Jump to
S2C1
S3C1
Energy calculated at B3LYP/6-31G*
| | hartrees |
| Energy at 0K | -38.479163 |
| Energy at 298.15K | |
| HF Energy | -38.479163 |
| Nuclear repulsion energy | 2.802156 |
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 B3LYP/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 B3LYP/6-31G*
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
-0.122 |
|
|
|
| 2 |
H |
0.122 |
|
|
|
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 |
-1.384 |
1.384 |
| CHELPG |
0.000 |
0.000 |
-1.224 |
1.224 |
| AIM |
0.000 |
0.000 |
-0.509 |
0.509 |
| ESP |
0.000 |
0.000 |
-1.266 |
1.266 |
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-7.283 |
0.000 |
0.000 |
| y |
0.000 |
-5.410 |
0.000 |
| z |
0.000 |
0.000 |
-7.463 |
|
| Traceless |
| | x | y | z |
| x |
-0.847 |
0.000 |
0.000 |
| y |
0.000 |
1.963 |
0.000 |
| z |
0.000 |
0.000 |
-1.116 |
|
| Polar |
| 3z2-r2 | -2.232 |
| x2-y2 | -1.873 |
| 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 |
1.022 |
0.000 |
0.000 |
| y |
0.000 |
1.234 |
0.000 |
| z |
0.000 |
0.000 |
1.894 |
<r2> (average value of r
2) Å
2
| <r2> |
5.297 |
| (<r2>)1/2 |
2.301 |
Jump to
S1C1
S3C1
Energy calculated at B3LYP/6-31G*
| | hartrees |
| Energy at 0K | -38.479163 |
| Energy at 298.15K | |
| HF Energy | -38.479163 |
| Nuclear repulsion energy | 2.802156 |
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 B3LYP/6-31G*
Geometric Data calculated at B3LYP/6-31G*
Point Group is C∞v
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Jump to
S1C1
S2C1
Energy calculated at B3LYP/6-31G*
| | hartrees |
| Energy at 0K | -38.446615 |
| Energy at 298.15K | -38.445264 |
| HF Energy | -38.446615 |
| Nuclear repulsion energy | 2.900025 |
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 B3LYP/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 |
-0.938 |
Atom - Atom Distances (Å)
More geometry information
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at B3LYP/6-31G*
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
-0.220 |
|
|
|
| 2 |
H |
0.220 |
|
|
|
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 |
-0.735 |
0.735 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-7.048 |
0.000 |
0.000 |
| y |
0.000 |
-7.048 |
0.000 |
| z |
0.000 |
0.000 |
-5.202 |
|
| Traceless |
| | x | y | z |
| x |
-0.923 |
0.000 |
0.000 |
| y |
0.000 |
-0.923 |
0.000 |
| z |
0.000 |
0.000 |
1.846 |
|
| Polar |
| 3z2-r2 | 3.691 |
| 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 |
0.665 |
0.000 |
0.000 |
| y |
0.000 |
0.665 |
0.000 |
| z |
0.000 |
0.000 |
1.381 |
<r2> (average value of r
2) Å
2
| <r2> |
5.045 |
| (<r2>)1/2 |
2.246 |