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S1C2
S2C1
S2C2
Energy calculated at B2PLYP/6-31G*
| | hartrees |
| Energy at 0K | -39.097000 |
| Energy at 298.15K | -39.096815 |
| HF Energy | -39.070000 |
| Nuclear repulsion energy | 6.153374 |
The energy at 298.15K was derived from the energy at 0K
and an integrated heat capacity that used the calculated vibrational frequencies.
Geometric Data calculated at B2PLYP/6-31G*
Point Group is C2v
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
0.000 |
0.000 |
0.108 |
| H2 |
0.000 |
0.988 |
-0.325 |
| H3 |
0.000 |
-0.988 |
-0.325 |
Atom - Atom Distances (Å)
| |
C1 |
H2 |
H3 |
| C1 | | 1.0789 | 1.0789 |
H2 | 1.0789 | | 1.9761 | H3 | 1.0789 | 1.9761 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| H2 |
C1 |
H3 |
132.636 |
|
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at B2PLYP/6-31G*
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
-0.351 |
|
|
|
| 2 |
H |
0.175 |
|
|
|
| 3 |
H |
0.175 |
|
|
|
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 |
-0.646 |
0.646 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-7.873 |
0.000 |
0.000 |
| y |
0.000 |
-5.767 |
0.000 |
| z |
0.000 |
0.000 |
-7.411 |
|
| Traceless |
| | x | y | z |
| x |
-1.284 |
0.000 |
0.000 |
| y |
0.000 |
1.875 |
0.000 |
| z |
0.000 |
0.000 |
-0.591 |
|
| Polar |
| 3z2-r2 | -1.182 |
| x2-y2 | -2.106 |
| 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 |
0.701 |
0.000 |
0.000 |
| y |
0.000 |
1.750 |
0.000 |
| z |
0.000 |
0.000 |
0.939 |
<r2> (average value of r
2) Å
2
| <r2> |
6.617 |
| (<r2>)1/2 |
2.572 |
Jump to
S1C1
S2C1
S2C2
Energy calculated at B2PLYP/6-31G*
| | hartrees |
| Energy at 0K | -39.086428 |
| Energy at 298.15K | |
| HF Energy | -39.059011 |
| Nuclear repulsion energy | 6.201680 |
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/6-31G*
| 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 |
3281 |
3114 |
0.00 |
|
|
|
| 2 |
Σu |
3614 |
3431 |
47.02 |
|
|
|
| 3 |
Πu |
1057i |
1003i |
129.01 |
|
|
|
| 3 |
Πu |
1057i |
1003i |
129.01 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 2390.5 cm
-1
Scaled (by 0.9492) Zero Point Vibrational Energy (zpe) 2269.1 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/6-31G*
Point Group is D∞h
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
0.000 |
0.000 |
0.000 |
| H2 |
0.000 |
0.000 |
1.067 |
| H3 |
0.000 |
0.000 |
-1.067 |
Atom - Atom Distances (Å)
| |
C1 |
H2 |
H3 |
| C1 | | 1.0666 | 1.0666 |
H2 | 1.0666 | | 2.1332 | H3 | 1.0666 | 2.1332 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| H2 |
C1 |
H3 |
180.000 |
|
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at B2PLYP/6-31G*
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
-0.419 |
|
|
|
| 2 |
H |
0.209 |
|
|
|
| 3 |
H |
0.209 |
|
|
|
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 |
-7.887 |
0.000 |
0.000 |
| y |
0.000 |
-7.887 |
0.000 |
| z |
0.000 |
0.000 |
-4.886 |
|
| Traceless |
| | x | y | z |
| x |
-1.500 |
0.000 |
0.000 |
| y |
0.000 |
-1.500 |
0.000 |
| z |
0.000 |
0.000 |
3.001 |
|
| Polar |
| 3z2-r2 | 6.002 |
| 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 |
0.741 |
0.000 |
0.000 |
| y |
0.000 |
0.741 |
0.000 |
| z |
0.000 |
0.000 |
1.555 |
<r2> (average value of r
2) Å
2
| <r2> |
6.577 |
| (<r2>)1/2 |
2.565 |
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S1C1
S1C2
S2C2
Energy calculated at B2PLYP/6-31G*
| | hartrees |
| Energy at 0K | -39.072633 |
| Energy at 298.15K | |
| HF Energy | -39.039855 |
| Nuclear repulsion energy | 6.011745 |
The energy at 298.15K was derived from the energy at 0K
and an integrated heat capacity that used the calculated vibrational frequencies.
Geometric Data calculated at B2PLYP/6-31G*
Point Group is D∞h
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Jump to
S1C1
S1C2
S2C1
Energy calculated at B2PLYP/6-31G*
| | hartrees |
| Energy at 0K | -39.072633 |
| Energy at 298.15K | |
| HF Energy | -39.039855 |
| Nuclear repulsion energy | 6.011745 |
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/6-31G*
Geometric Data calculated at B2PLYP/6-31G*
Point Group is D∞h
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability