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S1C2
S2C1
S2C2
Energy calculated at HF/6-311G**
| | hartrees |
| Energy at 0K | -38.934072 |
| Energy at 298.15K | -38.933895 |
| HF Energy | -38.934072 |
| Nuclear repulsion energy | 6.192906 |
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 HF/6-311G**
Point Group is C2v
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
0.000 |
0.000 |
0.110 |
| H2 |
0.000 |
0.978 |
-0.329 |
| H3 |
0.000 |
-0.978 |
-0.329 |
Atom - Atom Distances (Å)
| |
C1 |
H2 |
H3 |
| C1 | | 1.0722 | 1.0722 |
H2 | 1.0722 | | 1.9566 | H3 | 1.0722 | 1.9566 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| H2 |
C1 |
H3 |
131.685 |
|
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at HF/6-311G**
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
-0.253 |
|
|
|
| 2 |
H |
0.126 |
|
|
|
| 3 |
H |
0.126 |
|
|
|
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 |
-0.592 |
0.592 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-8.025 |
0.000 |
0.000 |
| y |
0.000 |
-5.922 |
0.000 |
| z |
0.000 |
0.000 |
-7.516 |
|
| Traceless |
| | x | y | z |
| x |
-1.305 |
0.000 |
0.000 |
| y |
0.000 |
1.848 |
0.000 |
| z |
0.000 |
0.000 |
-0.543 |
|
| Polar |
| 3z2-r2 | -1.086 |
| x2-y2 | -2.102 |
| 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 |
1.000 |
0.000 |
0.000 |
| y |
0.000 |
1.761 |
0.000 |
| z |
0.000 |
0.000 |
1.138 |
<r2> (average value of r
2) Å
2
| <r2> |
6.672 |
| (<r2>)1/2 |
2.583 |
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S1C1
S2C1
S2C2
Energy calculated at HF/6-311G**
| | hartrees |
| Energy at 0K | -38.922027 |
| Energy at 298.15K | |
| HF Energy | -38.922027 |
| Nuclear repulsion energy | 6.229148 |
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/6-311G**
| 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 |
3298 |
2996 |
0.00 |
|
|
|
| 2 |
Σu |
3639 |
3306 |
56.30 |
|
|
|
| 3 |
Πu |
1117i |
1015i |
109.15 |
|
|
|
| 4 |
Πu |
1117i |
1015i |
109.15 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 2351.8 cm
-1
Scaled (by 0.9085) Zero Point Vibrational Energy (zpe) 2136.6 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/6-311G**
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 |
1.062 |
| H3 |
0.000 |
0.000 |
-1.062 |
Atom - Atom Distances (Å)
| |
C1 |
H2 |
H3 |
| C1 | | 1.0619 | 1.0619 |
H2 | 1.0619 | | 2.1238 | H3 | 1.0619 | 2.1238 | |
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 HF/6-311G**
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
-0.352 |
|
|
|
| 2 |
H |
0.176 |
|
|
|
| 3 |
H |
0.176 |
|
|
|
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 |
-8.080 |
0.000 |
0.000 |
| y |
0.000 |
-8.080 |
0.000 |
| z |
0.000 |
0.000 |
-5.016 |
|
| Traceless |
| | x | y | z |
| x |
-1.532 |
0.000 |
0.000 |
| y |
0.000 |
-1.532 |
0.000 |
| z |
0.000 |
0.000 |
3.065 |
|
| Polar |
| 3z2-r2 | 6.129 |
| 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 |
1.048 |
0.000 |
0.000 |
| y |
0.000 |
1.048 |
0.000 |
| z |
0.000 |
0.000 |
1.584 |
<r2> (average value of r
2) Å
2
| <r2> |
6.664 |
| (<r2>)1/2 |
2.582 |
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S1C1
S1C2
S2C2
Energy calculated at HF/6-311G**
| | hartrees |
| Energy at 0K | -38.887511 |
| Energy at 298.15K | -38.887351 |
| HF Energy | -38.887511 |
| Nuclear repulsion energy | 6.085165 |
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 HF/6-311G**
Point Group is C2v
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
0.000 |
0.000 |
0.170 |
| H2 |
0.000 |
0.862 |
-0.511 |
| H3 |
0.000 |
-0.862 |
-0.511 |
Atom - Atom Distances (Å)
| |
C1 |
H2 |
H3 |
| C1 | | 1.0990 | 1.0990 |
H2 | 1.0990 | | 1.7236 | H3 | 1.0990 | 1.7236 | |
More geometry information
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at HF/6-311G**
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
-0.179 |
|
|
|
| 2 |
H |
0.090 |
|
|
|
| 3 |
H |
0.090 |
|
|
|
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 |
-2.038 |
2.038 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-6.180 |
0.000 |
0.000 |
| y |
0.000 |
-7.070 |
0.000 |
| z |
0.000 |
0.000 |
-9.475 |
|
| Traceless |
| | x | y | z |
| x |
2.093 |
0.000 |
0.000 |
| y |
0.000 |
0.757 |
0.000 |
| z |
0.000 |
0.000 |
-2.850 |
|
| Polar |
| 3z2-r2 | -5.699 |
| x2-y2 | 0.890 |
| 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 |
1.337 |
0.000 |
0.000 |
| y |
0.000 |
2.064 |
0.000 |
| z |
0.000 |
0.000 |
1.620 |
<r2> (average value of r
2) Å
2
| <r2> |
6.914 |
| (<r2>)1/2 |
2.630 |
Jump to
S1C1
S1C2
S2C1
Energy calculated at HF/6-311G**
| | hartrees |
| Energy at 0K | -38.887511 |
| Energy at 298.15K | -38.887351 |
| HF Energy | -38.887511 |
| Nuclear repulsion energy | 6.085165 |
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/6-311G**
Geometric Data calculated at HF/6-311G**
Point Group is C2v
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability