Jump to
S1C2
Energy calculated at HF/cc-pVTZ
| hartrees |
Energy at 0K | -1193.812549 |
Energy at 298.15K | -1193.815060 |
HF Energy | -1193.812549 |
Nuclear repulsion energy | 196.492636 |
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/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 |
2832 |
2578 |
0.44 |
|
|
|
2 |
A |
975 |
887 |
0.01 |
|
|
|
3 |
A |
533 |
485 |
0.34 |
|
|
|
4 |
A |
311 |
283 |
24.39 |
|
|
|
5 |
A |
225 |
204 |
0.04 |
|
|
|
6 |
B |
2832 |
2577 |
1.20 |
|
|
|
7 |
B |
964 |
878 |
9.41 |
|
|
|
8 |
B |
554 |
504 |
11.70 |
|
|
|
9 |
B |
338 |
307 |
17.30 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 4781.4 cm
-1
Scaled (by 0.9101) Zero Point Vibrational Energy (zpe) 4351.5 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/cc-pVTZ
Point Group is C2
Cartesians (Å)
Atom |
x (Å) |
y (Å) |
z (Å) |
S1 |
0.000 |
0.000 |
0.843 |
S2 |
0.000 |
1.653 |
-0.385 |
S3 |
0.000 |
-1.653 |
-0.385 |
H4 |
-1.312 |
1.752 |
-0.590 |
H5 |
1.312 |
-1.752 |
-0.590 |
Atom - Atom Distances (Å)
|
S1 |
S2 |
S3 |
H4 |
H5 |
S1 | | 2.0593 | 2.0593 | 2.6162 | 2.6162 |
S2 | 2.0593 | | 3.3060 | 1.3313 | 3.6544 | S3 | 2.0593 | 3.3060 | | 3.6544 | 1.3313 | H4 | 2.6162 | 1.3313 | 3.6544 | | 4.3767 | H5 | 2.6162 | 3.6544 | 1.3313 | 4.3767 | |
More geometry information
Calculated Bond Angles
atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
S1 |
S2 |
H4 |
98.720 |
|
S1 |
S3 |
H5 |
98.720 |
S2 |
S1 |
S3 |
106.781 |
|
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at HF/cc-pVTZ
Charges (e)
Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
1 |
S |
-0.026 |
|
|
|
2 |
S |
-0.103 |
|
|
|
3 |
S |
-0.103 |
|
|
|
4 |
H |
0.116 |
|
|
|
5 |
H |
0.116 |
|
|
|
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 |
-0.619 |
0.619 |
CHELPG |
|
|
|
|
AIM |
|
|
|
|
ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
Primitive |
| x | y | z |
x |
-37.499 |
-3.923 |
0.000 |
y |
-3.923 |
-39.705 |
0.000 |
z |
0.000 |
0.000 |
-41.674 |
|
Traceless |
| x | y | z |
x |
3.190 |
-3.923 |
0.000 |
y |
-3.923 |
-0.119 |
0.000 |
z |
0.000 |
0.000 |
-3.072 |
|
Polar |
3z2-r2 | -6.144 |
x2-y2 | 2.206 |
xy | -3.923 |
xz | 0.000 |
yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
|
x |
y |
z |
x |
6.232 |
-0.585 |
0.000 |
y |
-0.585 |
11.230 |
0.000 |
z |
0.000 |
0.000 |
6.881 |
<r2> (average value of r
2) Å
2
<r2> |
138.580 |
(<r2>)1/2 |
11.772 |
Jump to
S1C1
Energy calculated at HF/cc-pVTZ
| hartrees |
Energy at 0K | -1193.812282 |
Energy at 298.15K | -1193.814804 |
HF Energy | -1193.812282 |
Nuclear repulsion energy | 196.518330 |
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/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' |
2827 |
2573 |
2.68 |
|
|
|
2 |
A' |
977 |
890 |
5.53 |
|
|
|
3 |
A' |
533 |
485 |
0.31 |
|
|
|
4 |
A' |
340 |
309 |
18.99 |
|
|
|
5 |
A' |
226 |
206 |
0.06 |
|
|
|
6 |
A" |
2829 |
2575 |
0.75 |
|
|
|
7 |
A" |
967 |
880 |
5.15 |
|
|
|
8 |
A" |
554 |
504 |
12.65 |
|
|
|
9 |
A" |
316 |
287 |
11.02 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 4784.9 cm
-1
Scaled (by 0.9101) Zero Point Vibrational Energy (zpe) 4354.7 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 HF/cc-pVTZ
Point Group is Cs
Cartesians (Å)
Atom |
x (Å) |
y (Å) |
z (Å) |
S1 |
-0.053 |
0.841 |
0.000 |
S2 |
-0.053 |
-0.388 |
1.652 |
S3 |
-0.053 |
-0.388 |
-1.652 |
H4 |
1.264 |
-0.526 |
1.798 |
H5 |
1.264 |
-0.526 |
-1.798 |
Atom - Atom Distances (Å)
|
S1 |
S2 |
S3 |
H4 |
H5 |
S1 | | 2.0588 | 2.0588 | 2.6144 | 2.6144 |
S2 | 2.0588 | | 3.3044 | 1.3317 | 3.6955 | S3 | 2.0588 | 3.3044 | | 3.6955 | 1.3317 | H4 | 2.6144 | 1.3317 | 3.6955 | | 3.5963 | H5 | 2.6144 | 3.6955 | 1.3317 | 3.5963 | |
More geometry information
Calculated Bond Angles
atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
S1 |
S2 |
H4 |
98.631 |
|
S1 |
S3 |
H5 |
98.631 |
S2 |
S1 |
S3 |
106.738 |
|
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at HF/cc-pVTZ
Charges (e)
Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
1 |
S |
-0.027 |
|
|
|
2 |
S |
-0.096 |
|
|
|
3 |
S |
-0.096 |
|
|
|
4 |
H |
0.110 |
|
|
|
5 |
H |
0.110 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
|
x |
y |
z |
Total |
|
1.815 |
-0.524 |
0.000 |
1.889 |
CHELPG |
|
|
|
|
AIM |
|
|
|
|
ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
Primitive |
| x | y | z |
x |
-37.694 |
-1.554 |
0.000 |
y |
-1.554 |
-41.836 |
0.000 |
z |
0.000 |
0.000 |
-39.421 |
|
Traceless |
| x | y | z |
x |
2.934 |
-1.554 |
0.000 |
y |
-1.554 |
-3.278 |
0.000 |
z |
0.000 |
0.000 |
0.344 |
|
Polar |
3z2-r2 | 0.688 |
x2-y2 | 4.142 |
xy | -1.554 |
xz | 0.000 |
yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
|
x |
y |
z |
x |
6.213 |
-0.298 |
0.000 |
y |
-0.298 |
6.845 |
0.000 |
z |
0.000 |
0.000 |
11.257 |
<r2> (average value of r
2) Å
2
<r2> |
138.583 |
(<r2>)1/2 |
11.772 |