Jump to
S1C2
Energy calculated at B1B95/6-31G*
| | hartrees |
| Energy at 0K | -113.993370 |
| Energy at 298.15K | |
| HF Energy | -113.993370 |
| Nuclear repulsion energy | 36.796356 |
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 B1B95/6-31G*
Point Group is D∞h
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
0.000 |
0.000 |
0.000 |
| C2 |
0.000 |
0.000 |
1.294 |
| C3 |
0.000 |
0.000 |
-1.294 |
Atom - Atom Distances (Å)
| |
C1 |
C2 |
C3 |
| C1 | | 1.2943 | 1.2943 |
C2 | 1.2943 | | 2.5886 | C3 | 1.2943 | 2.5886 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| C2 |
C1 |
C3 |
180.000 |
|
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at B1B95/6-31G*
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
-0.031 |
|
|
|
| 2 |
C |
0.016 |
|
|
|
| 3 |
C |
0.016 |
|
|
|
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 |
0.000 |
0.000 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-15.801 |
0.000 |
0.000 |
| y |
0.000 |
-15.801 |
0.000 |
| z |
0.000 |
0.000 |
-21.701 |
|
| Traceless |
| | x | y | z |
| x |
2.950 |
0.000 |
0.000 |
| y |
0.000 |
2.950 |
0.000 |
| z |
0.000 |
0.000 |
-5.900 |
|
| Polar |
| 3z2-r2 | -11.800 |
| 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 |
2.375 |
0.000 |
0.000 |
| y |
0.000 |
2.375 |
0.000 |
| z |
0.000 |
0.000 |
6.571 |
<r2> (average value of r
2) Å
2
| <r2> |
31.200 |
| (<r2>)1/2 |
5.586 |
Jump to
S1C1
Energy calculated at B1B95/6-31G*
| | hartrees |
| Energy at 0K | -113.993370 |
| Energy at 298.15K | |
| HF Energy | -113.993370 |
| Nuclear repulsion energy | 36.796981 |
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 B1B95/6-31G*
Point Group is C2v
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
0.000 |
0.000 |
-0.000 |
| C2 |
0.000 |
1.294 |
0.000 |
| C3 |
0.000 |
-1.294 |
0.000 |
Atom - Atom Distances (Å)
| |
C1 |
C2 |
C3 |
| C1 | | 1.2943 | 1.2943 |
C2 | 1.2943 | | 2.5886 | C3 | 1.2943 | 2.5886 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| C2 |
C1 |
C3 |
179.958 |
|
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at B1B95/6-31G*
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
-0.031 |
|
|
|
| 2 |
C |
0.016 |
|
|
|
| 3 |
C |
0.016 |
|
|
|
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 |
-0.001 |
0.001 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-15.801 |
0.000 |
0.000 |
| y |
0.000 |
-21.701 |
0.000 |
| z |
0.000 |
0.000 |
-15.801 |
|
| Traceless |
| | x | y | z |
| x |
2.950 |
0.000 |
0.000 |
| y |
0.000 |
-5.900 |
0.000 |
| z |
0.000 |
0.000 |
2.950 |
|
| Polar |
| 3z2-r2 | 5.900 |
| x2-y2 | 5.900 |
| 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 |
2.375 |
0.000 |
0.000 |
| y |
0.000 |
6.571 |
0.000 |
| z |
0.000 |
0.000 |
2.375 |
<r2> (average value of r
2) Å
2
| <r2> |
31.200 |
| (<r2>)1/2 |
5.586 |