Jump to
S2C1
S3C1
Energy calculated at B3LYP/cc-pVTZ
| | hartrees |
| Energy at 0K | -38.496253 |
| Energy at 298.15K | |
| HF Energy | -38.496253 |
| Nuclear repulsion energy | 2.825860 |
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/cc-pVTZ
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 |
-0.963 |
Atom - Atom Distances (Å)
More geometry information
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at B3LYP/cc-pVTZ
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
-0.103 |
|
|
|
| 2 |
H |
0.103 |
|
|
|
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 |
-1.475 |
1.475 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
0.000 |
0.000 |
-1.344 |
1.344 |
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-7.671 |
0.000 |
0.000 |
| y |
0.000 |
-5.659 |
0.000 |
| z |
0.000 |
0.000 |
-7.689 |
|
| Traceless |
| | x | y | z |
| x |
-0.998 |
0.000 |
0.000 |
| y |
0.000 |
2.021 |
0.000 |
| z |
0.000 |
0.000 |
-1.024 |
|
| Polar |
| 3z2-r2 | -2.047 |
| x2-y2 | -2.013 |
| 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 |
1.526 |
0.000 |
0.000 |
| y |
0.000 |
1.510 |
0.000 |
| z |
0.000 |
0.000 |
2.196 |
<r2> (average value of r
2) Å
2
| <r2> |
5.458 |
| (<r2>)1/2 |
2.336 |
Jump to
S1C1
S3C1
Energy calculated at B3LYP/cc-pVTZ
| | hartrees |
| Energy at 0K | -38.496253 |
| Energy at 298.15K | |
| HF Energy | -38.496253 |
| Nuclear repulsion energy | 2.825860 |
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/cc-pVTZ
Geometric Data calculated at B3LYP/cc-pVTZ
Point Group is C∞v
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Jump to
S1C1
S2C1
Energy calculated at B3LYP/cc-pVTZ
| | hartrees |
| Energy at 0K | -38.462988 |
| Energy at 298.15K | -38.461636 |
| HF Energy | -38.462988 |
| Nuclear repulsion energy | 2.904511 |
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/cc-pVTZ
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 |
-0.937 |
Atom - Atom Distances (Å)
More geometry information
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at B3LYP/cc-pVTZ
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
-0.195 |
|
|
|
| 2 |
H |
0.195 |
|
|
|
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 |
-0.716 |
0.716 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-7.412 |
0.000 |
0.000 |
| y |
0.000 |
-7.412 |
0.000 |
| z |
0.000 |
0.000 |
-5.433 |
|
| Traceless |
| | x | y | z |
| x |
-0.990 |
0.000 |
0.000 |
| y |
0.000 |
-0.990 |
0.000 |
| z |
0.000 |
0.000 |
1.979 |
|
| Polar |
| 3z2-r2 | 3.958 |
| 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 |
1.243 |
0.000 |
0.000 |
| y |
0.000 |
1.243 |
0.000 |
| z |
0.000 |
0.000 |
1.683 |
<r2> (average value of r
2) Å
2
| <r2> |
5.242 |
| (<r2>)1/2 |
2.289 |