Jump to
S2C1
Energy calculated at B2PLYP/6-311G**
| | hartrees |
| Energy at 0K | -151.969224 |
| Energy at 298.15K | |
| HF Energy | -151.817929 |
| Nuclear repulsion energy | 63.276190 |
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/6-311G**
| 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 |
50.18 |
0.57 |
0.73 |
| 2 |
Σg |
931 |
931 |
0.00 |
71.71 |
0.40 |
0.57 |
| 3 |
Σu |
1578 |
1578 |
311.23 |
0.00 |
0.33 |
0.50 |
| 4 |
Πg |
345 |
345 |
0.00 |
3.61 |
0.75 |
0.86 |
| 4 |
Πg |
345 |
345 |
0.00 |
3.61 |
0.75 |
0.86 |
| 5 |
Πu |
172 |
172 |
21.94 |
0.00 |
0.75 |
0.86 |
| 5 |
Πu |
172 |
172 |
21.94 |
0.00 |
0.00 |
0.00 |
Unscaled Zero Point Vibrational Energy (zpe) 2831.1 cm
-1
Scaled (by 1) Zero Point Vibrational Energy (zpe) 2831.1 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 B2PLYP/6-311G**
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 |
1.958 |
| C4 |
0.000 |
0.000 |
-1.958 |
Atom - Atom Distances (Å)
| |
C1 |
C2 |
C3 |
C4 |
| C1 | | 1.2924 | 1.3119 | 2.6043 |
C2 | 1.2924 | | 2.6043 | 1.3119 | C3 | 1.3119 | 2.6043 | | 3.9163 | C4 | 2.6043 | 1.3119 | 3.9163 | |
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/6-311G**
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
0.063 |
|
|
|
| 2 |
C |
0.063 |
|
|
|
| 3 |
C |
-0.063 |
|
|
|
| 4 |
C |
-0.063 |
|
|
|
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 |
-22.002 |
0.000 |
0.000 |
| y |
0.000 |
-22.002 |
0.000 |
| z |
0.000 |
0.000 |
-33.039 |
|
| Traceless |
| | x | y | z |
| x |
5.519 |
0.000 |
0.000 |
| y |
0.000 |
5.519 |
0.000 |
| z |
0.000 |
0.000 |
-11.037 |
|
| Polar |
| 3z2-r2 | -22.075 |
| 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 |
3.290 |
0.000 |
0.000 |
| y |
0.000 |
3.290 |
0.000 |
| z |
0.000 |
0.000 |
12.742 |
<r2> (average value of r
2) Å
2
| <r2> |
67.062 |
| (<r2>)1/2 |
8.189 |
Jump to
S1C1
Energy calculated at B2PLYP/6-311G**
| | hartrees |
| Energy at 0K | -151.945895 |
| Energy at 298.15K | |
| HF Energy | -151.783104 |
| Nuclear repulsion energy | 63.088292 |
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/6-311G**
| 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 |
2100 |
2100 |
0.00 |
57.00 |
0.41 |
0.58 |
| 2 |
Σg |
920 |
920 |
0.00 |
70.48 |
0.33 |
0.50 |
| 3 |
Σu |
1583 |
1583 |
351.97 |
0.00 |
0.75 |
0.86 |
| 4 |
Πg |
427 |
427 |
0.00 |
33.47 |
0.75 |
0.86 |
| 4 |
Πg |
293 |
293 |
0.00 |
6.77 |
0.75 |
0.86 |
| 5 |
Πu |
204 |
204 |
6.74 |
0.00 |
0.74 |
0.85 |
| 5 |
Πu |
150 |
150 |
34.94 |
0.00 |
0.75 |
0.86 |
Unscaled Zero Point Vibrational Energy (zpe) 2838.4 cm
-1
Scaled (by 1) Zero Point Vibrational Energy (zpe) 2838.4 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/6-311G**
Point Group is D∞h
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
0.000 |
0.000 |
0.649 |
| C2 |
0.000 |
0.000 |
-0.649 |
| C3 |
0.000 |
0.000 |
1.964 |
| C4 |
0.000 |
0.000 |
-1.964 |
Atom - Atom Distances (Å)
| |
C1 |
C2 |
C3 |
C4 |
| C1 | | 1.2980 | 1.3148 | 2.6128 |
C2 | 1.2980 | | 2.6128 | 1.3148 | C3 | 1.3148 | 2.6128 | | 3.9276 | C4 | 2.6128 | 1.3148 | 3.9276 | |
More geometry information
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at B2PLYP/6-311G**
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
0.067 |
|
|
|
| 2 |
C |
0.067 |
|
|
|
| 3 |
C |
-0.067 |
|
|
|
| 4 |
C |
-0.067 |
|
|
|
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 |
-20.212 |
0.000 |
0.000 |
| y |
0.000 |
-23.906 |
0.000 |
| z |
0.000 |
0.000 |
-33.021 |
|
| Traceless |
| | x | y | z |
| x |
8.251 |
0.000 |
0.000 |
| y |
0.000 |
2.710 |
0.000 |
| z |
0.000 |
0.000 |
-10.961 |
|
| Polar |
| 3z2-r2 | -21.923 |
| x2-y2 | 3.694 |
| 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 |
3.233 |
0.000 |
0.000 |
| y |
0.000 |
2.981 |
0.000 |
| z |
0.000 |
0.000 |
12.427 |
<r2> (average value of r
2) Å
2
| <r2> |
67.392 |
| (<r2>)1/2 |
8.209 |