Jump to
S2C1
Energy calculated at B2PLYP/3-21G*
| | hartrees |
| Energy at 0K | -151.033118 |
| Energy at 298.15K | |
| HF Energy | -150.930637 |
| Nuclear repulsion energy | 62.970247 |
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 B2PLYP/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 |
2120 |
2120 |
0.00 |
48.02 |
0.68 |
0.81 |
| 2 |
Σg |
912 |
912 |
0.00 |
64.41 |
0.47 |
0.64 |
| 3 |
Σu |
1498 |
1498 |
237.88 |
0.00 |
0.00 |
0.00 |
| 4 |
Πg |
229 |
229 |
0.00 |
6.09 |
0.75 |
0.86 |
| 4 |
Πg |
229 |
229 |
0.00 |
6.09 |
0.75 |
0.86 |
| 5 |
Πu |
132 |
132 |
16.80 |
0.00 |
0.00 |
0.00 |
| 5 |
Πu |
132 |
132 |
16.80 |
0.00 |
0.00 |
0.00 |
Unscaled Zero Point Vibrational Energy (zpe) 2625.4 cm
-1
Scaled (by 1) Zero Point Vibrational Energy (zpe) 2625.4 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 B2PLYP/3-21G*
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 |
1.969 |
| C4 |
0.000 |
0.000 |
-1.969 |
Atom - Atom Distances (Å)
| |
C1 |
C2 |
C3 |
C4 |
| C1 | | 1.2872 | 1.3253 | 2.6125 |
C2 | 1.2872 | | 2.6125 | 1.3253 | C3 | 1.3253 | 2.6125 | | 3.9378 | C4 | 2.6125 | 1.3253 | 3.9378 | |
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 B2PLYP/3-21G*
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
-0.162 |
|
|
|
| 2 |
C |
-0.162 |
|
|
|
| 3 |
C |
0.162 |
|
|
|
| 4 |
C |
0.162 |
|
|
|
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 |
-21.989 |
0.000 |
0.000 |
| y |
0.000 |
-21.989 |
0.000 |
| z |
0.000 |
0.000 |
-32.460 |
|
| Traceless |
| | x | y | z |
| x |
5.236 |
0.000 |
0.000 |
| y |
0.000 |
5.236 |
0.000 |
| z |
0.000 |
0.000 |
-10.471 |
|
| Polar |
| 3z2-r2 | -20.942 |
| 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 |
2.674 |
0.000 |
0.000 |
| y |
0.000 |
2.674 |
0.000 |
| z |
0.000 |
0.000 |
11.967 |
<r2> (average value of r
2) Å
2
| <r2> |
67.404 |
| (<r2>)1/2 |
8.210 |
Jump to
S1C1
Energy calculated at B2PLYP/3-21G*
| | hartrees |
| Energy at 0K | -151.010983 |
| Energy at 298.15K | |
| HF Energy | -150.898695 |
| Nuclear repulsion energy | 62.810439 |
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 B2PLYP/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 |
2103 |
2103 |
0.00 |
32.11 |
0.42 |
0.60 |
| 2 |
Σg |
902 |
902 |
0.00 |
62.20 |
0.34 |
0.51 |
| 3 |
Σu |
1514 |
1514 |
291.34 |
0.00 |
0.33 |
0.50 |
| 4 |
Πg |
377 |
377 |
0.00 |
8.81 |
0.75 |
0.86 |
| 4 |
Πg |
198 |
198 |
0.00 |
6.61 |
0.75 |
0.86 |
| 5 |
Πu |
159 |
159 |
3.95 |
0.00 |
0.00 |
0.00 |
| 5 |
Πu |
142 |
142 |
24.25 |
0.00 |
0.75 |
0.86 |
Unscaled Zero Point Vibrational Energy (zpe) 2697.4 cm
-1
Scaled (by 1) Zero Point Vibrational Energy (zpe) 2697.4 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 B2PLYP/3-21G*
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 |
1.974 |
| C4 |
0.000 |
0.000 |
-1.974 |
Atom - Atom Distances (Å)
| |
C1 |
C2 |
C3 |
C4 |
| C1 | | 1.2929 | 1.3272 | 2.6201 |
C2 | 1.2929 | | 2.6201 | 1.3272 | C3 | 1.3272 | 2.6201 | | 3.9473 | C4 | 2.6201 | 1.3272 | 3.9473 | |
More geometry information
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at B2PLYP/3-21G*
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
-0.158 |
|
|
|
| 2 |
C |
-0.158 |
|
|
|
| 3 |
C |
0.158 |
|
|
|
| 4 |
C |
0.158 |
|
|
|
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 |
-23.872 |
0.000 |
0.000 |
| y |
0.000 |
-20.156 |
0.000 |
| z |
0.000 |
0.000 |
-32.317 |
|
| Traceless |
| | x | y | z |
| x |
2.364 |
0.000 |
0.000 |
| y |
0.000 |
7.938 |
0.000 |
| z |
0.000 |
0.000 |
-10.303 |
|
| Polar |
| 3z2-r2 | -20.606 |
| x2-y2 | -3.716 |
| 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 |
2.198 |
0.000 |
0.000 |
| y |
0.000 |
2.628 |
0.000 |
| z |
0.000 |
0.000 |
11.451 |
<r2> (average value of r
2) Å
2
| <r2> |
67.652 |
| (<r2>)1/2 |
8.225 |