Jump to
S1C2
Energy calculated at HF/LANL2DZ
| | hartrees |
| Energy at 0K | -89.077950 |
| Energy at 298.15K | -89.084321 |
| HF Energy | -89.077950 |
| Nuclear repulsion energy | 64.564731 |
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 HF/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' |
3293 |
2964 |
69.19 |
|
|
|
| 2 |
A' |
3274 |
2946 |
17.10 |
|
|
|
| 3 |
A' |
3207 |
2886 |
43.54 |
|
|
|
| 4 |
A' |
2708 |
2437 |
35.95 |
|
|
|
| 5 |
A' |
1651 |
1485 |
5.23 |
|
|
|
| 6 |
A' |
1642 |
1478 |
3.87 |
|
|
|
| 7 |
A' |
1574 |
1417 |
8.01 |
|
|
|
| 8 |
A' |
1454 |
1308 |
49.46 |
|
|
|
| 9 |
A' |
1213 |
1092 |
3.87 |
|
|
|
| 10 |
A' |
1079 |
971 |
6.68 |
|
|
|
| 11 |
A' |
916 |
824 |
6.06 |
|
|
|
| 12 |
A' |
670 |
603 |
6.86 |
|
|
|
| 13 |
A' |
327 |
295 |
5.10 |
|
|
|
| 14 |
A" |
3348 |
3013 |
53.17 |
|
|
|
| 15 |
A" |
3301 |
2971 |
23.46 |
|
|
|
| 16 |
A" |
1642 |
1478 |
10.20 |
|
|
|
| 17 |
A" |
1397 |
1257 |
1.40 |
|
|
|
| 18 |
A" |
1164 |
1048 |
0.01 |
|
|
|
| 19 |
A" |
872 |
785 |
5.68 |
|
|
|
| 20 |
A" |
262 |
236 |
1.87 |
|
|
|
| 21 |
A" |
184 |
166 |
34.73 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 17589.7 cm
-1
Scaled (by 0.8999) Zero Point Vibrational Energy (zpe) 15829.0 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 HF/LANL2DZ
Point Group is Cs
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
1.221 |
-0.335 |
0.000 |
| C2 |
0.000 |
0.588 |
0.000 |
| S3 |
-1.566 |
-0.465 |
0.000 |
| H4 |
2.129 |
0.257 |
0.000 |
| H5 |
1.231 |
-0.969 |
0.878 |
| H6 |
1.231 |
-0.969 |
-0.878 |
| H7 |
-0.014 |
1.213 |
0.879 |
| H8 |
-0.014 |
1.213 |
-0.879 |
| H9 |
-2.489 |
0.525 |
0.000 |
Atom - Atom Distances (Å)
| |
C1 |
C2 |
S3 |
H4 |
H5 |
H6 |
H7 |
H8 |
H9 |
| C1 | | 1.5303 | 2.7900 | 1.0845 | 1.0830 | 1.0830 | 2.1665 | 2.1665 | 3.8077 |
C2 | 1.5303 | | 1.8871 | 2.1546 | 2.1704 | 2.1704 | 1.0786 | 1.0786 | 2.4894 | S3 | 2.7900 | 1.8871 | | 3.7653 | 2.9747 | 2.9747 | 2.4484 | 2.4484 | 1.3529 | H4 | 1.0845 | 2.1546 | 3.7653 | | 1.7557 | 1.7557 | 2.5061 | 2.5061 | 4.6255 | H5 | 1.0830 | 2.1704 | 2.9747 | 1.7557 | | 1.7555 | 2.5125 | 3.0657 | 4.1034 | H6 | 1.0830 | 2.1704 | 2.9747 | 1.7557 | 1.7555 | | 3.0657 | 2.5125 | 4.1034 | H7 | 2.1665 | 1.0786 | 2.4484 | 2.5061 | 2.5125 | 3.0657 | | 1.7581 | 2.7142 | H8 | 2.1665 | 1.0786 | 2.4484 | 2.5061 | 3.0657 | 2.5125 | 1.7581 | | 2.7142 | H9 | 3.8077 | 2.4894 | 1.3529 | 4.6255 | 4.1034 | 4.1034 | 2.7142 | 2.7142 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| C1 |
C2 |
S3 |
109.005 |
|
C1 |
C2 |
H7 |
111.105 |
| C1 |
C2 |
H8 |
111.105 |
|
C2 |
C1 |
H4 |
109.800 |
| C2 |
C1 |
H5 |
111.145 |
|
C2 |
C1 |
H6 |
111.145 |
| C2 |
S3 |
H9 |
99.074 |
|
S3 |
C2 |
H7 |
108.180 |
| S3 |
C2 |
H8 |
108.180 |
|
H4 |
C1 |
H5 |
108.186 |
| H4 |
C1 |
H6 |
108.186 |
|
H5 |
C1 |
H6 |
108.278 |
| H7 |
C2 |
H8 |
109.174 |
|
Electronic energy levels
Electronic state
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at HF/LANL2DZ
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
-0.497 |
|
|
|
| 2 |
C |
-0.513 |
|
|
|
| 3 |
S |
-0.043 |
|
|
|
| 4 |
H |
0.181 |
|
|
|
| 5 |
H |
0.193 |
|
|
|
| 6 |
H |
0.193 |
|
|
|
| 7 |
H |
0.215 |
|
|
|
| 8 |
H |
0.215 |
|
|
|
| 9 |
H |
0.056 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
1.161 |
1.943 |
0.000 |
2.263 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-26.750 |
-3.150 |
0.000 |
| y |
-3.150 |
-27.738 |
0.000 |
| z |
0.000 |
0.000 |
-28.446 |
|
| Traceless |
| | x | y | z |
| x |
1.342 |
-3.150 |
0.000 |
| y |
-3.150 |
-0.140 |
0.000 |
| z |
0.000 |
0.000 |
-1.202 |
|
| Polar |
| 3z2-r2 | -2.404 |
| x2-y2 | 0.987 |
| xy | -3.150 |
| xz | 0.000 |
| yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
7.048 |
0.397 |
0.000 |
| y |
0.397 |
5.105 |
0.000 |
| z |
0.000 |
0.000 |
3.267 |
<r2> (average value of r
2) Å
2
| <r2> |
66.974 |
| (<r2>)1/2 |
8.184 |
Jump to
S1C1
Energy calculated at HF/LANL2DZ
| | hartrees |
| Energy at 0K | -89.078316 |
| Energy at 298.15K | -89.084740 |
| HF Energy | -89.078316 |
| Nuclear repulsion energy | 64.639665 |
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 HF/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 |
3348 |
3013 |
37.18 |
|
|
|
| 2 |
A |
3300 |
2970 |
30.59 |
|
|
|
| 3 |
A |
3284 |
2955 |
81.35 |
|
|
|
| 4 |
A |
3271 |
2943 |
4.76 |
|
|
|
| 5 |
A |
3199 |
2879 |
44.69 |
|
|
|
| 6 |
A |
2712 |
2440 |
30.58 |
|
|
|
| 7 |
A |
1647 |
1482 |
5.78 |
|
|
|
| 8 |
A |
1640 |
1476 |
12.42 |
|
|
|
| 9 |
A |
1633 |
1470 |
3.90 |
|
|
|
| 10 |
A |
1573 |
1415 |
6.20 |
|
|
|
| 11 |
A |
1453 |
1308 |
24.86 |
|
|
|
| 12 |
A |
1404 |
1263 |
3.26 |
|
|
|
| 13 |
A |
1234 |
1110 |
11.95 |
|
|
|
| 14 |
A |
1175 |
1057 |
2.12 |
|
|
|
| 15 |
A |
1075 |
967 |
10.50 |
|
|
|
| 16 |
A |
939 |
845 |
13.12 |
|
|
|
| 17 |
A |
805 |
725 |
2.45 |
|
|
|
| 18 |
A |
665 |
598 |
12.07 |
|
|
|
| 19 |
A |
348 |
313 |
1.70 |
|
|
|
| 20 |
A |
266 |
239 |
1.65 |
|
|
|
| 21 |
A |
211 |
190 |
32.18 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 17589.7 cm
-1
Scaled (by 0.8999) Zero Point Vibrational Energy (zpe) 15829.0 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 HF/LANL2DZ
Point Group is C1
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
1.662 |
-0.363 |
-0.052 |
| C2 |
0.531 |
0.656 |
0.091 |
| S3 |
-1.187 |
-0.097 |
-0.082 |
| H4 |
2.623 |
0.136 |
0.017 |
| H5 |
1.618 |
-1.113 |
0.730 |
| H6 |
1.608 |
-0.870 |
-1.007 |
| H7 |
0.576 |
1.168 |
1.040 |
| H8 |
0.569 |
1.396 |
-0.694 |
| H9 |
-1.156 |
-0.923 |
0.989 |
Atom - Atom Distances (Å)
| |
C1 |
C2 |
S3 |
H4 |
H5 |
H6 |
H7 |
H8 |
H9 |
| C1 | | 1.5298 | 2.8617 | 1.0857 | 1.0843 | 1.0825 | 2.1718 | 2.1684 | 3.0560 |
C2 | 1.5298 | | 1.8837 | 2.1578 | 2.1730 | 2.1674 | 1.0787 | 1.0792 | 2.4788 | S3 | 2.8617 | 1.8837 | | 3.8190 | 3.0924 | 3.0442 | 2.4427 | 2.3844 | 1.3525 | H4 | 1.0857 | 2.1578 | 3.8190 | | 1.7547 | 1.7584 | 2.5107 | 2.5128 | 4.0438 | H5 | 1.0843 | 2.1730 | 3.0924 | 1.7547 | | 1.7543 | 2.5268 | 3.0698 | 2.7933 | H6 | 1.0825 | 2.1674 | 3.0442 | 1.7584 | 1.7543 | | 3.0674 | 2.5125 | 3.4102 | H7 | 2.1718 | 1.0787 | 2.4427 | 2.5107 | 2.5268 | 3.0674 | | 1.7489 | 2.7152 | H8 | 2.1684 | 1.0792 | 2.3844 | 2.5128 | 3.0698 | 2.5125 | 1.7489 | | 3.3439 | H9 | 3.0560 | 2.4788 | 1.3525 | 4.0438 | 2.7933 | 3.4102 | 2.7152 | 3.3439 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| C1 |
C2 |
S3 |
113.528 |
|
C1 |
C2 |
H7 |
111.556 |
| C1 |
C2 |
H8 |
111.255 |
|
C2 |
C1 |
H4 |
110.017 |
| C2 |
C1 |
H5 |
111.317 |
|
C2 |
C1 |
H6 |
110.971 |
| C2 |
S3 |
H9 |
98.654 |
|
S3 |
C2 |
H7 |
107.982 |
| S3 |
C2 |
H8 |
103.835 |
|
H4 |
C1 |
H5 |
107.928 |
| H4 |
C1 |
H6 |
108.383 |
|
H5 |
C1 |
H6 |
108.118 |
| H7 |
C2 |
H8 |
108.277 |
|
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at HF/LANL2DZ
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
-0.485 |
|
|
|
| 2 |
C |
-0.526 |
|
|
|
| 3 |
S |
-0.029 |
|
|
|
| 4 |
H |
0.179 |
|
|
|
| 5 |
H |
0.174 |
|
|
|
| 6 |
H |
0.195 |
|
|
|
| 7 |
H |
0.218 |
|
|
|
| 8 |
H |
0.225 |
|
|
|
| 9 |
H |
0.049 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
2.113 |
0.058 |
1.035 |
2.354 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-29.573 |
1.549 |
-1.336 |
| y |
1.549 |
-26.691 |
-1.558 |
| z |
-1.336 |
-1.558 |
-26.688 |
|
| Traceless |
| | x | y | z |
| x |
-2.884 |
1.549 |
-1.336 |
| y |
1.549 |
1.439 |
-1.558 |
| z |
-1.336 |
-1.558 |
1.444 |
|
| Polar |
| 3z2-r2 | 2.889 |
| x2-y2 | -2.882 |
| xy | 1.549 |
| xz | -1.336 |
| yz | -1.558 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
6.490 |
0.982 |
0.209 |
| y |
0.982 |
4.493 |
-0.774 |
| z |
0.209 |
-0.774 |
4.422 |
<r2> (average value of r
2) Å
2
| <r2> |
71.875 |
| (<r2>)1/2 |
8.478 |