Jump to
S2C1
Energy calculated at B1B95/STO-3G
| | hartrees |
| Energy at 0K | -149.212863 |
| Energy at 298.15K | -149.210816 |
| HF Energy | -149.212863 |
| Nuclear repulsion energy | 44.242719 |
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/STO-3G
Point Group is C∞v
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
0.000 |
0.000 |
-1.453 |
| C2 |
0.000 |
0.000 |
-0.082 |
| O3 |
0.000 |
0.000 |
1.151 |
Atom - Atom Distances (Å)
| |
C1 |
C2 |
O3 |
| C1 | | 1.3718 | 2.6046 |
C2 | 1.3718 | | 1.2328 | O3 | 2.6046 | 1.2328 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| C1 |
C2 |
O3 |
180.000 |
|
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at B1B95/STO-3G
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
-0.021 |
|
|
|
| 2 |
C |
0.070 |
|
|
|
| 3 |
O |
-0.050 |
|
|
|
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 |
1.236 |
1.236 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-13.780 |
0.000 |
0.000 |
| y |
0.000 |
-13.780 |
0.000 |
| z |
0.000 |
0.000 |
-19.123 |
|
| Traceless |
| | x | y | z |
| x |
2.672 |
0.000 |
0.000 |
| y |
0.000 |
2.672 |
0.000 |
| z |
0.000 |
0.000 |
-5.343 |
|
| Polar |
| 3z2-r2 | -10.686 |
| 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 |
0.908 |
0.000 |
0.000 |
| y |
0.000 |
0.908 |
0.000 |
| z |
0.000 |
0.000 |
3.291 |
<r2> (average value of r
2) Å
2
| <r2> |
33.036 |
| (<r2>)1/2 |
5.748 |
Jump to
S1C1
Energy calculated at B1B95/STO-3G
| | hartrees |
| Energy at 0K | -149.166645 |
| Energy at 298.15K | -149.164745 |
| HF Energy | -149.166645 |
| Nuclear repulsion energy | 44.180353 |
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/STO-3G
Point Group is C∞v
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
0.000 |
0.000 |
-1.455 |
| C2 |
0.000 |
0.000 |
-0.082 |
| O3 |
0.000 |
0.000 |
1.153 |
Atom - Atom Distances (Å)
| |
C1 |
C2 |
O3 |
| C1 | | 1.3730 | 2.6081 |
C2 | 1.3730 | | 1.2350 | O3 | 2.6081 | 1.2350 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| C1 |
C2 |
O3 |
180.000 |
|
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at B1B95/STO-3G
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
0.002 |
|
|
|
| 2 |
C |
0.064 |
|
|
|
| 3 |
O |
-0.066 |
|
|
|
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 |
0.925 |
0.925 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-12.558 |
0.000 |
0.000 |
| y |
0.000 |
-14.971 |
0.000 |
| z |
0.000 |
0.000 |
-18.970 |
|
| Traceless |
| | x | y | z |
| x |
4.413 |
0.000 |
0.000 |
| y |
0.000 |
0.793 |
0.000 |
| z |
0.000 |
0.000 |
-5.206 |
|
| Polar |
| 3z2-r2 | -10.412 |
| x2-y2 | 2.413 |
| 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 |
1.029 |
0.000 |
0.000 |
| y |
0.000 |
0.579 |
0.000 |
| z |
0.000 |
0.000 |
3.171 |
<r2> (average value of r
2) Å
2
| <r2> |
33.060 |
| (<r2>)1/2 |
5.750 |