |
|
| Polar |
| 3z2-r2 | 2.282 |
| x2-y2 | -2.385 |
| xy | 1.518 |
| xz | -1.049 |
| yz | -1.600 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
6.773 |
0.852 |
0.272 |
| y |
0.852 |
4.651 |
-0.766 |
| z |
0.272 |
-0.766 |
4.514 |
<r2> (average value of r
2) Å
2
| <r2> |
72.335 |
| (<r2>)1/2 |
8.505 |