Jump to
S2C1
Energy calculated at B3PW91/6-311+G(3df,2p)
| | hartrees |
| Energy at 0K | -152.063015 |
| Energy at 298.15K | |
| HF Energy | -152.063015 |
| Nuclear repulsion energy | 63.553589 |
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 B3PW91/6-311+G(3df,2p)
| 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 |
2132 |
2041 |
0.00 |
63.94 |
0.58 |
0.73 |
| 2 |
Σg |
942 |
902 |
0.00 |
100.49 |
0.33 |
0.49 |
| 3 |
Σu |
1591 |
1523 |
325.74 |
0.00 |
0.00 |
0.00 |
| 4 |
Πg |
385 |
368 |
0.00 |
22.97 |
0.75 |
0.86 |
| 4 |
Πg |
385 |
368 |
0.00 |
22.97 |
0.75 |
0.86 |
| 5 |
Πu |
173 |
166 |
26.86 |
0.00 |
0.00 |
0.00 |
| 5 |
Πu |
173 |
166 |
26.86 |
0.00 |
0.00 |
0.00 |
Unscaled Zero Point Vibrational Energy (zpe) 2890.2 cm
-1
Scaled (by 0.9573) Zero Point Vibrational Energy (zpe) 2766.8 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 B3PW91/6-311+G(3df,2p)
Point Group is D∞h
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
0.000 |
0.000 |
0.643 |
| C2 |
0.000 |
0.000 |
-0.643 |
| C3 |
0.000 |
0.000 |
1.950 |
| C4 |
0.000 |
0.000 |
-1.950 |
Atom - Atom Distances (Å)
| |
C1 |
C2 |
C3 |
C4 |
| C1 | | 1.2853 | 1.3071 | 2.5924 |
C2 | 1.2853 | | 2.5924 | 1.3071 | C3 | 1.3071 | 2.5924 | | 3.8995 | C4 | 2.5924 | 1.3071 | 3.8995 | |
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 B3PW91/6-311+G(3df,2p)
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
0.549 |
|
|
|
| 2 |
C |
0.549 |
|
|
|
| 3 |
C |
-0.549 |
|
|
|
| 4 |
C |
-0.549 |
|
|
|
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 |
-22.038 |
0.000 |
0.000 |
| y |
0.000 |
-22.038 |
0.000 |
| z |
0.000 |
0.000 |
-33.202 |
|
| Traceless |
| | x | y | z |
| x |
5.582 |
0.000 |
0.000 |
| y |
0.000 |
5.582 |
0.000 |
| z |
0.000 |
0.000 |
-11.164 |
|
| Polar |
| 3z2-r2 | -22.329 |
| 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 |
4.724 |
0.000 |
0.000 |
| y |
0.000 |
4.724 |
0.000 |
| z |
0.000 |
0.000 |
13.647 |
<r2> (average value of r
2) Å
2
| <r2> |
66.662 |
| (<r2>)1/2 |
8.165 |
Jump to
S1C1
Energy calculated at B3PW91/6-311+G(3df,2p)
| | hartrees |
| Energy at 0K | -152.031183 |
| Energy at 298.15K | |
| HF Energy | -152.031183 |
| Nuclear repulsion energy | 63.460718 |
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 B3PW91/6-311+G(3df,2p)
| 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 |
2134 |
2043 |
0.00 |
92.55 |
0.37 |
0.54 |
| 2 |
Σg |
938 |
898 |
0.00 |
86.77 |
0.25 |
0.40 |
| 3 |
Σu |
1602 |
1533 |
408.51 |
0.00 |
0.00 |
0.00 |
| 4 |
Πg |
493 |
472 |
0.00 |
0.27 |
0.75 |
0.86 |
| 4 |
Πg |
281 |
269 |
0.00 |
18.83 |
0.75 |
0.86 |
| 5 |
Πu |
210 |
201 |
7.82 |
0.00 |
0.00 |
0.00 |
| 5 |
Πu |
142 |
136 |
38.88 |
0.00 |
0.00 |
0.00 |
Unscaled Zero Point Vibrational Energy (zpe) 2899.8 cm
-1
Scaled (by 0.9573) Zero Point Vibrational Energy (zpe) 2775.9 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 B3PW91/6-311+G(3df,2p)
Point Group is D∞h
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
0.000 |
0.000 |
0.645 |
| C2 |
0.000 |
0.000 |
-0.645 |
| C3 |
0.000 |
0.000 |
1.952 |
| C4 |
0.000 |
0.000 |
-1.952 |
Atom - Atom Distances (Å)
| |
C1 |
C2 |
C3 |
C4 |
| C1 | | 1.2897 | 1.3075 | 2.5972 |
C2 | 1.2897 | | 2.5972 | 1.3075 | C3 | 1.3075 | 2.5972 | | 3.9047 | C4 | 2.5972 | 1.3075 | 3.9047 | |
More geometry information
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at B3PW91/6-311+G(3df,2p)
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
0.541 |
|
|
|
| 2 |
C |
0.541 |
|
|
|
| 3 |
C |
-0.541 |
|
|
|
| 4 |
C |
-0.541 |
|
|
|
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 |
-20.339 |
0.000 |
0.000 |
| y |
0.000 |
-23.950 |
0.000 |
| z |
0.000 |
0.000 |
-32.994 |
|
| Traceless |
| | x | y | z |
| x |
8.133 |
0.000 |
0.000 |
| y |
0.000 |
2.716 |
0.000 |
| z |
0.000 |
0.000 |
-10.850 |
|
| Polar |
| 3z2-r2 | -21.699 |
| x2-y2 | 3.611 |
| 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 |
4.546 |
0.000 |
0.000 |
| y |
0.000 |
4.511 |
0.000 |
| z |
0.000 |
0.000 |
13.236 |
<r2> (average value of r
2) Å
2
| <r2> |
66.819 |
| (<r2>)1/2 |
8.174 |