Jump to
S2C1
Energy calculated at HF/STO-3G
| | hartrees |
| Energy at 0K | -148.468965 |
| Energy at 298.15K | -148.467209 |
| HF Energy | -148.468965 |
| Nuclear repulsion energy | 45.442141 |
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/STO-3G
Point Group is C∞v
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
0.000 |
0.000 |
-1.415 |
| C2 |
0.000 |
0.000 |
-0.080 |
| O3 |
0.000 |
0.000 |
1.121 |
Atom - Atom Distances (Å)
| |
C1 |
C2 |
O3 |
| C1 | | 1.3353 | 2.5358 |
C2 | 1.3353 | | 1.2005 | O3 | 2.5358 | 1.2005 | |
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 HF/STO-3G
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
-0.043 |
|
|
|
| 2 |
C |
0.093 |
|
|
|
| 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 |
1.727 |
1.727 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-13.711 |
0.000 |
0.000 |
| y |
0.000 |
-13.711 |
0.000 |
| z |
0.000 |
0.000 |
-20.192 |
|
| Traceless |
| | x | y | z |
| x |
3.241 |
0.000 |
0.000 |
| y |
0.000 |
3.241 |
0.000 |
| z |
0.000 |
0.000 |
-6.481 |
|
| Polar |
| 3z2-r2 | -12.962 |
| 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 |
1.084 |
0.000 |
0.000 |
| y |
0.000 |
1.084 |
0.000 |
| z |
0.000 |
0.000 |
3.677 |
<r2> (average value of r
2) Å
2
| <r2> |
32.014 |
| (<r2>)1/2 |
5.658 |
Jump to
S1C1
Energy calculated at HF/STO-3G
| | hartrees |
| Energy at 0K | -148.403893 |
| Energy at 298.15K | -148.402284 |
| HF Energy | -148.403893 |
| Nuclear repulsion energy | 45.488164 |
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/STO-3G
Point Group is C∞v
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
0.000 |
0.000 |
-1.414 |
| C2 |
0.000 |
0.000 |
-0.079 |
| O3 |
0.000 |
0.000 |
1.120 |
Atom - Atom Distances (Å)
| |
C1 |
C2 |
O3 |
| C1 | | 1.3356 | 2.5338 |
C2 | 1.3356 | | 1.1982 | O3 | 2.5338 | 1.1982 | |
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 HF/STO-3G
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
0.014 |
|
|
|
| 2 |
C |
0.098 |
|
|
|
| 3 |
O |
-0.112 |
|
|
|
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 |
0.841 |
0.841 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-14.852 |
0.000 |
0.000 |
| y |
0.000 |
-12.468 |
0.000 |
| z |
0.000 |
0.000 |
-19.965 |
|
| Traceless |
| | x | y | z |
| x |
1.364 |
0.000 |
0.000 |
| y |
0.000 |
4.941 |
0.000 |
| z |
0.000 |
0.000 |
-6.305 |
|
| Polar |
| 3z2-r2 | -12.610 |
| x2-y2 | -2.384 |
| 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 |
0.529 |
0.000 |
0.000 |
| y |
0.000 |
1.073 |
0.000 |
| z |
0.000 |
0.000 |
3.131 |
<r2> (average value of r
2) Å
2
| <r2> |
31.908 |
| (<r2>)1/2 |
5.649 |