Jump to
S2C1
Energy calculated at B3PW91/6-31G
| | hartrees |
| Energy at 0K | -151.976734 |
| Energy at 298.15K | |
| HF Energy | -151.976734 |
| Nuclear repulsion energy | 62.768453 |
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 B3PW91/6-31G
| Mode Number |
Symmetry |
Frequency (cm-1) |
Scaled Frequency (cm-1) |
IR Intensities (km mol-1) |
Raman Act (Å4/u) |
Dep P |
Dep U |
| 1 |
Σg |
2142 |
2051 |
0.00 |
|
|
|
| 2 |
Σg |
926 |
887 |
0.00 |
|
|
|
| 3 |
Σu |
1541 |
1475 |
256.03 |
|
|
|
| 4 |
Πg |
272 |
261 |
0.00 |
|
|
|
| 4 |
Πg |
272 |
261 |
0.00 |
|
|
|
| 5 |
Πu |
143 |
137 |
20.75 |
|
|
|
| 5 |
Πu |
143 |
137 |
20.75 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 2718.9 cm
-1
Scaled (by 0.9577) Zero Point Vibrational Energy (zpe) 2603.9 cm
-1
See section
III.C.1 List or set vibrational scaling factors
to change the scale factors used here.
See section
III.C.2
Calculate a vibrational scaling factor for a given set of molecules
to determine the least squares best scaling factor.
Geometric Data calculated at B3PW91/6-31G
Point Group is D∞h
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
0.000 |
0.000 |
0.647 |
| C2 |
0.000 |
0.000 |
-0.647 |
| C3 |
0.000 |
0.000 |
1.975 |
| C4 |
0.000 |
0.000 |
-1.975 |
Atom - Atom Distances (Å)
| |
C1 |
C2 |
C3 |
C4 |
| C1 | | 1.2931 | 1.3285 | 2.6216 |
C2 | 1.2931 | | 2.6216 | 1.3285 | C3 | 1.3285 | 2.6216 | | 3.9501 | C4 | 2.6216 | 1.3285 | 3.9501 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| C1 |
C2 |
C4 |
180.000 |
|
C2 |
C1 |
C3 |
180.000 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at B3PW91/6-31G
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
-0.098 |
|
|
|
| 2 |
C |
-0.098 |
|
|
|
| 3 |
C |
0.098 |
|
|
|
| 4 |
C |
0.098 |
|
|
|
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 |
-21.366 |
0.000 |
0.000 |
| y |
0.000 |
-21.366 |
0.000 |
| z |
0.000 |
0.000 |
-32.752 |
|
| Traceless |
| | x | y | z |
| x |
5.693 |
0.000 |
0.000 |
| y |
0.000 |
5.693 |
0.000 |
| z |
0.000 |
0.000 |
-11.387 |
|
| Polar |
| 3z2-r2 | -22.773 |
| 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 |
2.964 |
0.000 |
0.000 |
| y |
0.000 |
2.964 |
0.000 |
| z |
0.000 |
0.000 |
12.618 |
<r2> (average value of r
2) Å
2
| <r2> |
67.541 |
| (<r2>)1/2 |
8.218 |
Jump to
S1C1
Energy calculated at B3PW91/6-31G
| | hartrees |
| Energy at 0K | -151.946494 |
| Energy at 298.15K | |
| HF Energy | -151.946494 |
| Nuclear repulsion energy | 62.693434 |
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 B3PW91/6-31G
| Mode Number |
Symmetry |
Frequency (cm-1) |
Scaled Frequency (cm-1) |
IR Intensities (km mol-1) |
Raman Act (Å4/u) |
Dep P |
Dep U |
| 1 |
Σg |
2148 |
2058 |
0.00 |
|
|
|
| 2 |
Σg |
925 |
886 |
0.00 |
|
|
|
| 3 |
Σu |
1562 |
1496 |
344.92 |
|
|
|
| 4 |
Πg |
438 |
420 |
0.00 |
|
|
|
| 4 |
Πg |
232 |
222 |
0.00 |
|
|
|
| 5 |
Πu |
162 |
155 |
5.07 |
|
|
|
| 5 |
Πu |
162 |
155 |
28.16 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 2815.0 cm
-1
Scaled (by 0.9577) Zero Point Vibrational Energy (zpe) 2695.9 cm
-1
See section
III.C.1 List or set vibrational scaling factors
to change the scale factors used here.
See section
III.C.2
Calculate a vibrational scaling factor for a given set of molecules
to determine the least squares best scaling factor.
Geometric Data calculated at B3PW91/6-31G
Point Group is D∞h
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
0.000 |
0.000 |
0.649 |
| C2 |
0.000 |
0.000 |
-0.649 |
| C3 |
0.000 |
0.000 |
1.977 |
| C4 |
0.000 |
0.000 |
-1.977 |
Atom - Atom Distances (Å)
| |
C1 |
C2 |
C3 |
C4 |
| C1 | | 1.2979 | 1.3281 | 2.6260 |
C2 | 1.2979 | | 2.6260 | 1.3281 | C3 | 1.3281 | 2.6260 | | 3.9541 | C4 | 2.6260 | 1.3281 | 3.9541 | |
More geometry information
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at B3PW91/6-31G
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
-0.095 |
|
|
|
| 2 |
C |
-0.095 |
|
|
|
| 3 |
C |
0.095 |
|
|
|
| 4 |
C |
0.095 |
|
|
|
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 |
-23.268 |
0.000 |
0.000 |
| y |
0.000 |
-19.559 |
0.000 |
| z |
0.000 |
0.000 |
-32.431 |
|
| Traceless |
| | x | y | z |
| x |
2.727 |
0.000 |
0.000 |
| y |
0.000 |
8.290 |
0.000 |
| z |
0.000 |
0.000 |
-11.017 |
|
| Polar |
| 3z2-r2 | -22.034 |
| x2-y2 | -3.709 |
| 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 |
2.503 |
0.000 |
0.000 |
| y |
0.000 |
2.821 |
0.000 |
| z |
0.000 |
0.000 |
12.029 |
<r2> (average value of r
2) Å
2
| <r2> |
67.626 |
| (<r2>)1/2 |
8.223 |