Jump to
S2C1
S3C1
S4C1
Energy calculated at B97D3/6-311+G(3df,2p)
| | hartrees |
| Energy at 0K | -150.304578 |
| Energy at 298.15K | -150.304573 |
| HF Energy | -150.304578 |
| Nuclear repulsion energy | 27.914672 |
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 B97D3/6-311+G(3df,2p)
Point Group is D∞h
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| O1 |
0.000 |
0.000 |
0.607 |
| O2 |
0.000 |
0.000 |
-0.607 |
Atom - Atom Distances (Å)
More geometry information
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at B97D3/6-311+G(3df,2p)
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
O |
0.000 |
|
|
|
| 2 |
O |
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 |
-10.070 |
0.000 |
0.000 |
| y |
0.000 |
-10.070 |
0.000 |
| z |
0.000 |
0.000 |
-10.415 |
|
| Traceless |
| | x | y | z |
| x |
0.172 |
0.000 |
0.000 |
| y |
0.000 |
0.172 |
0.000 |
| z |
0.000 |
0.000 |
-0.345 |
|
| Polar |
| 3z2-r2 | -0.690 |
| 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 |
1.146 |
0.000 |
0.000 |
| y |
0.000 |
1.146 |
0.000 |
| z |
0.000 |
0.000 |
2.245 |
<r2> (average value of r
2) Å
2
| <r2> |
12.249 |
| (<r2>)1/2 |
3.500 |
Jump to
S1C1
S3C1
S4C1
Energy calculated at B97D3/6-311+G(3df,2p)
| | hartrees |
| Energy at 0K | -150.241022 |
| Energy at 298.15K | -150.241017 |
| HF Energy | -150.241022 |
| Nuclear repulsion energy | 27.923237 |
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 B97D3/6-311+G(3df,2p)
Point Group is D∞h
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| O1 |
0.000 |
0.000 |
0.606 |
| O2 |
0.000 |
0.000 |
-0.606 |
Atom - Atom Distances (Å)
More geometry information
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at B97D3/6-311+G(3df,2p)
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
O |
0.000 |
|
|
|
| 2 |
O |
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 |
-11.059 |
-0.351 |
0.000 |
| y |
-0.351 |
-9.250 |
0.000 |
| z |
0.000 |
0.000 |
-10.575 |
|
| Traceless |
| | x | y | z |
| x |
-1.146 |
-0.351 |
0.000 |
| y |
-0.351 |
1.567 |
0.000 |
| z |
0.000 |
0.000 |
-0.420 |
|
| Polar |
| 3z2-r2 | -0.840 |
| x2-y2 | -1.809 |
| xy | -0.351 |
| xz | 0.000 |
| yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
1.146 |
0.000 |
0.000 |
| y |
0.000 |
1.146 |
0.000 |
| z |
0.000 |
0.000 |
2.245 |
<r2> (average value of r
2) Å
2
| <r2> |
12.314 |
| (<r2>)1/2 |
3.509 |
Jump to
S1C1
S2C1
S4C1
Energy calculated at B97D3/6-311+G(3df,2p)
| | hartrees |
| Energy at 0K | -150.241022 |
| Energy at 298.15K | -150.241017 |
| HF Energy | -150.241022 |
| Nuclear repulsion energy | 27.923237 |
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 B97D3/6-311+G(3df,2p)
Geometric Data calculated at B97D3/6-311+G(3df,2p)
Point Group is D∞h
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Jump to
S1C1
S2C1
S3C1
Energy calculated at B97D3/6-311+G(3df,2p)
| | hartrees |
| Energy at 0K | -150.241022 |
| Energy at 298.15K | -150.241017 |
| HF Energy | -150.241022 |
| Nuclear repulsion energy | 27.923597 |
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 B97D3/6-311+G(3df,2p)
Point Group is D∞h
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| O1 |
0.000 |
0.000 |
0.606 |
| O2 |
0.000 |
0.000 |
-0.606 |
Atom - Atom Distances (Å)
More geometry information
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at B97D3/6-311+G(3df,2p)
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
O |
0.000 |
|
|
|
| 2 |
O |
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 |
-10.677 |
-0.817 |
0.000 |
| y |
-0.817 |
-9.632 |
0.000 |
| z |
0.000 |
0.000 |
-10.575 |
|
| Traceless |
| | x | y | z |
| x |
-0.574 |
-0.817 |
0.000 |
| y |
-0.817 |
0.994 |
0.000 |
| z |
0.000 |
0.000 |
-0.420 |
|
| Polar |
| 3z2-r2 | -0.841 |
| x2-y2 | -1.046 |
| xy | -0.817 |
| xz | 0.000 |
| yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
1.146 |
0.000 |
0.000 |
| y |
0.000 |
1.146 |
0.000 |
| z |
0.000 |
0.000 |
2.245 |
<r2> (average value of r
2) Å
2
| <r2> |
12.314 |
| (<r2>)1/2 |
3.509 |