Jump to
S2C1
Energy calculated at B1B95/3-21G
| | hartrees |
| Energy at 0K | -151.168464 |
| Energy at 298.15K | |
| HF Energy | -151.168464 |
| Nuclear repulsion energy | 63.209030 |
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 B1B95/3-21G
| 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 |
2158 |
2065 |
0.00 |
57.16 |
0.61 |
0.76 |
| 2 |
Σg |
930 |
890 |
0.00 |
81.16 |
0.43 |
0.61 |
| 3 |
Σu |
1536 |
1470 |
244.39 |
0.00 |
0.00 |
0.00 |
| 4 |
Πg |
355 |
339 |
0.00 |
4.91 |
0.75 |
0.86 |
| 4 |
Πg |
355 |
339 |
0.00 |
4.91 |
0.75 |
0.86 |
| 5 |
Πu |
148 |
141 |
14.76 |
0.00 |
0.00 |
0.00 |
| 5 |
Πu |
148 |
141 |
14.76 |
0.00 |
0.00 |
0.00 |
Unscaled Zero Point Vibrational Energy (zpe) 2814.0 cm
-1
Scaled (by 0.9567) Zero Point Vibrational Energy (zpe) 2692.2 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 B1B95/3-21G
Point Group is D∞h
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
0.000 |
0.000 |
0.641 |
| C2 |
0.000 |
0.000 |
-0.641 |
| C3 |
0.000 |
0.000 |
1.961 |
| C4 |
0.000 |
0.000 |
-1.961 |
Atom - Atom Distances (Å)
| |
C1 |
C2 |
C3 |
C4 |
| C1 | | 1.2823 | 1.3203 | 2.6026 |
C2 | 1.2823 | | 2.6026 | 1.3203 | C3 | 1.3203 | 2.6026 | | 3.9229 | C4 | 2.6026 | 1.3203 | 3.9229 | |
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 B1B95/3-21G
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
-0.139 |
|
|
|
| 2 |
C |
-0.139 |
|
|
|
| 3 |
C |
0.139 |
|
|
|
| 4 |
C |
0.139 |
|
|
|
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 |
-21.896 |
0.000 |
0.000 |
| y |
0.000 |
-21.896 |
0.000 |
| z |
0.000 |
0.000 |
-31.677 |
|
| Traceless |
| | x | y | z |
| x |
4.890 |
0.000 |
0.000 |
| y |
0.000 |
4.890 |
0.000 |
| z |
0.000 |
0.000 |
-9.781 |
|
| Polar |
| 3z2-r2 | -19.562 |
| 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 |
2.614 |
0.000 |
0.000 |
| y |
0.000 |
2.614 |
0.000 |
| z |
0.000 |
0.000 |
11.926 |
<r2> (average value of r
2) Å
2
| <r2> |
66.814 |
| (<r2>)1/2 |
8.174 |
Jump to
S1C1
Energy calculated at B1B95/3-21G
| | hartrees |
| Energy at 0K | -151.139789 |
| Energy at 298.15K | |
| HF Energy | -151.139789 |
| Nuclear repulsion energy | 63.135254 |
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 B1B95/3-21G
| 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 |
2163 |
2069 |
0.00 |
49.36 |
0.42 |
0.59 |
| 2 |
Σg |
929 |
888 |
0.00 |
68.43 |
0.35 |
0.52 |
| 3 |
Σu |
1556 |
1489 |
324.35 |
0.00 |
0.00 |
0.00 |
| 4 |
Πg |
495 |
473 |
0.00 |
9.98 |
0.75 |
0.86 |
| 4 |
Πg |
286 |
273 |
0.00 |
8.72 |
0.75 |
0.86 |
| 5 |
Πu |
174 |
166 |
3.02 |
0.00 |
0.00 |
0.00 |
| 5 |
Πu |
153 |
146 |
21.85 |
0.00 |
0.00 |
0.00 |
Unscaled Zero Point Vibrational Energy (zpe) 2877.0 cm
-1
Scaled (by 0.9567) Zero Point Vibrational Energy (zpe) 2752.4 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 B1B95/3-21G
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 |
1.963 |
| C4 |
0.000 |
0.000 |
-1.963 |
Atom - Atom Distances (Å)
| |
C1 |
C2 |
C3 |
C4 |
| C1 | | 1.2865 | 1.3202 | 2.6067 |
C2 | 1.2865 | | 2.6067 | 1.3202 | C3 | 1.3202 | 2.6067 | | 3.9269 | C4 | 2.6067 | 1.3202 | 3.9269 | |
More geometry information
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at B1B95/3-21G
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
-0.140 |
|
|
|
| 2 |
C |
-0.140 |
|
|
|
| 3 |
C |
0.140 |
|
|
|
| 4 |
C |
0.140 |
|
|
|
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 |
-20.060 |
0.000 |
0.000 |
| y |
0.000 |
-23.802 |
0.000 |
| z |
0.000 |
0.000 |
-31.404 |
|
| Traceless |
| | x | y | z |
| x |
7.543 |
0.000 |
0.000 |
| y |
0.000 |
1.929 |
0.000 |
| z |
0.000 |
0.000 |
-9.473 |
|
| Polar |
| 3z2-r2 | -18.945 |
| x2-y2 | 3.743 |
| 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 |
2.626 |
0.000 |
0.000 |
| y |
0.000 |
2.175 |
0.000 |
| z |
0.000 |
0.000 |
11.417 |
<r2> (average value of r
2) Å
2
| <r2> |
66.897 |
| (<r2>)1/2 |
8.179 |