Jump to
S1C2
Energy calculated at HF/LANL2DZ
| | hartrees |
| Energy at 0K | -29.542304 |
| Energy at 298.15K | -29.542503 |
| HF Energy | -29.542304 |
| Nuclear repulsion energy | 23.856732 |
The energy at 298.15K was derived from the energy at 0K
and an integrated heat capacity that used the calculated vibrational frequencies.
Geometric Data calculated at HF/LANL2DZ
Point Group is C2v
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| S1 |
0.000 |
0.000 |
0.745 |
| S2 |
0.000 |
1.744 |
-0.373 |
| S3 |
0.000 |
-1.744 |
-0.373 |
Atom - Atom Distances (Å)
| |
S1 |
S2 |
S3 |
| S1 | | 2.0714 | 2.0714 |
S2 | 2.0714 | | 3.4874 | S3 | 2.0714 | 3.4874 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| S2 |
S1 |
S3 |
114.663 |
|
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at HF/LANL2DZ
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
S |
0.140 |
|
|
|
| 2 |
S |
-0.070 |
|
|
|
| 3 |
S |
-0.070 |
|
|
|
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 |
0.639 |
0.639 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-36.766 |
0.000 |
0.000 |
| y |
0.000 |
-41.227 |
0.000 |
| z |
0.000 |
0.000 |
-39.868 |
|
| Traceless |
| | x | y | z |
| x |
3.782 |
0.000 |
0.000 |
| y |
0.000 |
-2.910 |
0.000 |
| z |
0.000 |
0.000 |
-0.871 |
|
| Polar |
| 3z2-r2 | -1.743 |
| x2-y2 | 4.461 |
| xy | 0.000 |
| xz | 0.000 |
| yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
1.394 |
0.000 |
0.000 |
| y |
0.000 |
19.461 |
0.000 |
| z |
0.000 |
0.000 |
3.865 |
<r2> (average value of r
2) Å
2
| <r2> |
66.024 |
| (<r2>)1/2 |
8.126 |
Jump to
S1C1
Energy calculated at HF/LANL2DZ
| | hartrees |
| Energy at 0K | -29.561277 |
| Energy at 298.15K | -29.561525 |
| HF Energy | -29.561277 |
| Nuclear repulsion energy | 24.865127 |
The energy at 298.15K was derived from the energy at 0K
and an integrated heat capacity that used the calculated vibrational frequencies.
Geometric Data calculated at HF/LANL2DZ
Point Group is D3h
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| S1 |
0.000 |
1.327 |
0.000 |
| S2 |
1.149 |
-0.664 |
0.000 |
| S3 |
-1.149 |
-0.664 |
0.000 |
Atom - Atom Distances (Å)
| |
S1 |
S2 |
S3 |
| S1 | | 2.2984 | 2.2984 |
S2 | 2.2984 | | 2.2984 | S3 | 2.2984 | 2.2984 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| S2 |
S1 |
S3 |
60.000 |
|
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at HF/LANL2DZ
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
S |
0.000 |
|
|
|
| 2 |
S |
0.000 |
|
|
|
| 3 |
S |
0.000 |
|
|
|
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 |
0.000 |
0.000 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-36.869 |
0.000 |
0.000 |
| y |
0.000 |
-36.869 |
0.000 |
| z |
0.000 |
0.000 |
-41.555 |
|
| Traceless |
| | x | y | z |
| x |
2.343 |
0.000 |
0.000 |
| y |
0.000 |
2.343 |
0.000 |
| z |
0.000 |
0.000 |
-4.686 |
|
| Polar |
| 3z2-r2 | -9.372 |
| x2-y2 | 0.000 |
| xy | 0.000 |
| xz | 0.000 |
| yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
10.100 |
0.000 |
0.000 |
| y |
0.000 |
10.100 |
0.000 |
| z |
0.000 |
0.000 |
0.241 |
<r2> (average value of r
2) Å
2
| <r2> |
55.700 |
| (<r2>)1/2 |
7.463 |