Jump to
S1C2
Energy calculated at B1B95/6-311G**
| | hartrees |
| Energy at 0K | -1194.709487 |
| Energy at 298.15K | -1194.709915 |
| HF Energy | -1194.709487 |
| Nuclear repulsion energy | 181.815389 |
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 B1B95/6-311G**
Point Group is C2v
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| S1 |
0.000 |
0.000 |
0.662 |
| S2 |
0.000 |
1.649 |
-0.331 |
| S3 |
0.000 |
-1.649 |
-0.331 |
Atom - Atom Distances (Å)
| |
S1 |
S2 |
S3 |
| S1 | | 1.9250 | 1.9250 |
S2 | 1.9250 | | 3.2986 | S3 | 1.9250 | 3.2986 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| S2 |
S1 |
S3 |
117.910 |
|
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at B1B95/6-311G**
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
S |
0.251 |
|
|
|
| 2 |
S |
-0.126 |
|
|
|
| 3 |
S |
-0.126 |
|
|
|
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 |
0.687 |
0.687 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-37.564 |
0.000 |
0.000 |
| y |
0.000 |
-41.214 |
0.000 |
| z |
0.000 |
0.000 |
-39.990 |
|
| Traceless |
| | x | y | z |
| x |
3.038 |
0.000 |
0.000 |
| y |
0.000 |
-2.437 |
0.000 |
| z |
0.000 |
0.000 |
-0.601 |
|
| Polar |
| 3z2-r2 | -1.202 |
| x2-y2 | 3.650 |
| 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 |
3.382 |
0.000 |
0.000 |
| y |
0.000 |
15.274 |
0.000 |
| z |
0.000 |
0.000 |
5.283 |
<r2> (average value of r
2) Å
2
| <r2> |
122.284 |
| (<r2>)1/2 |
11.058 |
Jump to
S1C1
Energy calculated at B1B95/6-311G**
| | hartrees |
| Energy at 0K | -1194.704061 |
| Energy at 298.15K | -1194.704579 |
| HF Energy | -1194.704061 |
| Nuclear repulsion energy | 194.639318 |
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 B1B95/6-311G**
Point Group is D3h
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| S1 |
0.000 |
1.206 |
0.000 |
| S2 |
1.044 |
-0.603 |
0.000 |
| S3 |
-1.044 |
-0.603 |
0.000 |
Atom - Atom Distances (Å)
| |
S1 |
S2 |
S3 |
| S1 | | 2.0880 | 2.0880 |
S2 | 2.0880 | | 2.0880 | S3 | 2.0880 | 2.0880 | |
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 B1B95/6-311G**
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 |
-36.237 |
0.000 |
0.000 |
| y |
0.000 |
-36.237 |
0.000 |
| z |
0.000 |
0.000 |
-42.643 |
|
| Traceless |
| | x | y | z |
| x |
3.203 |
0.000 |
0.000 |
| y |
0.000 |
3.203 |
0.000 |
| z |
0.000 |
0.000 |
-6.407 |
|
| Polar |
| 3z2-r2 | -12.813 |
| 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 |
7.764 |
0.000 |
0.000 |
| y |
0.000 |
7.763 |
0.000 |
| z |
0.000 |
0.000 |
3.470 |
<r2> (average value of r
2) Å
2
| <r2> |
93.723 |
| (<r2>)1/2 |
9.681 |