Jump to
S2C1
Energy calculated at B1B95/6-31+G**
| | hartrees |
| Energy at 0K | -152.032722 |
| Energy at 298.15K | |
| HF Energy | -152.032722 |
| Nuclear repulsion energy | 63.298482 |
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 B1B95/6-31+G**
| 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 |
2160 |
2066 |
0.00 |
67.29 |
0.54 |
0.70 |
| 2 |
Σg |
952 |
911 |
0.00 |
99.46 |
0.36 |
0.53 |
| 3 |
Σu |
1618 |
1548 |
328.20 |
0.00 |
0.00 |
0.00 |
| 4 |
Πg |
378 |
362 |
0.00 |
8.64 |
0.75 |
0.86 |
| 4 |
Πg |
378 |
362 |
0.00 |
8.64 |
0.75 |
0.86 |
| 5 |
Πu |
174 |
166 |
21.53 |
0.00 |
0.00 |
0.00 |
| 5 |
Πu |
174 |
166 |
21.53 |
0.00 |
0.00 |
0.00 |
Unscaled Zero Point Vibrational Energy (zpe) 2917.2 cm
-1
Scaled (by 0.9566) Zero Point Vibrational Energy (zpe) 2790.6 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 B1B95/6-31+G**
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 |
1.957 |
| C4 |
0.000 |
0.000 |
-1.957 |
Atom - Atom Distances (Å)
| |
C1 |
C2 |
C3 |
C4 |
| C1 | | 1.2925 | 1.3112 | 2.6036 |
C2 | 1.2925 | | 2.6036 | 1.3112 | C3 | 1.3112 | 2.6036 | | 3.9148 | C4 | 2.6036 | 1.3112 | 3.9148 | |
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 B1B95/6-31+G**
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
1.099 |
|
|
|
| 2 |
C |
1.099 |
|
|
|
| 3 |
C |
-1.099 |
|
|
|
| 4 |
C |
-1.099 |
|
|
|
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 |
-22.091 |
0.000 |
0.000 |
| y |
0.000 |
-22.091 |
0.000 |
| z |
0.000 |
0.000 |
-33.123 |
|
| Traceless |
| | x | y | z |
| x |
5.516 |
0.000 |
0.000 |
| y |
0.000 |
5.516 |
0.000 |
| z |
0.000 |
0.000 |
-11.032 |
|
| Polar |
| 3z2-r2 | -22.063 |
| 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 |
3.848 |
0.000 |
0.000 |
| y |
0.000 |
3.848 |
0.000 |
| z |
0.000 |
0.000 |
13.751 |
<r2> (average value of r
2) Å
2
| <r2> |
67.082 |
| (<r2>)1/2 |
8.190 |
Jump to
S1C1
Energy calculated at B1B95/6-31+G**
| | hartrees |
| Energy at 0K | -152.002644 |
| Energy at 298.15K | |
| HF Energy | -152.002644 |
| Nuclear repulsion energy | 63.199237 |
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 B1B95/6-31+G**
| 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 |
2162 |
2069 |
0.00 |
91.36 |
0.39 |
0.56 |
| 2 |
Σg |
949 |
907 |
0.00 |
84.08 |
0.30 |
0.47 |
| 3 |
Σu |
1623 |
1553 |
412.48 |
0.00 |
0.00 |
0.00 |
| 4 |
Πg |
472 |
452 |
0.00 |
1.23 |
0.75 |
0.86 |
| 4 |
Πg |
304 |
291 |
0.00 |
12.58 |
0.75 |
0.86 |
| 5 |
Πu |
202 |
194 |
5.11 |
0.00 |
0.00 |
0.00 |
| 5 |
Πu |
157 |
151 |
33.11 |
0.00 |
0.00 |
0.00 |
Unscaled Zero Point Vibrational Energy (zpe) 2935.0 cm
-1
Scaled (by 0.9566) Zero Point Vibrational Energy (zpe) 2807.6 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 B1B95/6-31+G**
Point Group is D∞h
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
0.000 |
0.000 |
0.648 |
| C2 |
0.000 |
0.000 |
-0.648 |
| C3 |
0.000 |
0.000 |
1.960 |
| C4 |
0.000 |
0.000 |
-1.960 |
Atom - Atom Distances (Å)
| |
C1 |
C2 |
C3 |
C4 |
| C1 | | 1.2960 | 1.3123 | 2.6083 |
C2 | 1.2960 | | 2.6083 | 1.3123 | C3 | 1.3123 | 2.6083 | | 3.9206 | C4 | 2.6083 | 1.3123 | 3.9206 | |
More geometry information
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at B1B95/6-31+G**
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
1.064 |
|
|
|
| 2 |
C |
1.064 |
|
|
|
| 3 |
C |
-1.064 |
|
|
|
| 4 |
C |
-1.064 |
|
|
|
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 |
-20.319 |
0.000 |
0.000 |
| y |
0.000 |
-24.083 |
0.000 |
| z |
0.000 |
0.000 |
-32.877 |
|
| Traceless |
| | x | y | z |
| x |
8.161 |
0.000 |
0.000 |
| y |
0.000 |
2.515 |
0.000 |
| z |
0.000 |
0.000 |
-10.676 |
|
| Polar |
| 3z2-r2 | -21.352 |
| x2-y2 | 3.764 |
| 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 |
3.651 |
0.000 |
0.000 |
| y |
0.000 |
3.677 |
0.000 |
| z |
0.000 |
0.000 |
13.339 |
<r2> (average value of r
2) Å
2
| <r2> |
67.242 |
| (<r2>)1/2 |
8.200 |