Jump to
S1C2
S2C1
S2C2
Energy calculated at B3PW91/STO-3G
| | hartrees |
| Energy at 0K | -38.641072 |
| Energy at 298.15K | -38.640893 |
| HF Energy | -38.641072 |
| Nuclear repulsion energy | 6.058591 |
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 B3PW91/STO-3G
Point Group is C2v
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
0.000 |
0.000 |
0.124 |
| H2 |
0.000 |
0.978 |
-0.373 |
| H3 |
0.000 |
-0.978 |
-0.373 |
Atom - Atom Distances (Å)
| |
C1 |
H2 |
H3 |
| C1 | | 1.0971 | 1.0971 |
H2 | 1.0971 | | 1.9556 | H3 | 1.0971 | 1.9556 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| H2 |
C1 |
H3 |
126.056 |
|
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at B3PW91/STO-3G
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
-0.131 |
|
|
|
| 2 |
H |
0.066 |
|
|
|
| 3 |
H |
0.066 |
|
|
|
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 |
-0.342 |
0.342 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-6.697 |
0.000 |
0.000 |
| y |
0.000 |
-5.711 |
0.000 |
| z |
0.000 |
0.000 |
-6.327 |
|
| Traceless |
| | x | y | z |
| x |
-0.678 |
0.000 |
0.000 |
| y |
0.000 |
0.801 |
0.000 |
| z |
0.000 |
0.000 |
-0.123 |
|
| Polar |
| 3z2-r2 | -0.245 |
| x2-y2 | -0.986 |
| 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 |
0.277 |
0.000 |
0.000 |
| y |
0.000 |
0.921 |
0.000 |
| z |
0.000 |
0.000 |
0.414 |
<r2> (average value of r
2) Å
2
| <r2> |
6.184 |
| (<r2>)1/2 |
2.487 |
Jump to
S1C1
S2C1
S2C2
Energy calculated at B3PW91/STO-3G
| | hartrees |
| Energy at 0K | -38.621529 |
| Energy at 298.15K | |
| HF Energy | -38.621529 |
| Nuclear repulsion energy | 6.131690 |
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 B3PW91/STO-3G
| 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 |
3415 |
3023 |
0.00 |
|
|
|
| 2 |
Σu |
3800 |
3363 |
42.15 |
|
|
|
| 3 |
Πu |
1266i |
1121i |
52.94 |
|
|
|
| 4 |
Πu |
1266i |
1121i |
52.94 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 2341.6 cm
-1
Scaled (by 0.885) Zero Point Vibrational Energy (zpe) 2072.3 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 B3PW91/STO-3G
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 |
1.079 |
| H3 |
0.000 |
0.000 |
-1.079 |
Atom - Atom Distances (Å)
| |
C1 |
H2 |
H3 |
| C1 | | 1.0788 | 1.0788 |
H2 | 1.0788 | | 2.1576 | H3 | 1.0788 | 2.1576 | |
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 B3PW91/STO-3G
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
-0.189 |
|
|
|
| 2 |
H |
0.094 |
|
|
|
| 3 |
H |
0.094 |
|
|
|
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 |
-6.663 |
0.000 |
0.000 |
| y |
0.000 |
-6.663 |
0.000 |
| z |
0.000 |
0.000 |
-4.909 |
|
| Traceless |
| | x | y | z |
| x |
-0.877 |
0.000 |
0.000 |
| y |
0.000 |
-0.877 |
0.000 |
| z |
0.000 |
0.000 |
1.754 |
|
| Polar |
| 3z2-r2 | 3.508 |
| 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 |
0.315 |
0.000 |
0.000 |
| y |
0.000 |
0.315 |
0.000 |
| z |
0.000 |
0.000 |
1.021 |
<r2> (average value of r
2) Å
2
| <r2> |
6.124 |
| (<r2>)1/2 |
2.475 |
Jump to
S1C1
S1C2
S2C2
Energy calculated at B3PW91/STO-3G
| | hartrees |
| Energy at 0K | -38.603978 |
| Energy at 298.15K | -38.603818 |
| HF Energy | -38.603978 |
| Nuclear repulsion energy | 5.811067 |
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 B3PW91/STO-3G
Point Group is C2v
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
0.000 |
0.000 |
0.191 |
| H2 |
0.000 |
0.864 |
-0.574 |
| H3 |
0.000 |
-0.864 |
-0.574 |
Atom - Atom Distances (Å)
| |
C1 |
H2 |
H3 |
| C1 | | 1.1536 | 1.1536 |
H2 | 1.1536 | | 1.7271 | H3 | 1.1536 | 1.7271 | |
More geometry information
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at B3PW91/STO-3G
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
-0.061 |
|
|
|
| 2 |
H |
0.030 |
|
|
|
| 3 |
H |
0.030 |
|
|
|
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 |
-1.488 |
1.488 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-5.528 |
0.000 |
0.000 |
| y |
0.000 |
-6.670 |
0.000 |
| z |
0.000 |
0.000 |
-7.703 |
|
| Traceless |
| | x | y | z |
| x |
1.659 |
0.000 |
0.000 |
| y |
0.000 |
-0.054 |
0.000 |
| z |
0.000 |
0.000 |
-1.604 |
|
| Polar |
| 3z2-r2 | -3.209 |
| x2-y2 | 1.142 |
| 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 |
0.790 |
0.000 |
0.000 |
| y |
0.000 |
1.014 |
0.000 |
| z |
0.000 |
0.000 |
0.594 |
<r2> (average value of r
2) Å
2
| <r2> |
6.512 |
| (<r2>)1/2 |
2.552 |
Jump to
S1C1
S1C2
S2C1
Energy calculated at B3PW91/STO-3G
| | hartrees |
| Energy at 0K | -38.603978 |
| Energy at 298.15K | -38.603818 |
| HF Energy | -38.603978 |
| Nuclear repulsion energy | 5.811067 |
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 B3PW91/STO-3G
Geometric Data calculated at B3PW91/STO-3G
Point Group is C2v
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability