Jump to
S2C1
Energy calculated at B3LYP/6-311+G(3df,2p)
| | hartrees |
| Energy at 0K | -152.141881 |
| Energy at 298.15K | |
| HF Energy | -152.141881 |
| Nuclear repulsion energy | 63.618083 |
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 B3LYP/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 |
2124 |
2054 |
0.00 |
68.51 |
0.54 |
0.70 |
| 2 |
Σg |
942 |
911 |
0.00 |
98.20 |
0.32 |
0.48 |
| 3 |
Σu |
1597 |
1544 |
321.16 |
0.00 |
0.00 |
0.00 |
| 4 |
Πg |
388 |
376 |
0.00 |
17.63 |
0.75 |
0.86 |
| 4 |
Πg |
388 |
376 |
0.00 |
17.63 |
0.75 |
0.86 |
| 5 |
Πu |
177 |
171 |
26.33 |
0.00 |
0.00 |
0.00 |
| 5 |
Πu |
177 |
171 |
26.33 |
0.00 |
0.00 |
0.00 |
Unscaled Zero Point Vibrational Energy (zpe) 2896.3 cm
-1
Scaled (by 0.967) Zero Point Vibrational Energy (zpe) 2800.8 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 B3LYP/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 |
1.948 |
| C4 |
0.000 |
0.000 |
-1.948 |
Atom - Atom Distances (Å)
| |
C1 |
C2 |
C3 |
C4 |
| C1 | | 1.2858 | 1.3047 | 2.5905 |
C2 | 1.2858 | | 2.5905 | 1.3047 | C3 | 1.3047 | 2.5905 | | 3.8951 | C4 | 2.5905 | 1.3047 | 3.8951 | |
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 B3LYP/6-311+G(3df,2p)
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
0.514 |
|
|
|
| 2 |
C |
0.514 |
|
|
|
| 3 |
C |
-0.514 |
|
|
|
| 4 |
C |
-0.514 |
|
|
|
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 |
-22.211 |
0.000 |
0.000 |
| y |
0.000 |
-22.211 |
0.000 |
| z |
0.000 |
0.000 |
-33.599 |
|
| Traceless |
| | x | y | z |
| x |
5.694 |
0.000 |
0.000 |
| y |
0.000 |
5.694 |
0.000 |
| z |
0.000 |
0.000 |
-11.388 |
|
| Polar |
| 3z2-r2 | -22.775 |
| 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 |
4.731 |
0.000 |
0.000 |
| y |
0.000 |
4.731 |
0.000 |
| z |
0.000 |
0.000 |
13.642 |
<r2> (average value of r
2) Å
2
| <r2> |
66.720 |
| (<r2>)1/2 |
8.168 |
Jump to
S1C1
Energy calculated at B3LYP/6-311+G(3df,2p)
| | hartrees |
| Energy at 0K | -152.113442 |
| Energy at 298.15K | |
| HF Energy | -152.113442 |
| Nuclear repulsion energy | 63.519768 |
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 B3LYP/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 |
2126 |
2056 |
0.00 |
95.67 |
0.37 |
0.54 |
| 2 |
Σg |
938 |
907 |
0.00 |
86.04 |
0.25 |
0.40 |
| 3 |
Σu |
1602 |
1549 |
390.63 |
0.00 |
0.00 |
0.00 |
| 4 |
Πg |
485 |
469 |
0.00 |
0.25 |
0.75 |
0.86 |
| 4 |
Πg |
297 |
288 |
0.00 |
18.04 |
0.75 |
0.86 |
| 5 |
Πu |
210 |
203 |
8.02 |
0.00 |
0.00 |
0.00 |
| 5 |
Πu |
150 |
145 |
39.10 |
0.00 |
0.00 |
0.00 |
Unscaled Zero Point Vibrational Energy (zpe) 2904.3 cm
-1
Scaled (by 0.967) Zero Point Vibrational Energy (zpe) 2808.4 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 B3LYP/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 |
1.950 |
| C4 |
0.000 |
0.000 |
-1.950 |
Atom - Atom Distances (Å)
| |
C1 |
C2 |
C3 |
C4 |
| C1 | | 1.2895 | 1.3057 | 2.5951 |
C2 | 1.2895 | | 2.5951 | 1.3057 | C3 | 1.3057 | 2.5951 | | 3.9008 | C4 | 2.5951 | 1.3057 | 3.9008 | |
More geometry information
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at B3LYP/6-311+G(3df,2p)
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
0.509 |
|
|
|
| 2 |
C |
0.509 |
|
|
|
| 3 |
C |
-0.509 |
|
|
|
| 4 |
C |
-0.509 |
|
|
|
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 |
-24.130 |
0.000 |
0.000 |
| y |
0.000 |
-20.510 |
0.000 |
| z |
0.000 |
0.000 |
-33.426 |
|
| Traceless |
| | x | y | z |
| x |
2.838 |
0.000 |
0.000 |
| y |
0.000 |
8.268 |
0.000 |
| z |
0.000 |
0.000 |
-11.106 |
|
| Polar |
| 3z2-r2 | -22.213 |
| x2-y2 | -3.620 |
| 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 |
4.532 |
0.000 |
0.000 |
| y |
0.000 |
4.574 |
0.000 |
| z |
0.000 |
0.000 |
13.282 |
<r2> (average value of r
2) Å
2
| <r2> |
66.890 |
| (<r2>)1/2 |
8.179 |