Jump to
S2C1
S3C1
Energy calculated at HF/6-31G(2df,p)
| | hartrees |
| Energy at 0K | -38.271345 |
| Energy at 298.15K | |
| HF Energy | -38.271345 |
| Nuclear repulsion energy | 2.859770 |
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 HF/6-31G(2df,p)
Point Group is C∞v
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
0.000 |
0.000 |
0.159 |
| H2 |
0.000 |
0.000 |
-0.952 |
Atom - Atom Distances (Å)
More geometry information
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at HF/6-31G(2df,p)
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
-0.155 |
|
|
|
| 2 |
H |
0.155 |
|
|
|
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 |
-1.523 |
1.523 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-5.432 |
0.000 |
0.000 |
| y |
0.000 |
-7.365 |
0.000 |
| z |
0.000 |
0.000 |
-7.456 |
|
| Traceless |
| | x | y | z |
| x |
1.978 |
0.000 |
0.000 |
| y |
0.000 |
-0.921 |
0.000 |
| z |
0.000 |
0.000 |
-1.058 |
|
| Polar |
| 3z2-r2 | -2.116 |
| x2-y2 | 1.933 |
| 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 |
1.208 |
0.000 |
0.000 |
| y |
0.000 |
1.260 |
0.000 |
| z |
0.000 |
0.000 |
1.781 |
<r2> (average value of r
2) Å
2
| <r2> |
5.273 |
| (<r2>)1/2 |
2.296 |
Jump to
S1C1
S3C1
Energy calculated at HF/6-31G(2df,p)
| | hartrees |
| Energy at 0K | -38.271345 |
| Energy at 298.15K | |
| HF Energy | -38.271345 |
| Nuclear repulsion energy | 2.859770 |
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 HF/6-31G(2df,p)
Geometric Data calculated at HF/6-31G(2df,p)
Point Group is C∞v
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Jump to
S1C1
S2C1
Energy calculated at HF/6-31G(2df,p)
| | hartrees |
| Energy at 0K | -38.279733 |
| Energy at 298.15K | -38.278381 |
| HF Energy | -38.279733 |
| Nuclear repulsion energy | 2.961566 |
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 HF/6-31G(2df,p)
Point Group is C∞v
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
0.000 |
0.000 |
0.153 |
| H2 |
0.000 |
0.000 |
-0.919 |
Atom - Atom Distances (Å)
More geometry information
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at HF/6-31G(2df,p)
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
-0.217 |
|
|
|
| 2 |
H |
0.217 |
|
|
|
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 |
-0.546 |
0.546 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-7.004 |
0.000 |
0.000 |
| y |
0.000 |
-7.004 |
0.000 |
| z |
0.000 |
0.000 |
-5.318 |
|
| Traceless |
| | x | y | z |
| x |
-0.843 |
0.000 |
0.000 |
| y |
0.000 |
-0.843 |
0.000 |
| z |
0.000 |
0.000 |
1.686 |
|
| Polar |
| 3z2-r2 | 3.372 |
| 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 |
0.889 |
0.000 |
0.000 |
| y |
0.000 |
0.889 |
0.000 |
| z |
0.000 |
0.000 |
1.356 |
<r2> (average value of r
2) Å
2
| <r2> |
5.009 |
| (<r2>)1/2 |
2.238 |