Jump to
S2C1
Energy calculated at B3PW91/6-311G**
| | hartrees |
| Energy at 0K | -152.050246 |
| Energy at 298.15K | |
| HF Energy | -152.050246 |
| Nuclear repulsion energy | 63.360533 |
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 B3PW91/6-311G**
| 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 |
2133 |
2054 |
0.00 |
59.53 |
0.63 |
0.78 |
| 2 |
Σg |
939 |
905 |
0.00 |
93.41 |
0.42 |
0.59 |
| 3 |
Σu |
1589 |
1530 |
293.66 |
0.00 |
0.00 |
0.00 |
| 4 |
Πg |
330 |
318 |
0.00 |
13.24 |
0.75 |
0.86 |
| 4 |
Πg |
330 |
318 |
0.00 |
13.24 |
0.75 |
0.86 |
| 5 |
Πu |
164 |
158 |
23.71 |
0.00 |
0.00 |
0.00 |
| 5 |
Πu |
164 |
158 |
23.71 |
0.00 |
0.00 |
0.00 |
Unscaled Zero Point Vibrational Energy (zpe) 2823.8 cm
-1
Scaled (by 0.9631) Zero Point Vibrational Energy (zpe) 2719.6 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 B3PW91/6-311G**
Point Group is D∞h
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
0.000 |
0.000 |
0.644 |
| C2 |
0.000 |
0.000 |
-0.644 |
| C3 |
0.000 |
0.000 |
1.956 |
| C4 |
0.000 |
0.000 |
-1.956 |
Atom - Atom Distances (Å)
| |
C1 |
C2 |
C3 |
C4 |
| C1 | | 1.2884 | 1.3115 | 2.6000 |
C2 | 1.2884 | | 2.6000 | 1.3115 | C3 | 1.3115 | 2.6000 | | 3.9115 | C4 | 2.6000 | 1.3115 | 3.9115 | |
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 B3PW91/6-311G**
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
0.094 |
|
|
|
| 2 |
C |
0.094 |
|
|
|
| 3 |
C |
-0.094 |
|
|
|
| 4 |
C |
-0.094 |
|
|
|
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 |
-21.838 |
0.000 |
0.000 |
| y |
0.000 |
-21.838 |
0.000 |
| z |
0.000 |
0.000 |
-32.740 |
|
| Traceless |
| | x | y | z |
| x |
5.451 |
0.000 |
0.000 |
| y |
0.000 |
5.451 |
0.000 |
| z |
0.000 |
0.000 |
-10.901 |
|
| Polar |
| 3z2-r2 | -21.803 |
| 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 |
3.379 |
0.000 |
0.000 |
| y |
0.000 |
3.379 |
0.000 |
| z |
0.000 |
0.000 |
12.943 |
<r2> (average value of r
2) Å
2
| <r2> |
66.790 |
| (<r2>)1/2 |
8.172 |
Jump to
S1C1
Energy calculated at B3PW91/6-311G**
| | hartrees |
| Energy at 0K | -152.018582 |
| Energy at 298.15K | |
| HF Energy | -152.018582 |
| Nuclear repulsion energy | 63.265414 |
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 B3PW91/6-311G**
| 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 |
2136 |
2057 |
0.00 |
71.48 |
0.43 |
0.60 |
| 2 |
Σg |
936 |
902 |
0.00 |
77.43 |
0.34 |
0.51 |
| 3 |
Σu |
1601 |
1542 |
378.90 |
0.00 |
0.00 |
0.00 |
| 4 |
Πg |
462 |
445 |
0.00 |
5.85 |
0.75 |
0.86 |
| 4 |
Πg |
249 |
240 |
0.00 |
12.17 |
0.75 |
0.86 |
| 5 |
Πu |
204 |
197 |
6.45 |
0.00 |
0.00 |
0.00 |
| 5 |
Πu |
137 |
132 |
34.67 |
0.00 |
0.00 |
0.00 |
Unscaled Zero Point Vibrational Energy (zpe) 2862.3 cm
-1
Scaled (by 0.9631) Zero Point Vibrational Energy (zpe) 2756.7 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 B3PW91/6-311G**
Point Group is D∞h
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
0.000 |
0.000 |
0.646 |
| C2 |
0.000 |
0.000 |
-0.646 |
| C3 |
0.000 |
0.000 |
1.958 |
| C4 |
0.000 |
0.000 |
-1.958 |
Atom - Atom Distances (Å)
| |
C1 |
C2 |
C3 |
C4 |
| C1 | | 1.2930 | 1.3119 | 2.6049 |
C2 | 1.2930 | | 2.6049 | 1.3119 | C3 | 1.3119 | 2.6049 | | 3.9169 | C4 | 2.6049 | 1.3119 | 3.9169 | |
More geometry information
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at B3PW91/6-311G**
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
0.090 |
|
|
|
| 2 |
C |
0.090 |
|
|
|
| 3 |
C |
-0.090 |
|
|
|
| 4 |
C |
-0.090 |
|
|
|
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 |
-20.080 |
0.000 |
0.000 |
| y |
0.000 |
-23.764 |
0.000 |
| z |
0.000 |
0.000 |
-32.499 |
|
| Traceless |
| | x | y | z |
| x |
8.051 |
0.000 |
0.000 |
| y |
0.000 |
2.526 |
0.000 |
| z |
0.000 |
0.000 |
-10.577 |
|
| Polar |
| 3z2-r2 | -21.155 |
| x2-y2 | 3.684 |
| 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 |
3.274 |
0.000 |
0.000 |
| y |
0.000 |
2.999 |
0.000 |
| z |
0.000 |
0.000 |
12.499 |
<r2> (average value of r
2) Å
2
| <r2> |
66.935 |
| (<r2>)1/2 |
8.181 |