Jump to
S2C1
Energy calculated at HF/6-311+G(3df,2p)
| | hartrees |
| Energy at 0K | -151.230782 |
| Energy at 298.15K | |
| HF Energy | -151.230782 |
| Nuclear repulsion energy | 64.243956 |
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 HF/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 |
2323 |
2111 |
0.00 |
107.16 |
0.39 |
0.57 |
| 2 |
Σg |
1008 |
916 |
0.00 |
311.83 |
0.30 |
0.46 |
| 3 |
Σu |
1723 |
1566 |
176.31 |
0.00 |
0.00 |
0.00 |
| 4 |
Πg |
503 |
457 |
0.00 |
18.34 |
0.75 |
0.86 |
| 4 |
Πg |
503 |
457 |
0.00 |
18.34 |
0.75 |
0.86 |
| 5 |
Πu |
225 |
204 |
26.75 |
0.00 |
0.00 |
0.00 |
| 5 |
Πu |
225 |
204 |
26.75 |
0.00 |
0.00 |
0.00 |
Unscaled Zero Point Vibrational Energy (zpe) 3255.1 cm
-1
Scaled (by 0.9086) Zero Point Vibrational Energy (zpe) 2957.5 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 HF/6-311+G(3df,2p)
Point Group is D∞h
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
0.000 |
0.000 |
0.635 |
| C2 |
0.000 |
0.000 |
-0.635 |
| C3 |
0.000 |
0.000 |
1.929 |
| C4 |
0.000 |
0.000 |
-1.929 |
Atom - Atom Distances (Å)
| |
C1 |
C2 |
C3 |
C4 |
| C1 | | 1.2709 | 1.2934 | 2.5643 |
C2 | 1.2709 | | 2.5643 | 1.2934 | C3 | 1.2934 | 2.5643 | | 3.8577 | C4 | 2.5643 | 1.2934 | 3.8577 | |
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 HF/6-311+G(3df,2p)
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
0.450 |
|
|
|
| 2 |
C |
0.450 |
|
|
|
| 3 |
C |
-0.450 |
|
|
|
| 4 |
C |
-0.450 |
|
|
|
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 |
-22.450 |
0.000 |
0.000 |
| y |
0.000 |
-22.450 |
0.000 |
| z |
0.000 |
0.000 |
-33.636 |
|
| Traceless |
| | x | y | z |
| x |
5.593 |
0.000 |
0.000 |
| y |
0.000 |
5.593 |
0.000 |
| z |
0.000 |
0.000 |
-11.186 |
|
| Polar |
| 3z2-r2 | -22.373 |
| 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 |
4.801 |
0.000 |
0.000 |
| y |
0.000 |
4.801 |
0.000 |
| z |
0.000 |
0.000 |
15.802 |
<r2> (average value of r
2) Å
2
| <r2> |
65.842 |
| (<r2>)1/2 |
8.114 |
Jump to
S1C1
Energy calculated at HF/6-311+G(3df,2p)
| | hartrees |
| Energy at 0K | -151.181328 |
| Energy at 298.15K | |
| HF Energy | -151.181328 |
| Nuclear repulsion energy | 64.228426 |
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 HF/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 |
2317 |
2105 |
0.00 |
90.62 |
0.28 |
0.44 |
| 2 |
Σg |
1012 |
920 |
0.00 |
121.71 |
0.22 |
0.35 |
| 3 |
Σu |
1716 |
1559 |
482.34 |
0.00 |
0.00 |
0.00 |
| 4 |
Πg |
545 |
496 |
0.00 |
1.62 |
0.75 |
0.86 |
| 4 |
Πg |
422 |
384 |
0.00 |
12.84 |
0.75 |
0.86 |
| 5 |
Πu |
231 |
210 |
5.28 |
0.00 |
0.00 |
0.00 |
| 5 |
Πu |
209 |
190 |
29.30 |
0.00 |
0.00 |
0.00 |
Unscaled Zero Point Vibrational Energy (zpe) 3226.0 cm
-1
Scaled (by 0.9086) Zero Point Vibrational Energy (zpe) 2931.1 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 HF/6-311+G(3df,2p)
Point Group is D∞h
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
0.000 |
0.000 |
0.638 |
| C2 |
0.000 |
0.000 |
-0.638 |
| C3 |
0.000 |
0.000 |
1.929 |
| C4 |
0.000 |
0.000 |
-1.929 |
Atom - Atom Distances (Å)
| |
C1 |
C2 |
C3 |
C4 |
| C1 | | 1.2750 | 1.2914 | 2.5664 |
C2 | 1.2750 | | 2.5664 | 1.2914 | C3 | 1.2914 | 2.5664 | | 3.8578 | C4 | 2.5664 | 1.2914 | 3.8578 | |
More geometry information
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at HF/6-311+G(3df,2p)
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
0.433 |
|
|
|
| 2 |
C |
0.433 |
|
|
|
| 3 |
C |
-0.433 |
|
|
|
| 4 |
C |
-0.433 |
|
|
|
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 |
-20.704 |
0.000 |
0.000 |
| y |
0.000 |
-24.555 |
0.000 |
| z |
0.000 |
0.000 |
-32.574 |
|
| Traceless |
| | x | y | z |
| x |
7.860 |
0.000 |
0.000 |
| y |
0.000 |
2.084 |
0.000 |
| z |
0.000 |
0.000 |
-9.944 |
|
| Polar |
| 3z2-r2 | -19.889 |
| x2-y2 | 3.851 |
| 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 |
4.495 |
0.000 |
0.000 |
| y |
0.000 |
4.380 |
0.000 |
| z |
0.000 |
0.000 |
13.585 |
<r2> (average value of r
2) Å
2
| <r2> |
65.730 |
| (<r2>)1/2 |
8.107 |