Jump to
S1C2
Energy calculated at HF/daug-cc-pVTZ
| hartrees |
Energy at 0K | -1193.814660 |
Energy at 298.15K | -1193.817146 |
HF Energy | -1193.814660 |
Nuclear repulsion energy | 196.479929 |
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/daug-cc-pVTZ
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 |
2833 |
2562 |
0.37 |
|
|
|
2 |
A |
974 |
881 |
0.01 |
|
|
|
3 |
A |
532 |
482 |
0.30 |
|
|
|
4 |
A |
308 |
278 |
22.39 |
|
|
|
5 |
A |
224 |
203 |
0.05 |
|
|
|
6 |
B |
2832 |
2562 |
0.31 |
|
|
|
7 |
B |
964 |
872 |
11.15 |
|
|
|
8 |
B |
553 |
501 |
11.30 |
|
|
|
9 |
B |
333 |
301 |
16.06 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 4776.2 cm
-1
Scaled (by 0.9046) Zero Point Vibrational Energy (zpe) 4320.5 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 HF/daug-cc-pVTZ
Point Group is C2
Cartesians (Å)
Atom |
x (Å) |
y (Å) |
z (Å) |
S1 |
0.000 |
0.000 |
0.842 |
S2 |
0.000 |
1.654 |
-0.385 |
S3 |
0.000 |
-1.654 |
-0.385 |
H4 |
-1.312 |
1.757 |
-0.584 |
H5 |
1.312 |
-1.757 |
-0.584 |
Atom - Atom Distances (Å)
|
S1 |
S2 |
S3 |
H4 |
H5 |
S1 | | 2.0591 | 2.0591 | 2.6159 | 2.6159 |
S2 | 2.0591 | | 3.3074 | 1.3312 | 3.6599 | S3 | 2.0591 | 3.3074 | | 3.6599 | 1.3312 | H4 | 2.6159 | 1.3312 | 3.6599 | | 4.3860 | H5 | 2.6159 | 3.6599 | 1.3312 | 4.3860 | |
More geometry information
Calculated Bond Angles
atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
S1 |
S2 |
H4 |
98.714 |
|
S1 |
S3 |
H5 |
98.714 |
S2 |
S1 |
S3 |
106.853 |
|
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at HF/daug-cc-pVTZ
Charges (e)
Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
1 |
S |
-0.032 |
|
|
|
2 |
S |
-0.315 |
|
|
|
3 |
S |
-0.315 |
|
|
|
4 |
H |
0.331 |
|
|
|
5 |
H |
0.331 |
|
|
|
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 |
-0.594 |
0.594 |
CHELPG |
|
|
|
|
AIM |
|
|
|
|
ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
Primitive |
| x | y | z |
x |
-37.603 |
-3.842 |
0.000 |
y |
-3.842 |
-39.950 |
0.000 |
z |
0.000 |
0.000 |
-41.905 |
|
Traceless |
| x | y | z |
x |
3.325 |
-3.842 |
0.000 |
y |
-3.842 |
-0.196 |
0.000 |
z |
0.000 |
0.000 |
-3.129 |
|
Polar |
3z2-r2 | -6.257 |
x2-y2 | 2.347 |
xy | -3.842 |
xz | 0.000 |
yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
|
x |
y |
z |
x |
7.438 |
-0.552 |
0.000 |
y |
-0.552 |
12.636 |
0.000 |
z |
0.000 |
0.000 |
8.451 |
<r2> (average value of r
2) Å
2
<r2> |
138.766 |
(<r2>)1/2 |
11.780 |
Jump to
S1C1
Energy calculated at HF/daug-cc-pVTZ
| hartrees |
Energy at 0K | -1193.814497 |
Energy at 298.15K | -1193.816998 |
HF Energy | -1193.814497 |
Nuclear repulsion energy | 196.515704 |
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/daug-cc-pVTZ
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' |
2829 |
2559 |
1.00 |
|
|
|
2 |
A' |
976 |
883 |
6.26 |
|
|
|
3 |
A' |
532 |
481 |
0.30 |
|
|
|
4 |
A' |
335 |
303 |
17.44 |
|
|
|
5 |
A' |
226 |
204 |
0.06 |
|
|
|
6 |
A" |
2831 |
2561 |
0.36 |
|
|
|
7 |
A" |
966 |
874 |
5.78 |
|
|
|
8 |
A" |
554 |
501 |
12.03 |
|
|
|
9 |
A" |
315 |
285 |
10.41 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 4781.8 cm
-1
Scaled (by 0.9046) Zero Point Vibrational Energy (zpe) 4325.6 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/daug-cc-pVTZ
Point Group is Cs
Cartesians (Å)
Atom |
x (Å) |
y (Å) |
z (Å) |
S1 |
-0.053 |
0.840 |
0.000 |
S2 |
-0.053 |
-0.387 |
1.653 |
S3 |
-0.053 |
-0.387 |
-1.653 |
H4 |
1.263 |
-0.524 |
1.801 |
H5 |
1.263 |
-0.524 |
-1.801 |
Atom - Atom Distances (Å)
|
S1 |
S2 |
S3 |
H4 |
H5 |
S1 | | 2.0586 | 2.0586 | 2.6148 | 2.6148 |
S2 | 2.0586 | | 3.3057 | 1.3314 | 3.6990 | S3 | 2.0586 | 3.3057 | | 3.6990 | 1.3314 | H4 | 2.6148 | 1.3314 | 3.6990 | | 3.6030 | H5 | 2.6148 | 3.6990 | 1.3314 | 3.6030 | |
More geometry information
Calculated Bond Angles
atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
S1 |
S2 |
H4 |
98.679 |
|
S1 |
S3 |
H5 |
98.679 |
S2 |
S1 |
S3 |
106.819 |
|
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at HF/daug-cc-pVTZ
Charges (e)
Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
1 |
S |
-0.017 |
|
|
|
2 |
S |
-0.307 |
|
|
|
3 |
S |
-0.307 |
|
|
|
4 |
H |
0.315 |
|
|
|
5 |
H |
0.315 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
|
x |
y |
z |
Total |
|
1.745 |
-0.508 |
0.000 |
1.817 |
CHELPG |
|
|
|
|
AIM |
|
|
|
|
ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
Primitive |
| x | y | z |
x |
-37.793 |
-1.543 |
0.000 |
y |
-1.543 |
-42.055 |
0.000 |
z |
0.000 |
0.000 |
-39.686 |
|
Traceless |
| x | y | z |
x |
3.078 |
-1.543 |
0.000 |
y |
-1.543 |
-3.316 |
0.000 |
z |
0.000 |
0.000 |
0.238 |
|
Polar |
3z2-r2 | 0.476 |
x2-y2 | 4.263 |
xy | -1.543 |
xz | 0.000 |
yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
|
x |
y |
z |
x |
7.412 |
-0.220 |
0.000 |
y |
-0.220 |
8.425 |
0.000 |
z |
0.000 |
0.000 |
12.652 |
<r2> (average value of r
2) Å
2
<r2> |
138.757 |
(<r2>)1/2 |
11.780 |