Jump to
S1C2
Energy calculated at LSDA/cc-pVDZ
| hartrees |
Energy at 0K | -552.239726 |
Energy at 298.15K | -552.244704 |
Nuclear repulsion energy | 198.925493 |
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 LSDA/cc-pVDZ
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 |
3197 |
3161 |
0.73 |
|
|
|
2 |
A |
3094 |
3060 |
0.00 |
|
|
|
3 |
A |
3078 |
3044 |
5.64 |
|
|
|
4 |
A |
1651 |
1633 |
4.24 |
|
|
|
5 |
A |
1330 |
1316 |
7.33 |
|
|
|
6 |
A |
1224 |
1210 |
1.49 |
|
|
|
7 |
A |
1003 |
992 |
1.80 |
|
|
|
8 |
A |
921 |
911 |
0.00 |
|
|
|
9 |
A |
825 |
816 |
0.00 |
|
|
|
10 |
A |
723 |
715 |
0.13 |
|
|
|
11 |
A |
600 |
594 |
0.00 |
|
|
|
12 |
A |
404 |
399 |
0.80 |
|
|
|
13 |
A |
168 |
166 |
0.22 |
|
|
|
14 |
A |
84 |
83 |
0.00 |
|
|
|
15 |
A |
3197 |
3162 |
0.17 |
|
|
|
16 |
A |
3095 |
3061 |
0.93 |
|
|
|
17 |
A |
3084 |
3050 |
2.80 |
|
|
|
18 |
A |
1624 |
1606 |
184.91 |
|
|
|
19 |
A |
1327 |
1312 |
0.19 |
|
|
|
20 |
A |
1197 |
1184 |
10.69 |
|
|
|
21 |
A |
974 |
963 |
39.09 |
|
|
|
22 |
A |
931 |
921 |
46.84 |
|
|
|
23 |
A |
826 |
817 |
72.64 |
|
|
|
24 |
A |
748 |
740 |
37.13 |
|
|
|
25 |
A |
532 |
526 |
23.78 |
|
|
|
26 |
A |
371 |
367 |
4.68 |
|
|
|
27 |
A |
46 |
46 |
0.18 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 18125.6 cm
-1
Scaled (by 0.989) Zero Point Vibrational Energy (zpe) 17926.2 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 LSDA/cc-pVDZ
Point Group is C2
Cartesians (Å)
Atom |
x (Å) |
y (Å) |
z (Å) |
S1 |
0.000 |
0.000 |
0.626 |
C2 |
0.000 |
1.347 |
-0.485 |
C3 |
0.000 |
-1.347 |
-0.485 |
C4 |
0.000 |
2.630 |
-0.107 |
C5 |
0.000 |
-2.630 |
-0.107 |
H6 |
0.000 |
1.054 |
-1.551 |
H7 |
-0.000 |
-1.054 |
-1.551 |
H8 |
0.000 |
3.425 |
-0.866 |
H9 |
-0.000 |
2.929 |
0.953 |
H10 |
-0.000 |
-3.425 |
-0.866 |
H11 |
0.000 |
-2.929 |
0.953 |
Atom - Atom Distances (Å)
|
S1 |
C2 |
C3 |
C4 |
C5 |
H6 |
H7 |
H8 |
H9 |
H10 |
H11 |
S1 | | 1.7459 | 1.7459 | 2.7301 | 2.7301 | 2.4192 | 2.4192 | 3.7362 | 2.9470 | 3.7362 | 2.9470 |
C2 | 1.7459 | | 2.6935 | 1.3374 | 3.9944 | 1.1056 | 2.6273 | 2.1131 | 2.1378 | 4.7871 | 4.5109 | C3 | 1.7459 | 2.6935 | | 3.9944 | 1.3374 | 2.6273 | 1.1056 | 4.7871 | 4.5109 | 2.1131 | 2.1378 | C4 | 2.7301 | 1.3374 | 3.9944 | | 5.2595 | 2.1370 | 3.9571 | 1.0996 | 1.1015 | 6.1023 | 5.6588 | C5 | 2.7301 | 3.9944 | 1.3374 | 5.2595 | | 3.9571 | 2.1370 | 6.1023 | 5.6588 | 1.0996 | 1.1015 | H6 | 2.4192 | 1.1056 | 2.6273 | 2.1370 | 3.9571 | | 2.1088 | 2.4676 | 3.1279 | 4.5316 | 4.7050 | H7 | 2.4192 | 2.6273 | 1.1056 | 3.9571 | 2.1370 | 2.1088 | | 4.5316 | 4.7050 | 2.4676 | 3.1279 | H8 | 3.7362 | 2.1131 | 4.7871 | 1.0996 | 6.1023 | 2.4676 | 4.5316 | | 1.8858 | 6.8502 | 6.6093 | H9 | 2.9470 | 2.1378 | 4.5109 | 1.1015 | 5.6588 | 3.1279 | 4.7050 | 1.8858 | | 6.6093 | 5.8576 | H10 | 3.7362 | 4.7871 | 2.1131 | 6.1023 | 1.0996 | 4.5316 | 2.4676 | 6.8502 | 6.6093 | | 1.8858 | H11 | 2.9470 | 4.5109 | 2.1378 | 5.6588 | 1.1015 | 4.7050 | 3.1279 | 6.6093 | 5.8576 | 1.8858 | |
More geometry information
Calculated Bond Angles
atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
S1 |
C2 |
C4 |
124.075 |
|
S1 |
C2 |
H6 |
114.189 |
S1 |
C3 |
C5 |
124.075 |
|
S1 |
C3 |
H7 |
114.189 |
C2 |
S1 |
C3 |
100.959 |
|
C2 |
C4 |
H8 |
119.925 |
C2 |
C4 |
H9 |
122.159 |
|
C3 |
C5 |
H10 |
119.925 |
C3 |
C5 |
H11 |
122.159 |
|
C4 |
C2 |
H6 |
121.737 |
C5 |
C3 |
H7 |
121.737 |
|
H8 |
C4 |
H9 |
117.916 |
H10 |
C5 |
H11 |
117.916 |
|
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at LSDA/cc-pVDZ
Charges (e)
Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
1 |
S |
0.133 |
|
|
|
2 |
C |
-0.186 |
|
|
|
3 |
C |
-0.186 |
|
|
|
4 |
C |
-0.081 |
|
|
|
5 |
C |
-0.081 |
|
|
|
6 |
H |
0.065 |
|
|
|
7 |
H |
0.065 |
|
|
|
8 |
H |
0.071 |
|
|
|
9 |
H |
0.064 |
|
|
|
10 |
H |
0.071 |
|
|
|
11 |
H |
0.064 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
|
x |
y |
z |
Total |
|
0.000 |
0.000 |
-0.978 |
0.978 |
CHELPG |
|
|
|
|
AIM |
|
|
|
|
ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
Primitive |
| x | y | z |
x |
-41.982 |
0.000 |
0.000 |
y |
0.000 |
-33.989 |
0.000 |
z |
0.000 |
0.000 |
-34.936 |
|
Traceless |
| x | y | z |
x |
-7.520 |
0.000 |
0.000 |
y |
0.000 |
4.470 |
0.000 |
z |
0.000 |
0.000 |
3.049 |
|
Polar |
3z2-r2 | 6.099 |
x2-y2 | -7.993 |
xy | 0.000 |
xz | 0.000 |
yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
|
x |
y |
z |
x |
3.842 |
0.000 |
0.000 |
y |
0.000 |
17.811 |
0.000 |
z |
0.000 |
0.000 |
8.116 |
<r2> (average value of r
2) Å
2
<r2> |
0.000 |
(<r2>)1/2 |
0.000 |
Jump to
S1C1
Energy calculated at LSDA/cc-pVDZ
| hartrees |
Energy at 0K | -552.240905 |
Energy at 298.15K | -552.246264 |
HF Energy | -552.240905 |
Nuclear repulsion energy | 202.429427 |
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 LSDA/cc-pVDZ
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 |
3192 |
3157 |
0.68 |
|
|
|
2 |
A |
3191 |
3156 |
0.50 |
|
|
|
3 |
A |
3112 |
3078 |
0.54 |
|
|
|
4 |
A |
3090 |
3056 |
0.31 |
|
|
|
5 |
A |
3086 |
3052 |
1.59 |
|
|
|
6 |
A |
3074 |
3040 |
2.18 |
|
|
|
7 |
A |
1637 |
1619 |
53.35 |
|
|
|
8 |
A |
1625 |
1607 |
40.39 |
|
|
|
9 |
A |
1327 |
1313 |
3.41 |
|
|
|
10 |
A |
1323 |
1309 |
8.02 |
|
|
|
11 |
A |
1222 |
1209 |
0.67 |
|
|
|
12 |
A |
1204 |
1191 |
6.92 |
|
|
|
13 |
A |
1002 |
991 |
15.05 |
|
|
|
14 |
A |
971 |
960 |
13.38 |
|
|
|
15 |
A |
944 |
934 |
20.70 |
|
|
|
16 |
A |
926 |
916 |
35.70 |
|
|
|
17 |
A |
859 |
850 |
31.75 |
|
|
|
18 |
A |
825 |
816 |
39.36 |
|
|
|
19 |
A |
745 |
736 |
13.22 |
|
|
|
20 |
A |
705 |
697 |
4.80 |
|
|
|
21 |
A |
602 |
596 |
9.95 |
|
|
|
22 |
A |
585 |
579 |
16.53 |
|
|
|
23 |
A |
458 |
453 |
0.57 |
|
|
|
24 |
A |
355 |
351 |
0.51 |
|
|
|
25 |
A |
225 |
223 |
0.80 |
|
|
|
26 |
A |
167 |
165 |
4.06 |
|
|
|
27 |
A |
90 |
89 |
0.63 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 18270.5 cm
-1
Scaled (by 0.989) Zero Point Vibrational Energy (zpe) 18069.5 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 LSDA/cc-pVDZ
Point Group is C1
Cartesians (Å)
Atom |
x (Å) |
y (Å) |
z (Å) |
S1 |
0.024 |
-0.962 |
0.009 |
C2 |
1.049 |
0.424 |
0.295 |
C3 |
-1.560 |
-0.224 |
-0.010 |
C4 |
2.298 |
0.522 |
-0.173 |
C5 |
-1.845 |
1.079 |
-0.132 |
H6 |
0.607 |
1.183 |
0.968 |
H7 |
-2.356 |
-0.980 |
0.109 |
H8 |
2.942 |
1.360 |
0.137 |
H9 |
2.721 |
-0.231 |
-0.858 |
H10 |
-1.059 |
1.835 |
-0.290 |
H11 |
-2.890 |
1.420 |
-0.088 |
Atom - Atom Distances (Å)
|
S1 |
C2 |
C3 |
C4 |
C5 |
H6 |
H7 |
H8 |
H9 |
H10 |
H11 |
S1 | | 1.7468 | 1.7475 | 2.7213 | 2.7703 | 2.4208 | 2.3824 | 3.7305 | 2.9255 | 3.0135 | 3.7644 |
C2 | 1.7468 | | 2.7057 | 1.3377 | 2.9979 | 1.1066 | 3.6878 | 2.1174 | 2.1338 | 2.6035 | 4.0810 | C3 | 1.7475 | 2.7057 | | 3.9334 | 1.3390 | 2.7631 | 1.1038 | 4.7746 | 4.3645 | 2.1374 | 2.1158 | C4 | 2.7213 | 1.3377 | 3.9334 | | 4.1808 | 2.1443 | 4.8988 | 1.1008 | 1.1018 | 3.6070 | 5.2661 | C5 | 2.7703 | 2.9979 | 1.3390 | 4.1808 | | 2.6901 | 2.1343 | 4.8024 | 4.8050 | 1.1019 | 1.1001 | H6 | 2.4208 | 1.1066 | 2.7631 | 2.1443 | 2.6901 | | 3.7681 | 2.4842 | 3.1304 | 2.1877 | 3.6610 | H7 | 2.3824 | 3.6878 | 1.1038 | 4.8988 | 2.1343 | 3.7681 | | 5.7914 | 5.2224 | 3.1244 | 2.4659 | H8 | 3.7305 | 2.1174 | 4.7746 | 1.1008 | 4.8024 | 2.4842 | 5.7914 | | 1.8885 | 4.0514 | 5.8361 | H9 | 2.9255 | 2.1338 | 4.3645 | 1.1018 | 4.8050 | 3.1304 | 5.2224 | 1.8885 | | 4.3447 | 5.8990 | H10 | 3.0135 | 2.6035 | 2.1374 | 3.6070 | 1.1019 | 2.1877 | 3.1244 | 4.0514 | 4.3447 | | 1.8880 | H11 | 3.7644 | 4.0810 | 2.1158 | 5.2661 | 1.1001 | 3.6610 | 2.4659 | 5.8361 | 5.8990 | 1.8880 | |
More geometry information
Calculated Bond Angles
atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
S1 |
C2 |
C4 |
123.282 |
|
S1 |
C2 |
H6 |
114.192 |
S1 |
C3 |
C5 |
127.174 |
|
S1 |
C3 |
H7 |
111.338 |
C2 |
S1 |
C3 |
101.482 |
|
C2 |
C4 |
H8 |
120.221 |
C2 |
C4 |
H9 |
121.720 |
|
C3 |
C5 |
H10 |
121.939 |
C3 |
C5 |
H11 |
120.008 |
|
C4 |
C2 |
H6 |
122.351 |
C5 |
C3 |
H7 |
121.485 |
|
H8 |
C4 |
H9 |
118.052 |
H10 |
C5 |
H11 |
118.050 |
|
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at LSDA/cc-pVDZ
Charges (e)
Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
1 |
S |
0.105 |
|
|
|
2 |
C |
-0.197 |
|
|
|
3 |
C |
-0.190 |
|
|
|
4 |
C |
-0.066 |
|
|
|
5 |
C |
-0.075 |
|
|
|
6 |
H |
0.077 |
|
|
|
7 |
H |
0.077 |
|
|
|
8 |
H |
0.071 |
|
|
|
9 |
H |
0.067 |
|
|
|
10 |
H |
0.064 |
|
|
|
11 |
H |
0.065 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
|
x |
y |
z |
Total |
|
-0.133 |
0.694 |
0.196 |
0.733 |
CHELPG |
|
|
|
|
AIM |
|
|
|
|
ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
Primitive |
| x | y | z |
x |
-33.217 |
1.430 |
-0.741 |
y |
1.430 |
-36.684 |
1.046 |
z |
-0.741 |
1.046 |
-40.642 |
|
Traceless |
| x | y | z |
x |
5.446 |
1.430 |
-0.741 |
y |
1.430 |
0.246 |
1.046 |
z |
-0.741 |
1.046 |
-5.691 |
|
Polar |
3z2-r2 | -11.383 |
x2-y2 | 3.467 |
xy | 1.430 |
xz | -0.741 |
yz | 1.046 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
|
x |
y |
z |
x |
14.222 |
-0.094 |
-0.645 |
y |
-0.094 |
9.433 |
0.320 |
z |
-0.645 |
0.320 |
4.729 |
<r2> (average value of r
2) Å
2
<r2> |
164.831 |
(<r2>)1/2 |
12.839 |