Jump to
S1C2
Energy calculated at PBEPBE/cc-pVDZ
| hartrees |
Energy at 0K | -553.795452 |
Energy at 298.15K | -553.800344 |
Nuclear repulsion energy | 196.938130 |
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/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 |
3187 |
3169 |
5.71 |
|
|
|
2 |
A |
3097 |
3079 |
2.39 |
|
|
|
3 |
A |
3084 |
3066 |
6.68 |
|
|
|
4 |
A |
1621 |
1612 |
4.23 |
|
|
|
5 |
A |
1353 |
1345 |
7.26 |
|
|
|
6 |
A |
1248 |
1241 |
0.63 |
|
|
|
7 |
A |
1013 |
1007 |
0.97 |
|
|
|
8 |
A |
928 |
923 |
0.00 |
|
|
|
9 |
A |
828 |
823 |
0.00 |
|
|
|
10 |
A |
703 |
699 |
0.32 |
|
|
|
11 |
A |
594 |
591 |
0.00 |
|
|
|
12 |
A |
395 |
393 |
0.67 |
|
|
|
13 |
A |
168 |
167 |
0.16 |
|
|
|
14 |
A |
58 |
58 |
0.00 |
|
|
|
15 |
A |
3188 |
3169 |
0.10 |
|
|
|
16 |
A |
3099 |
3081 |
0.61 |
|
|
|
17 |
A |
3085 |
3067 |
0.18 |
|
|
|
18 |
A |
1596 |
1587 |
167.02 |
|
|
|
19 |
A |
1349 |
1341 |
5.15 |
|
|
|
20 |
A |
1219 |
1212 |
14.16 |
|
|
|
21 |
A |
984 |
978 |
31.22 |
|
|
|
22 |
A |
936 |
931 |
47.37 |
|
|
|
23 |
A |
829 |
824 |
58.08 |
|
|
|
24 |
A |
719 |
715 |
42.35 |
|
|
|
25 |
A |
529 |
526 |
20.71 |
|
|
|
26 |
A |
375 |
373 |
4.70 |
|
|
|
27 |
A |
35 |
35 |
0.18 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 18109.2 cm
-1
Scaled (by 0.9942) Zero Point Vibrational Energy (zpe) 18004.2 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 PBEPBE/cc-pVDZ
Point Group is C2
Cartesians (Å)
Atom |
x (Å) |
y (Å) |
z (Å) |
S1 |
0.000 |
0.000 |
0.627 |
C2 |
0.000 |
1.371 |
-0.493 |
C3 |
0.000 |
-1.371 |
-0.493 |
C4 |
0.001 |
2.660 |
-0.101 |
C5 |
-0.001 |
-2.660 |
-0.101 |
H6 |
-0.001 |
1.092 |
-1.560 |
H7 |
0.001 |
-1.092 |
-1.560 |
H8 |
0.000 |
3.460 |
-0.854 |
H9 |
0.001 |
2.955 |
0.959 |
H10 |
-0.000 |
-3.460 |
-0.854 |
H11 |
-0.001 |
-2.955 |
0.959 |
Atom - Atom Distances (Å)
|
S1 |
C2 |
C3 |
C4 |
C5 |
H6 |
H7 |
H8 |
H9 |
H10 |
H11 |
S1 | | 1.7706 | 1.7706 | 2.7576 | 2.7576 | 2.4448 | 2.4448 | 3.7638 | 2.9735 | 3.7638 | 2.9735 |
C2 | 1.7706 | | 2.7428 | 1.3464 | 4.0500 | 1.1030 | 2.6850 | 2.1197 | 2.1481 | 4.8450 | 4.5634 | C3 | 1.7706 | 2.7428 | | 4.0500 | 1.3464 | 2.6850 | 1.1030 | 4.8450 | 4.5634 | 2.1197 | 2.1481 | C4 | 2.7576 | 1.3464 | 4.0500 | | 5.3193 | 2.1411 | 4.0257 | 1.0988 | 1.1001 | 6.1659 | 5.7138 | C5 | 2.7576 | 4.0500 | 1.3464 | 5.3193 | | 4.0257 | 2.1411 | 6.1659 | 5.7138 | 1.0988 | 1.1001 | H6 | 2.4448 | 1.1030 | 2.6850 | 2.1411 | 4.0257 | | 2.1848 | 2.4707 | 3.1324 | 4.6069 | 4.7670 | H7 | 2.4448 | 2.6850 | 1.1030 | 4.0257 | 2.1411 | 2.1848 | | 4.6069 | 4.7670 | 2.4707 | 3.1324 | H8 | 3.7638 | 2.1197 | 4.8450 | 1.0988 | 6.1659 | 2.4707 | 4.6069 | | 1.8816 | 6.9202 | 6.6662 | H9 | 2.9735 | 2.1481 | 4.5634 | 1.1001 | 5.7138 | 3.1324 | 4.7670 | 1.8816 | | 6.6662 | 5.9100 | H10 | 3.7638 | 4.8450 | 2.1197 | 6.1659 | 1.0988 | 4.6069 | 2.4707 | 6.9202 | 6.6662 | | 1.8816 | H11 | 2.9735 | 4.5634 | 2.1481 | 5.7138 | 1.1001 | 4.7670 | 3.1324 | 6.6662 | 5.9100 | 1.8816 | |
More geometry information
Calculated Bond Angles
atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
S1 |
C2 |
C4 |
123.851 |
|
S1 |
C2 |
H6 |
114.587 |
S1 |
C3 |
C5 |
123.851 |
|
S1 |
C3 |
H7 |
114.587 |
C2 |
S1 |
C3 |
101.523 |
|
C2 |
C4 |
H8 |
119.847 |
C2 |
C4 |
H9 |
122.486 |
|
C3 |
C5 |
H10 |
119.847 |
C3 |
C5 |
H11 |
122.486 |
|
C4 |
C2 |
H6 |
121.562 |
C5 |
C3 |
H7 |
121.562 |
|
H8 |
C4 |
H9 |
117.667 |
H10 |
C5 |
H11 |
117.667 |
|
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at PBEPBE/cc-pVDZ
Charges (e)
Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
1 |
S |
0.117 |
|
|
|
2 |
C |
-0.162 |
|
|
|
3 |
C |
-0.162 |
|
|
|
4 |
C |
-0.004 |
|
|
|
5 |
C |
-0.004 |
|
|
|
6 |
H |
0.036 |
|
|
|
7 |
H |
0.036 |
|
|
|
8 |
H |
0.039 |
|
|
|
9 |
H |
0.033 |
|
|
|
10 |
H |
0.039 |
|
|
|
11 |
H |
0.033 |
|
|
|
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 |
-0.990 |
0.990 |
CHELPG |
|
|
|
|
AIM |
|
|
|
|
ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
Primitive |
| x | y | z |
x |
-41.915 |
0.001 |
0.000 |
y |
0.001 |
-33.977 |
0.000 |
z |
0.000 |
0.000 |
-35.079 |
|
Traceless |
| x | y | z |
x |
-7.387 |
0.001 |
0.000 |
y |
0.001 |
4.520 |
0.000 |
z |
0.000 |
0.000 |
2.867 |
|
Polar |
3z2-r2 | 5.734 |
x2-y2 | -7.938 |
xy | 0.001 |
xz | 0.000 |
yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
|
x |
y |
z |
x |
3.873 |
0.003 |
0.000 |
y |
0.003 |
17.917 |
0.000 |
z |
0.000 |
0.000 |
8.117 |
<r2> (average value of r
2) Å
2
<r2> |
191.846 |
(<r2>)1/2 |
13.851 |
Jump to
S1C1
Energy calculated at PBEPBE/cc-pVDZ
| hartrees |
Energy at 0K | -553.795839 |
Energy at 298.15K | -553.801134 |
HF Energy | -553.795839 |
Nuclear repulsion energy | 199.974019 |
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/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 |
3187 |
3169 |
4.32 |
|
|
|
2 |
A |
3184 |
3166 |
3.29 |
|
|
|
3 |
A |
3109 |
3091 |
2.51 |
|
|
|
4 |
A |
3094 |
3076 |
3.84 |
|
|
|
5 |
A |
3087 |
3069 |
1.20 |
|
|
|
6 |
A |
3080 |
3062 |
1.71 |
|
|
|
7 |
A |
1608 |
1599 |
55.81 |
|
|
|
8 |
A |
1600 |
1590 |
32.94 |
|
|
|
9 |
A |
1351 |
1343 |
4.20 |
|
|
|
10 |
A |
1348 |
1340 |
5.60 |
|
|
|
11 |
A |
1244 |
1237 |
1.24 |
|
|
|
12 |
A |
1225 |
1218 |
8.99 |
|
|
|
13 |
A |
1011 |
1005 |
14.24 |
|
|
|
14 |
A |
983 |
977 |
9.10 |
|
|
|
15 |
A |
952 |
946 |
24.56 |
|
|
|
16 |
A |
936 |
930 |
32.06 |
|
|
|
17 |
A |
863 |
858 |
25.56 |
|
|
|
18 |
A |
829 |
824 |
31.96 |
|
|
|
19 |
A |
721 |
717 |
15.89 |
|
|
|
20 |
A |
678 |
674 |
5.04 |
|
|
|
21 |
A |
598 |
594 |
10.34 |
|
|
|
22 |
A |
579 |
576 |
13.08 |
|
|
|
23 |
A |
453 |
451 |
0.52 |
|
|
|
24 |
A |
351 |
349 |
0.45 |
|
|
|
25 |
A |
210 |
209 |
0.65 |
|
|
|
26 |
A |
153 |
152 |
4.00 |
|
|
|
27 |
A |
91 |
91 |
0.75 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 18261.6 cm
-1
Scaled (by 0.9942) Zero Point Vibrational Energy (zpe) 18155.7 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/cc-pVDZ
Point Group is C1
Cartesians (Å)
Atom |
x (Å) |
y (Å) |
z (Å) |
S1 |
0.031 |
-0.959 |
0.007 |
C2 |
1.086 |
0.431 |
0.309 |
C3 |
-1.583 |
-0.229 |
-0.005 |
C4 |
2.336 |
0.526 |
-0.184 |
C5 |
-1.909 |
1.072 |
-0.136 |
H6 |
0.674 |
1.179 |
1.008 |
H7 |
-2.358 |
-1.003 |
0.117 |
H8 |
2.992 |
1.351 |
0.131 |
H9 |
2.743 |
-0.212 |
-0.891 |
H10 |
-1.158 |
1.859 |
-0.293 |
H11 |
-2.965 |
1.375 |
-0.092 |
Atom - Atom Distances (Å)
|
S1 |
C2 |
C3 |
C4 |
C5 |
H6 |
H7 |
H8 |
H9 |
H10 |
H11 |
S1 | | 1.7714 | 1.7712 | 2.7489 | 2.8127 | 2.4469 | 2.3921 | 3.7576 | 2.9529 | 3.0734 | 3.7996 |
C2 | 1.7714 | | 2.7672 | 1.3466 | 3.0955 | 1.1036 | 3.7360 | 2.1234 | 2.1441 | 2.7270 | 4.1792 | C3 | 1.7712 | 2.7672 | | 3.9945 | 1.3477 | 2.8467 | 1.1025 | 4.8416 | 4.4153 | 2.1501 | 2.1196 | C4 | 2.7489 | 1.3466 | 3.9945 | | 4.2802 | 2.1466 | 4.9460 | 1.1000 | 1.1002 | 3.7405 | 5.3692 | C5 | 2.8127 | 3.0955 | 1.3477 | 4.2802 | | 2.8279 | 2.1379 | 4.9164 | 4.8850 | 1.0995 | 1.0994 | H6 | 2.4469 | 1.1036 | 2.8467 | 2.1466 | 2.8279 | | 3.8407 | 2.4839 | 3.1337 | 2.3481 | 3.8074 | H7 | 2.3921 | 3.7360 | 1.1025 | 4.9460 | 2.1379 | 3.8407 | | 5.8451 | 5.2596 | 3.1304 | 2.4632 | H8 | 3.7576 | 2.1234 | 4.8416 | 1.1000 | 4.9164 | 2.4839 | 5.8451 | | 1.8842 | 4.2021 | 5.9613 | H9 | 2.9529 | 2.1441 | 4.4153 | 1.1002 | 4.8850 | 3.1337 | 5.2596 | 1.8842 | | 4.4568 | 5.9784 | H10 | 3.0734 | 2.7270 | 2.1501 | 3.7405 | 1.0995 | 2.3481 | 3.1304 | 4.2021 | 4.4568 | | 1.8818 | H11 | 3.7996 | 4.1792 | 2.1196 | 5.3692 | 1.0994 | 3.8074 | 2.4632 | 5.9613 | 5.9784 | 1.8818 | |
More geometry information
Calculated Bond Angles
atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
S1 |
C2 |
C4 |
123.095 |
|
S1 |
C2 |
H6 |
114.661 |
S1 |
C3 |
C5 |
128.283 |
|
S1 |
C3 |
H7 |
110.530 |
C2 |
S1 |
C3 |
102.727 |
|
C2 |
C4 |
H8 |
120.098 |
C2 |
C4 |
H9 |
122.070 |
|
C3 |
C5 |
H10 |
122.622 |
C3 |
C5 |
H11 |
119.683 |
|
C4 |
C2 |
H6 |
122.035 |
C5 |
C3 |
H7 |
121.186 |
|
H8 |
C4 |
H9 |
117.822 |
H10 |
C5 |
H11 |
117.695 |
|
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at PBEPBE/cc-pVDZ
Charges (e)
Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
1 |
S |
0.085 |
|
|
|
2 |
C |
-0.166 |
|
|
|
3 |
C |
-0.159 |
|
|
|
4 |
C |
0.009 |
|
|
|
5 |
C |
-0.004 |
|
|
|
6 |
H |
0.045 |
|
|
|
7 |
H |
0.044 |
|
|
|
8 |
H |
0.040 |
|
|
|
9 |
H |
0.036 |
|
|
|
10 |
H |
0.035 |
|
|
|
11 |
H |
0.035 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
|
x |
y |
z |
Total |
|
-0.101 |
0.740 |
0.204 |
0.774 |
CHELPG |
|
|
|
|
AIM |
|
|
|
|
ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
Primitive |
| x | y | z |
x |
-33.329 |
1.403 |
-0.692 |
y |
1.403 |
-36.803 |
1.022 |
z |
-0.692 |
1.022 |
-40.513 |
|
Traceless |
| x | y | z |
x |
5.329 |
1.403 |
-0.692 |
y |
1.403 |
0.118 |
1.022 |
z |
-0.692 |
1.022 |
-5.446 |
|
Polar |
3z2-r2 | -10.893 |
x2-y2 | 3.474 |
xy | 1.403 |
xz | -0.692 |
yz | 1.022 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
|
x |
y |
z |
x |
14.414 |
-0.098 |
-0.663 |
y |
-0.098 |
9.423 |
0.314 |
z |
-0.663 |
0.314 |
4.799 |
<r2> (average value of r
2) Å
2
<r2> |
169.538 |
(<r2>)1/2 |
13.021 |