Jump to
S2C1
Energy calculated at TPSSh/6-31G(2df,p)
| | hartrees |
| Energy at 0K | -796.376980 |
| Energy at 298.15K | -796.376906 |
| HF Energy | -796.376980 |
| Nuclear repulsion energy | 71.085848 |
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 TPSSh/6-31G(2df,p)
Point Group is D∞h
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| S1 |
0.000 |
0.000 |
0.953 |
| S2 |
0.000 |
0.000 |
-0.953 |
Atom - Atom Distances (Å)
More geometry information
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at TPSSh/6-31G(2df,p)
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
S |
0.000 |
|
|
|
| 2 |
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
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
3.190 |
0.000 |
0.000 |
| y |
0.000 |
3.190 |
0.000 |
| z |
0.000 |
0.000 |
7.829 |
<r2> (average value of r
2) Å
2
| <r2> |
44.655 |
| (<r2>)1/2 |
6.682 |
Jump to
S1C1
Energy calculated at TPSSh/6-31G(2df,p)
| | hartrees |
| Energy at 0K | -796.338179 |
| Energy at 298.15K | -796.338100 |
| HF Energy | -796.338179 |
| Nuclear repulsion energy | 70.958895 |
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 TPSSh/6-31G(2df,p)
Point Group is D∞h
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| S1 |
0.000 |
0.000 |
0.949 |
| S2 |
0.000 |
0.000 |
-0.949 |
Atom - Atom Distances (Å)
More geometry information
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability