Jump to
S2C1
S3C1
Energy calculated at B3PW91/6-311G*
| | hartrees |
| Energy at 0K | -38.467957 |
| Energy at 298.15K | |
| HF Energy | -38.467957 |
| Nuclear repulsion energy | 2.812326 |
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 B3PW91/6-311G*
Point Group is C∞v
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
0.000 |
0.000 |
0.161 |
| H2 |
0.000 |
0.000 |
-0.968 |
Atom - Atom Distances (Å)
More geometry information
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at B3PW91/6-311G*
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
-0.187 |
|
|
|
| 2 |
H |
0.187 |
|
|
|
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 |
-1.534 |
1.534 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-7.564 |
0.000 |
0.000 |
| y |
0.000 |
-5.568 |
0.000 |
| z |
0.000 |
0.000 |
-7.589 |
|
| Traceless |
| | x | y | z |
| x |
-0.986 |
0.000 |
0.000 |
| y |
0.000 |
2.009 |
0.000 |
| z |
0.000 |
0.000 |
-1.023 |
|
| Polar |
| 3z2-r2 | -2.045 |
| x2-y2 | -1.996 |
| 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 |
1.256 |
0.000 |
0.000 |
| y |
0.000 |
1.100 |
0.000 |
| z |
0.000 |
0.000 |
2.014 |
<r2> (average value of r
2) Å
2
| <r2> |
5.407 |
| (<r2>)1/2 |
2.325 |
Jump to
S1C1
S3C1
Energy calculated at B3PW91/6-311G*
| | hartrees |
| Energy at 0K | -38.467957 |
| Energy at 298.15K | |
| HF Energy | -38.467957 |
| Nuclear repulsion energy | 2.812326 |
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 B3PW91/6-311G*
Geometric Data calculated at B3PW91/6-311G*
Point Group is C∞v
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Jump to
S1C1
S2C1
Energy calculated at B3PW91/6-311G*
| | hartrees |
| Energy at 0K | -38.447364 |
| Energy at 298.15K | -38.446013 |
| HF Energy | -38.447364 |
| Nuclear repulsion energy | 2.913250 |
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 B3PW91/6-311G*
Point Group is C∞v
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
0.000 |
0.000 |
0.156 |
| H2 |
0.000 |
0.000 |
-0.934 |
Atom - Atom Distances (Å)
More geometry information
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at B3PW91/6-311G*
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
-0.281 |
|
|
|
| 2 |
H |
0.281 |
|
|
|
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 |
-0.738 |
0.738 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-7.319 |
0.000 |
0.000 |
| y |
0.000 |
-7.319 |
0.000 |
| z |
0.000 |
0.000 |
-5.329 |
|
| Traceless |
| | x | y | z |
| x |
-0.995 |
0.000 |
0.000 |
| y |
0.000 |
-0.995 |
0.000 |
| z |
0.000 |
0.000 |
1.991 |
|
| Polar |
| 3z2-r2 | 3.981 |
| 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 |
0.868 |
0.000 |
0.000 |
| y |
0.000 |
0.868 |
0.000 |
| z |
0.000 |
0.000 |
1.394 |
<r2> (average value of r
2) Å
2
| <r2> |
5.175 |
| (<r2>)1/2 |
2.275 |