Jump to
S1C2
Energy calculated at B3LYP/6-311G**
| hartrees |
Energy at 0K | -554.242095 |
Energy at 298.15K | -554.247297 |
Nuclear repulsion energy | 198.138430 |
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/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 |
3225 |
3118 |
9.47 |
|
|
|
2 |
A |
3162 |
3057 |
5.40 |
|
|
|
3 |
A |
3137 |
3033 |
1.37 |
|
|
|
4 |
A |
1660 |
1605 |
6.21 |
|
|
|
5 |
A |
1420 |
1373 |
10.40 |
|
|
|
6 |
A |
1306 |
1263 |
0.71 |
|
|
|
7 |
A |
1057 |
1021 |
0.43 |
|
|
|
8 |
A |
997 |
964 |
7.75 |
|
|
|
9 |
A |
925 |
894 |
19.02 |
|
|
|
10 |
A |
722 |
698 |
0.58 |
|
|
|
11 |
A |
624 |
603 |
11.98 |
|
|
|
12 |
A |
382 |
369 |
0.44 |
|
|
|
13 |
A |
186 |
180 |
0.00 |
|
|
|
14 |
A |
75 |
73 |
0.17 |
|
|
|
15 |
A |
3225 |
3118 |
5.61 |
|
|
|
16 |
A |
3158 |
3053 |
9.45 |
|
|
|
17 |
A |
3137 |
3033 |
2.40 |
|
|
|
18 |
A |
1642 |
1588 |
93.68 |
|
|
|
19 |
A |
1413 |
1366 |
5.10 |
|
|
|
20 |
A |
1293 |
1250 |
17.18 |
|
|
|
21 |
A |
1038 |
1003 |
11.35 |
|
|
|
22 |
A |
988 |
955 |
77.24 |
|
|
|
23 |
A |
925 |
894 |
54.66 |
|
|
|
24 |
A |
708 |
685 |
25.87 |
|
|
|
25 |
A |
595 |
575 |
19.58 |
|
|
|
26 |
A |
399 |
386 |
1.59 |
|
|
|
27 |
A |
67 |
65 |
3.16 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 18732.4 cm
-1
Scaled (by 0.9668) Zero Point Vibrational Energy (zpe) 18110.5 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 B3LYP/6-311G**
Point Group is C2
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at B3LYP/6-311G**
Charges (e)
Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
1 |
S |
0.195 |
|
|
|
2 |
C |
-0.295 |
|
|
|
3 |
C |
-0.295 |
|
|
|
4 |
C |
-0.185 |
|
|
|
5 |
C |
-0.185 |
|
|
|
6 |
H |
0.145 |
|
|
|
7 |
H |
0.145 |
|
|
|
8 |
H |
0.118 |
|
|
|
9 |
H |
0.121 |
|
|
|
10 |
H |
0.118 |
|
|
|
11 |
H |
0.121 |
|
|
|
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 |
-1.199 |
1.199 |
CHELPG |
|
|
|
|
AIM |
|
|
|
|
ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
Primitive |
| x | y | z |
x |
-40.509 |
-1.742 |
0.000 |
y |
-1.742 |
-33.299 |
0.000 |
z |
0.000 |
0.000 |
-37.459 |
|
Traceless |
| x | y | z |
x |
-5.130 |
-1.742 |
0.000 |
y |
-1.742 |
5.684 |
0.000 |
z |
0.000 |
0.000 |
-0.555 |
|
Polar |
3z2-r2 | -1.109 |
x2-y2 | -7.209 |
xy | -1.742 |
xz | 0.000 |
yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
|
x |
y |
z |
x |
6.087 |
-2.977 |
0.000 |
y |
-2.977 |
15.944 |
0.000 |
z |
0.000 |
0.000 |
7.617 |
<r2> (average value of r
2) Å
2
<r2> |
187.228 |
(<r2>)1/2 |
13.683 |
Jump to
S1C1
Energy calculated at B3LYP/6-311G**
| hartrees |
Energy at 0K | -554.242965 |
Energy at 298.15K | -554.248403 |
HF Energy | -554.242965 |
Nuclear repulsion energy | 201.288531 |
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/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 |
3228 |
3120 |
8.15 |
|
|
|
2 |
A |
3225 |
3118 |
6.33 |
|
|
|
3 |
A |
3166 |
3060 |
4.48 |
|
|
|
4 |
A |
3154 |
3049 |
6.61 |
|
|
|
5 |
A |
3141 |
3037 |
1.37 |
|
|
|
6 |
A |
3136 |
3032 |
2.47 |
|
|
|
7 |
A |
1653 |
1598 |
42.79 |
|
|
|
8 |
A |
1643 |
1589 |
34.93 |
|
|
|
9 |
A |
1421 |
1373 |
5.05 |
|
|
|
10 |
A |
1417 |
1370 |
7.31 |
|
|
|
11 |
A |
1307 |
1264 |
2.13 |
|
|
|
12 |
A |
1295 |
1252 |
9.67 |
|
|
|
13 |
A |
1059 |
1024 |
10.44 |
|
|
|
14 |
A |
1034 |
999 |
13.30 |
|
|
|
15 |
A |
999 |
966 |
26.34 |
|
|
|
16 |
A |
986 |
954 |
34.06 |
|
|
|
17 |
A |
937 |
906 |
36.48 |
|
|
|
18 |
A |
899 |
869 |
43.97 |
|
|
|
19 |
A |
725 |
701 |
15.10 |
|
|
|
20 |
A |
677 |
655 |
4.95 |
|
|
|
21 |
A |
628 |
607 |
18.32 |
|
|
|
22 |
A |
604 |
584 |
15.32 |
|
|
|
23 |
A |
462 |
446 |
0.64 |
|
|
|
24 |
A |
368 |
355 |
0.43 |
|
|
|
25 |
A |
214 |
207 |
1.11 |
|
|
|
26 |
A |
146 |
141 |
4.57 |
|
|
|
27 |
A |
89 |
86 |
1.49 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 18805.3 cm
-1
Scaled (by 0.9668) Zero Point Vibrational Energy (zpe) 18180.9 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/6-311G**
Point Group is C1
Cartesians (Å)
Atom |
x (Å) |
y (Å) |
z (Å) |
S1 |
0.019 |
-0.975 |
0.002 |
C2 |
1.097 |
0.385 |
0.363 |
C3 |
-1.575 |
-0.201 |
-0.018 |
C4 |
2.283 |
0.549 |
-0.216 |
C5 |
-1.854 |
1.096 |
-0.131 |
H6 |
0.752 |
1.036 |
1.161 |
H7 |
-2.364 |
-0.939 |
0.081 |
H8 |
2.954 |
1.332 |
0.119 |
H9 |
2.625 |
-0.091 |
-1.021 |
H10 |
-1.088 |
1.851 |
-0.260 |
H11 |
-2.884 |
1.433 |
-0.104 |
Atom - Atom Distances (Å)
|
S1 |
C2 |
C3 |
C4 |
C5 |
H6 |
H7 |
H8 |
H9 |
H10 |
H11 |
S1 | | 1.7725 | 1.7723 | 2.7379 | 2.7960 | 2.4339 | 2.3843 | 3.7350 | 2.9363 | 3.0459 | 3.7732 |
C2 | 1.7725 | | 2.7619 | 1.3304 | 3.0759 | 1.0860 | 3.7162 | 2.0990 | 2.1166 | 2.7037 | 4.1429 | C3 | 1.7723 | 2.7619 | | 3.9354 | 1.3315 | 2.8870 | 1.0852 | 4.7835 | 4.3200 | 2.1222 | 2.0952 | C4 | 2.7379 | 1.3304 | 3.9354 | | 4.1747 | 2.1166 | 4.8885 | 1.0842 | 1.0838 | 3.6142 | 5.2436 | C5 | 2.7960 | 3.0759 | 1.3315 | 4.1747 | | 2.9099 | 2.1093 | 4.8209 | 4.7191 | 1.0831 | 1.0835 | H6 | 2.4339 | 1.0860 | 2.8870 | 2.1166 | 2.9099 | | 3.8440 | 2.4546 | 3.0893 | 2.4634 | 3.8700 | H7 | 2.3843 | 3.7162 | 1.0852 | 4.8885 | 2.1093 | 3.8440 | | 5.7828 | 5.1794 | 3.0869 | 2.4361 | H8 | 3.7350 | 2.0990 | 4.7835 | 1.0842 | 4.8209 | 2.4546 | 5.7828 | | 1.8526 | 4.0929 | 5.8433 | H9 | 2.9363 | 2.1166 | 4.3200 | 1.0838 | 4.7191 | 3.0893 | 5.1794 | 1.8526 | | 4.2589 | 5.7894 | H10 | 3.0459 | 2.7037 | 2.1222 | 3.6142 | 1.0831 | 2.4634 | 3.0869 | 4.0929 | 4.2589 | | 1.8504 | H11 | 3.7732 | 4.1429 | 2.0952 | 5.2436 | 1.0835 | 3.8700 | 2.4361 | 5.8433 | 5.7894 | 1.8504 | |
More geometry information
Calculated Bond Angles
atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
S1 |
C2 |
C4 |
123.223 |
|
S1 |
C2 |
H6 |
114.603 |
S1 |
C3 |
C5 |
127.967 |
|
S1 |
C3 |
H7 |
110.802 |
C2 |
S1 |
C3 |
102.364 |
|
C2 |
C4 |
H8 |
120.409 |
C2 |
C4 |
H9 |
122.172 |
|
C3 |
C5 |
H10 |
122.685 |
C3 |
C5 |
H11 |
119.998 |
|
C4 |
C2 |
H6 |
121.980 |
C5 |
C3 |
H7 |
121.230 |
|
H8 |
C4 |
H9 |
117.414 |
H10 |
C5 |
H11 |
117.315 |
|
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at B3LYP/6-311G**
Charges (e)
Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
1 |
S |
0.199 |
|
|
|
2 |
C |
-0.299 |
|
|
|
3 |
C |
-0.284 |
|
|
|
4 |
C |
-0.182 |
|
|
|
5 |
C |
-0.206 |
|
|
|
6 |
H |
0.149 |
|
|
|
7 |
H |
0.144 |
|
|
|
8 |
H |
0.119 |
|
|
|
9 |
H |
0.125 |
|
|
|
10 |
H |
0.118 |
|
|
|
11 |
H |
0.117 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
|
x |
y |
z |
Total |
|
-0.039 |
0.999 |
0.196 |
1.018 |
CHELPG |
|
|
|
|
AIM |
|
|
|
|
ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
Primitive |
| x | y | z |
x |
-33.322 |
1.655 |
-0.745 |
y |
1.655 |
-37.844 |
1.123 |
z |
-0.745 |
1.123 |
-40.848 |
|
Traceless |
| x | y | z |
x |
6.023 |
1.655 |
-0.745 |
y |
1.655 |
-0.758 |
1.123 |
z |
-0.745 |
1.123 |
-5.265 |
|
Polar |
3z2-r2 | -10.530 |
x2-y2 | 4.521 |
xy | 1.655 |
xz | -0.745 |
yz | 1.123 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
|
x |
y |
z |
x |
13.479 |
-0.086 |
-0.719 |
y |
-0.086 |
9.686 |
0.218 |
z |
-0.719 |
0.218 |
5.413 |
<r2> (average value of r
2) Å
2
<r2> |
166.859 |
(<r2>)1/2 |
12.917 |