Jump to
S2C1
Energy calculated at B3PW91/6-31G*
| hartrees |
Energy at 0K | -152.018343 |
Energy at 298.15K | |
HF Energy | -152.018343 |
Nuclear repulsion energy | 63.125828 |
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 |
2140 |
2047 |
0.00 |
|
|
|
2 |
Σg |
945 |
904 |
0.00 |
|
|
|
3 |
Σu |
1596 |
1527 |
266.48 |
|
|
|
4 |
Πg |
364 |
348 |
0.00 |
|
|
|
4 |
Πg |
364 |
348 |
0.00 |
|
|
|
5 |
Πu |
174 |
167 |
24.49 |
|
|
|
5 |
Πu |
174 |
167 |
24.49 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 2878.1 cm
-1
Scaled (by 0.9567) Zero Point Vibrational Energy (zpe) 2753.4 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 |
1.963 |
C4 |
0.000 |
0.000 |
-1.963 |
Atom - Atom Distances (Å)
|
C1 |
C2 |
C3 |
C4 |
C1 | | 1.2932 | 1.3164 | 2.6096 |
C2 | 1.2932 | | 2.6096 | 1.3164 | C3 | 1.3164 | 2.6096 | | 3.9261 | C4 | 2.6096 | 1.3164 | 3.9261 | |
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 |
0.109 |
|
|
|
2 |
C |
0.109 |
|
|
|
3 |
C |
-0.109 |
|
|
|
4 |
C |
-0.109 |
|
|
|
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 |
-21.227 |
0.000 |
0.000 |
y |
0.000 |
-21.227 |
0.000 |
z |
0.000 |
0.000 |
-32.154 |
|
Traceless |
| x | y | z |
x |
5.463 |
0.000 |
0.000 |
y |
0.000 |
5.463 |
0.000 |
z |
0.000 |
0.000 |
-10.927 |
|
Polar |
3z2-r2 | -21.854 |
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 |
2.972 |
0.000 |
0.000 |
y |
0.000 |
2.972 |
0.000 |
z |
0.000 |
0.000 |
12.411 |
<r2> (average value of r
2) Å
2
<r2> |
66.792 |
(<r2>)1/2 |
8.173 |
Jump to
S1C1
Energy calculated at B3PW91/6-31G*
| hartrees |
Energy at 0K | -151.986395 |
Energy at 298.15K | |
HF Energy | -151.986395 |
Nuclear repulsion energy | 63.036800 |
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 |
2145 |
2052 |
0.00 |
|
|
|
2 |
Σg |
942 |
901 |
0.00 |
|
|
|
3 |
Σu |
1611 |
1542 |
355.73 |
|
|
|
4 |
Πg |
486 |
465 |
0.00 |
|
|
|
4 |
Πg |
293 |
280 |
0.00 |
|
|
|
5 |
Πu |
208 |
199 |
7.97 |
|
|
|
5 |
Πu |
156 |
150 |
34.01 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 2920.3 cm
-1
Scaled (by 0.9567) Zero Point Vibrational Energy (zpe) 2793.8 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 |
1.965 |
C4 |
0.000 |
0.000 |
-1.965 |
Atom - Atom Distances (Å)
|
C1 |
C2 |
C3 |
C4 |
C1 | | 1.2981 | 1.3164 | 2.6146 |
C2 | 1.2981 | | 2.6146 | 1.3164 | C3 | 1.3164 | 2.6146 | | 3.9310 | C4 | 2.6146 | 1.3164 | 3.9310 | |
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 |
0.108 |
|
|
|
2 |
C |
0.108 |
|
|
|
3 |
C |
-0.108 |
|
|
|
4 |
C |
-0.108 |
|
|
|
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 |
-23.059 |
0.000 |
0.000 |
y |
0.000 |
-19.508 |
0.000 |
z |
0.000 |
0.000 |
-31.881 |
|
Traceless |
| x | y | z |
x |
2.635 |
0.000 |
0.000 |
y |
0.000 |
7.961 |
0.000 |
z |
0.000 |
0.000 |
-10.597 |
|
Polar |
3z2-r2 | -21.194 |
x2-y2 | -3.551 |
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 |
2.596 |
0.000 |
0.000 |
y |
0.000 |
2.914 |
0.000 |
z |
0.000 |
0.000 |
11.943 |
<r2> (average value of r
2) Å
2
<r2> |
66.913 |
(<r2>)1/2 |
8.180 |