Jump to
S2C1
S3C1
Energy calculated at B3PW91/6-31G*
| | hartrees |
| Energy at 0K | -38.457862 |
| Energy at 298.15K | |
| HF Energy | -38.457862 |
| Nuclear repulsion energy | 2.802270 |
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 B3PW91/6-31G*
Point Group is C∞v
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
0.000 |
0.000 |
0.162 |
| H2 |
0.000 |
0.000 |
-0.971 |
Atom - Atom Distances (Å)
More geometry information
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at B3PW91/6-31G*
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
-0.131 |
|
|
|
| 2 |
H |
0.131 |
|
|
|
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 |
-1.416 |
1.416 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
0.000 |
0.000 |
-1.298 |
1.298 |
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-7.293 |
0.000 |
0.000 |
| y |
0.000 |
-5.418 |
0.000 |
| z |
0.000 |
0.000 |
-7.448 |
|
| Traceless |
| | x | y | z |
| x |
-0.860 |
0.000 |
0.000 |
| y |
0.000 |
1.952 |
0.000 |
| z |
0.000 |
0.000 |
-1.092 |
|
| Polar |
| 3z2-r2 | -2.184 |
| x2-y2 | -1.875 |
| 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 |
1.046 |
0.000 |
0.000 |
| y |
0.000 |
1.037 |
0.000 |
| z |
0.000 |
0.000 |
1.911 |
<r2> (average value of r
2) Å
2
| <r2> |
5.298 |
| (<r2>)1/2 |
2.302 |
Jump to
S1C1
S3C1
Energy calculated at B3PW91/6-31G*
| | hartrees |
| Energy at 0K | -38.457862 |
| Energy at 298.15K | |
| HF Energy | -38.457862 |
| Nuclear repulsion energy | 2.802270 |
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 B3PW91/6-31G*
Geometric Data calculated at B3PW91/6-31G*
Point Group is C∞v
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Jump to
S1C1
S2C1
Energy calculated at B3PW91/6-31G*
| | hartrees |
| Energy at 0K | -38.438175 |
| Energy at 298.15K | -38.436824 |
| HF Energy | -38.438175 |
| Nuclear repulsion energy | 2.913649 |
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 B3PW91/6-31G*
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 B3PW91/6-31G*
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
-0.230 |
|
|
|
| 2 |
H |
0.230 |
|
|
|
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 |
-0.703 |
0.703 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-7.038 |
0.000 |
0.000 |
| y |
0.000 |
-7.038 |
0.000 |
| z |
0.000 |
0.000 |
-5.207 |
|
| Traceless |
| | x | y | z |
| x |
-0.915 |
0.000 |
0.000 |
| y |
0.000 |
-0.915 |
0.000 |
| z |
0.000 |
0.000 |
1.831 |
|
| Polar |
| 3z2-r2 | 3.662 |
| 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 |
0.659 |
0.000 |
0.000 |
| y |
0.000 |
0.659 |
0.000 |
| z |
0.000 |
0.000 |
1.333 |
<r2> (average value of r
2) Å
2
| <r2> |
5.032 |
| (<r2>)1/2 |
2.243 |