Jump to
S1C2
Energy calculated at B3PW91/3-21G*
| | hartrees |
| Energy at 0K | -475.653793 |
| Energy at 298.15K | -475.660005 |
| HF Energy | -475.653793 |
| Nuclear repulsion energy | 106.902925 |
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 B3PW91/3-21G*
| 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' |
3137 |
3010 |
17.37 |
|
|
|
| 2 |
A' |
3080 |
2955 |
17.80 |
|
|
|
| 3 |
A' |
3063 |
2938 |
14.25 |
|
|
|
| 4 |
A' |
2694 |
2585 |
16.21 |
|
|
|
| 5 |
A' |
1564 |
1500 |
6.09 |
|
|
|
| 6 |
A' |
1537 |
1475 |
6.42 |
|
|
|
| 7 |
A' |
1461 |
1402 |
11.73 |
|
|
|
| 8 |
A' |
1338 |
1283 |
29.61 |
|
|
|
| 9 |
A' |
1133 |
1087 |
3.74 |
|
|
|
| 10 |
A' |
1005 |
964 |
6.32 |
|
|
|
| 11 |
A' |
877 |
841 |
1.96 |
|
|
|
| 12 |
A' |
674 |
646 |
0.99 |
|
|
|
| 13 |
A' |
312 |
300 |
2.97 |
|
|
|
| 14 |
A" |
3151 |
3024 |
23.24 |
|
|
|
| 15 |
A" |
3124 |
2997 |
0.06 |
|
|
|
| 16 |
A" |
1556 |
1493 |
12.19 |
|
|
|
| 17 |
A" |
1312 |
1259 |
1.23 |
|
|
|
| 18 |
A" |
1082 |
1038 |
0.02 |
|
|
|
| 19 |
A" |
819 |
786 |
8.32 |
|
|
|
| 20 |
A" |
253 |
242 |
0.64 |
|
|
|
| 21 |
A" |
145 |
139 |
23.84 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 16658.5 cm
-1
Scaled (by 0.9594) Zero Point Vibrational Energy (zpe) 15982.2 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 B3PW91/3-21G*
Point Group is Cs
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
1.530 |
0.679 |
0.000 |
| C2 |
0.000 |
0.836 |
0.000 |
| S3 |
-0.763 |
-0.836 |
0.000 |
| H4 |
2.005 |
1.667 |
0.000 |
| H5 |
1.862 |
0.133 |
0.890 |
| H6 |
1.862 |
0.133 |
-0.890 |
| H7 |
-0.322 |
1.384 |
0.892 |
| H8 |
-0.322 |
1.384 |
-0.892 |
| H9 |
-2.047 |
-0.424 |
0.000 |
Atom - Atom Distances (Å)
| |
C1 |
C2 |
S3 |
H4 |
H5 |
H6 |
H7 |
H8 |
H9 |
| C1 | | 1.5376 | 2.7483 | 1.0961 | 1.0956 | 1.0956 | 2.1726 | 2.1726 | 3.7429 |
C2 | 1.5376 | | 1.8382 | 2.1699 | 2.1803 | 2.1803 | 1.0947 | 1.0947 | 2.4041 | S3 | 2.7483 | 1.8382 | | 3.7318 | 2.9368 | 2.9368 | 2.4321 | 2.4321 | 1.3479 | H4 | 1.0961 | 2.1699 | 3.7318 | | 1.7788 | 1.7788 | 2.5079 | 2.5079 | 4.5595 | H5 | 1.0956 | 2.1803 | 2.9368 | 1.7788 | | 1.7796 | 2.5169 | 3.0835 | 4.0478 | H6 | 1.0956 | 2.1803 | 2.9368 | 1.7788 | 1.7796 | | 3.0835 | 2.5169 | 4.0478 | H7 | 2.1726 | 1.0947 | 2.4321 | 2.5079 | 2.5169 | 3.0835 | | 1.7834 | 2.6529 | H8 | 2.1726 | 1.0947 | 2.4321 | 2.5079 | 3.0835 | 2.5169 | 1.7834 | | 2.6529 | H9 | 3.7429 | 2.4041 | 1.3479 | 4.5595 | 4.0478 | 4.0478 | 2.6529 | 2.6529 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| C1 |
C2 |
S3 |
108.674 |
|
C1 |
C2 |
H7 |
110.116 |
| C1 |
C2 |
H8 |
110.116 |
|
C2 |
C1 |
H4 |
109.820 |
| C2 |
C1 |
H5 |
110.668 |
|
C2 |
C1 |
H6 |
110.668 |
| C2 |
S3 |
H9 |
96.766 |
|
S3 |
C2 |
H7 |
109.415 |
| S3 |
C2 |
H8 |
109.415 |
|
H4 |
C1 |
H5 |
108.505 |
| H4 |
C1 |
H6 |
108.505 |
|
H5 |
C1 |
H6 |
108.614 |
| H7 |
C2 |
H8 |
109.088 |
|
Electronic energy levels
Electronic state
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at B3PW91/3-21G*
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
-0.638 |
|
|
|
| 2 |
C |
-0.599 |
|
|
|
| 3 |
S |
-0.073 |
|
|
|
| 4 |
H |
0.225 |
|
|
|
| 5 |
H |
0.232 |
|
|
|
| 6 |
H |
0.232 |
|
|
|
| 7 |
H |
0.245 |
|
|
|
| 8 |
H |
0.245 |
|
|
|
| 9 |
H |
0.132 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
-0.035 |
1.792 |
0.000 |
1.793 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-24.351 |
-0.196 |
0.000 |
| y |
-0.196 |
-28.211 |
0.000 |
| z |
0.000 |
0.000 |
-28.845 |
|
| Traceless |
| | x | y | z |
| x |
4.177 |
-0.196 |
0.000 |
| y |
-0.196 |
-1.613 |
0.000 |
| z |
0.000 |
0.000 |
-2.564 |
|
| Polar |
| 3z2-r2 | -5.128 |
| x2-y2 | 3.859 |
| xy | -0.196 |
| xz | 0.000 |
| yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
6.012 |
0.756 |
0.000 |
| y |
0.756 |
5.561 |
0.000 |
| z |
0.000 |
0.000 |
4.058 |
<r2> (average value of r
2) Å
2
| <r2> |
83.800 |
| (<r2>)1/2 |
9.154 |
Jump to
S1C1
Energy calculated at B3PW91/3-21G*
| | hartrees |
| Energy at 0K | -475.654769 |
| Energy at 298.15K | -475.661162 |
| HF Energy | -475.654769 |
| Nuclear repulsion energy | 106.704083 |
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 B3PW91/3-21G*
| 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 |
3152 |
3024 |
20.04 |
|
|
|
| 2 |
A |
3129 |
3002 |
11.91 |
|
|
|
| 3 |
A |
3118 |
2992 |
11.86 |
|
|
|
| 4 |
A |
3081 |
2956 |
11.06 |
|
|
|
| 5 |
A |
3054 |
2930 |
18.99 |
|
|
|
| 6 |
A |
2700 |
2590 |
13.82 |
|
|
|
| 7 |
A |
1559 |
1496 |
5.06 |
|
|
|
| 8 |
A |
1553 |
1490 |
13.90 |
|
|
|
| 9 |
A |
1531 |
1469 |
6.69 |
|
|
|
| 10 |
A |
1459 |
1400 |
9.43 |
|
|
|
| 11 |
A |
1341 |
1287 |
10.04 |
|
|
|
| 12 |
A |
1320 |
1267 |
6.57 |
|
|
|
| 13 |
A |
1154 |
1107 |
10.94 |
|
|
|
| 14 |
A |
1088 |
1044 |
2.46 |
|
|
|
| 15 |
A |
990 |
950 |
7.41 |
|
|
|
| 16 |
A |
911 |
874 |
12.73 |
|
|
|
| 17 |
A |
761 |
730 |
3.91 |
|
|
|
| 18 |
A |
661 |
634 |
3.89 |
|
|
|
| 19 |
A |
339 |
325 |
1.76 |
|
|
|
| 20 |
A |
271 |
260 |
9.57 |
|
|
|
| 21 |
A |
240 |
231 |
15.18 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 16706.5 cm
-1
Scaled (by 0.9594) Zero Point Vibrational Energy (zpe) 16028.2 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 B3PW91/3-21G*
Point Group is C1
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
1.641 |
-0.357 |
-0.053 |
| C2 |
0.497 |
0.655 |
0.090 |
| S3 |
-1.166 |
-0.102 |
-0.080 |
| H4 |
2.610 |
0.155 |
0.005 |
| H5 |
1.600 |
-1.105 |
0.748 |
| H6 |
1.573 |
-0.877 |
-1.014 |
| H7 |
0.558 |
1.188 |
1.045 |
| H8 |
0.546 |
1.402 |
-0.711 |
| H9 |
-1.057 |
-0.925 |
0.982 |
Atom - Atom Distances (Å)
| |
C1 |
C2 |
S3 |
H4 |
H5 |
H6 |
H7 |
H8 |
H9 |
| C1 | | 1.5344 | 2.8192 | 1.0977 | 1.0963 | 1.0948 | 2.1835 | 2.1739 | 2.9453 |
C2 | 1.5344 | | 1.8354 | 2.1732 | 2.1787 | 2.1739 | 1.0950 | 1.0960 | 2.3890 | S3 | 2.8192 | 1.8354 | | 3.7862 | 3.0568 | 2.9961 | 2.4291 | 2.3647 | 1.3480 | H4 | 1.0977 | 2.1732 | 3.7862 | | 1.7771 | 1.7837 | 2.5221 | 2.5155 | 3.9458 | H5 | 1.0963 | 2.1787 | 3.0568 | 1.7771 | | 1.7765 | 2.5362 | 3.0856 | 2.6737 | H6 | 1.0948 | 2.1739 | 2.9961 | 1.7837 | 1.7765 | | 3.0881 | 2.5184 | 3.3020 | H7 | 2.1835 | 1.0950 | 2.4291 | 2.5221 | 2.5362 | 3.0881 | | 1.7684 | 2.6599 | H8 | 2.1739 | 1.0960 | 2.3647 | 2.5155 | 3.0856 | 2.5184 | 1.7684 | | 3.2938 | H9 | 2.9453 | 2.3890 | 1.3480 | 3.9458 | 2.6737 | 3.3020 | 2.6599 | 3.2938 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| C1 |
C2 |
S3 |
113.261 |
|
C1 |
C2 |
H7 |
111.181 |
| C1 |
C2 |
H8 |
110.355 |
|
C2 |
C1 |
H4 |
110.207 |
| C2 |
C1 |
H5 |
110.718 |
|
C2 |
C1 |
H6 |
110.429 |
| C2 |
S3 |
H9 |
96.050 |
|
S3 |
C2 |
H7 |
109.366 |
| S3 |
C2 |
H8 |
104.713 |
|
H4 |
C1 |
H5 |
108.188 |
| H4 |
C1 |
H6 |
108.892 |
|
H5 |
C1 |
H6 |
108.342 |
| H7 |
C2 |
H8 |
107.634 |
|
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at B3PW91/3-21G*
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
-0.622 |
|
|
|
| 2 |
C |
-0.608 |
|
|
|
| 3 |
S |
-0.070 |
|
|
|
| 4 |
H |
0.219 |
|
|
|
| 5 |
H |
0.215 |
|
|
|
| 6 |
H |
0.233 |
|
|
|
| 7 |
H |
0.247 |
|
|
|
| 8 |
H |
0.252 |
|
|
|
| 9 |
H |
0.134 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
1.646 |
0.049 |
0.833 |
1.845 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-29.048 |
1.344 |
-0.886 |
| y |
1.344 |
-26.861 |
-1.680 |
| z |
-0.886 |
-1.680 |
-26.847 |
|
| Traceless |
| | x | y | z |
| x |
-2.194 |
1.344 |
-0.886 |
| y |
1.344 |
1.086 |
-1.680 |
| z |
-0.886 |
-1.680 |
1.108 |
|
| Polar |
| 3z2-r2 | 2.215 |
| x2-y2 | -2.187 |
| xy | 1.344 |
| xz | -0.886 |
| yz | -1.680 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
6.319 |
0.490 |
0.062 |
| y |
0.490 |
4.760 |
-0.426 |
| z |
0.062 |
-0.426 |
4.634 |
<r2> (average value of r
2) Å
2
| <r2> |
84.280 |
| (<r2>)1/2 |
9.180 |