Jump to
S2C1
Energy calculated at B3LYP/LANL2DZ
| | hartrees |
| Energy at 0K | -151.226936 |
| Energy at 298.15K | -151.225149 |
| HF Energy | -151.226936 |
| Nuclear repulsion energy | 44.705355 |
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/LANL2DZ
Point Group is C∞v
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
0.000 |
0.000 |
-1.450 |
| C2 |
0.000 |
0.000 |
-0.065 |
| O3 |
0.000 |
0.000 |
1.137 |
Atom - Atom Distances (Å)
| |
C1 |
C2 |
O3 |
| C1 | | 1.3849 | 2.5870 |
C2 | 1.3849 | | 1.2021 | O3 | 2.5870 | 1.2021 | |
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 B3LYP/LANL2DZ
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
-0.053 |
|
|
|
| 2 |
C |
0.102 |
|
|
|
| 3 |
O |
-0.049 |
|
|
|
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 |
1.112 |
1.112 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-15.873 |
0.000 |
0.000 |
| y |
0.000 |
-15.873 |
0.000 |
| z |
0.000 |
0.000 |
-23.236 |
|
| Traceless |
| | x | y | z |
| x |
3.681 |
0.000 |
0.000 |
| y |
0.000 |
3.681 |
0.000 |
| z |
0.000 |
0.000 |
-7.363 |
|
| Polar |
| 3z2-r2 | -14.726 |
| 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 |
2.127 |
0.000 |
0.000 |
| y |
0.000 |
2.127 |
0.000 |
| z |
0.000 |
0.000 |
5.722 |
<r2> (average value of r
2) Å
2
| <r2> |
34.428 |
| (<r2>)1/2 |
5.868 |
Jump to
S1C1
Energy calculated at B3LYP/LANL2DZ
| | hartrees |
| Energy at 0K | -151.189160 |
| Energy at 298.15K | -151.187481 |
| HF Energy | -151.189160 |
| Nuclear repulsion energy | 44.604324 |
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/LANL2DZ
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 |
-0.067 |
| O3 |
0.000 |
0.000 |
1.139 |
Atom - Atom Distances (Å)
| |
C1 |
C2 |
O3 |
| C1 | | 1.3861 | 2.5921 |
C2 | 1.3861 | | 1.2060 | O3 | 2.5921 | 1.2060 | |
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 B3LYP/LANL2DZ
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
-0.038 |
|
|
|
| 2 |
C |
0.099 |
|
|
|
| 3 |
O |
-0.062 |
|
|
|
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 |
0.845 |
0.845 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-17.707 |
0.000 |
0.000 |
| y |
0.000 |
-14.199 |
0.000 |
| z |
0.000 |
0.000 |
-23.038 |
|
| Traceless |
| | x | y | z |
| x |
0.912 |
0.000 |
0.000 |
| y |
0.000 |
6.174 |
0.000 |
| z |
0.000 |
0.000 |
-7.085 |
|
| Polar |
| 3z2-r2 | -14.171 |
| x2-y2 | -3.508 |
| 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 |
1.647 |
0.000 |
0.000 |
| y |
0.000 |
2.004 |
0.000 |
| z |
0.000 |
0.000 |
5.552 |
<r2> (average value of r
2) Å
2
| <r2> |
34.514 |
| (<r2>)1/2 |
5.875 |