Jump to
S1C2
S2C1
S2C2
Energy calculated at B3PW91/3-21G
| | hartrees |
| Energy at 0K | -38.922926 |
| Energy at 298.15K | -38.922736 |
| HF Energy | -38.922926 |
| Nuclear repulsion energy | 6.132507 |
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 B3PW91/3-21G
Point Group is C2v
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
0.000 |
0.000 |
0.109 |
| H2 |
0.000 |
0.991 |
-0.326 |
| H3 |
0.000 |
-0.991 |
-0.326 |
Atom - Atom Distances (Å)
| |
C1 |
H2 |
H3 |
| C1 | | 1.0826 | 1.0826 |
H2 | 1.0826 | | 1.9829 | H3 | 1.0826 | 1.9829 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| H2 |
C1 |
H3 |
132.638 |
|
Electronic energy levels
Electronic state
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at B3PW91/3-21G
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
-0.416 |
|
|
|
| 2 |
H |
0.208 |
|
|
|
| 3 |
H |
0.208 |
|
|
|
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 |
-0.692 |
0.692 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-7.921 |
0.000 |
0.000 |
| y |
0.000 |
-5.705 |
0.000 |
| z |
0.000 |
0.000 |
-7.459 |
|
| Traceless |
| | x | y | z |
| x |
-1.340 |
0.000 |
0.000 |
| y |
0.000 |
1.985 |
0.000 |
| z |
0.000 |
0.000 |
-0.646 |
|
| Polar |
| 3z2-r2 | -1.291 |
| x2-y2 | -2.216 |
| 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 |
0.567 |
0.000 |
0.000 |
| y |
0.000 |
1.664 |
0.000 |
| z |
0.000 |
0.000 |
0.826 |
<r2> (average value of r
2) Å
2
| <r2> |
6.639 |
| (<r2>)1/2 |
2.577 |
Jump to
S1C1
S2C1
S2C2
Energy calculated at B3PW91/3-21G
| | hartrees |
| Energy at 0K | -38.913880 |
| Energy at 298.15K | |
| HF Energy | -38.913880 |
| Nuclear repulsion energy | 6.179596 |
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 B3PW91/3-21G
| 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 |
3210 |
3086 |
0.00 |
|
|
|
| 2 |
Σu |
3555 |
3417 |
26.03 |
|
|
|
| 3 |
Πu |
951i |
914i |
148.09 |
|
|
|
| 3 |
Πu |
951i |
914i |
148.09 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 2431.6 cm
-1
Scaled (by 0.9612) Zero Point Vibrational Energy (zpe) 2337.3 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 B3PW91/3-21G
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 |
1.070 |
| H3 |
0.000 |
0.000 |
-1.070 |
Atom - Atom Distances (Å)
| |
C1 |
H2 |
H3 |
| C1 | | 1.0704 | 1.0704 |
H2 | 1.0704 | | 2.1408 | H3 | 1.0704 | 2.1408 | |
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 B3PW91/3-21G
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
-0.504 |
|
|
|
| 2 |
H |
0.252 |
|
|
|
| 3 |
H |
0.252 |
|
|
|
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 |
-7.924 |
0.000 |
0.000 |
| y |
0.000 |
-7.924 |
0.000 |
| z |
0.000 |
0.000 |
-4.772 |
|
| Traceless |
| | x | y | z |
| x |
-1.576 |
0.000 |
0.000 |
| y |
0.000 |
-1.576 |
0.000 |
| z |
0.000 |
0.000 |
3.152 |
|
| Polar |
| 3z2-r2 | 6.303 |
| 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 |
0.615 |
0.000 |
0.000 |
| y |
0.000 |
0.615 |
0.000 |
| z |
0.000 |
0.000 |
1.444 |
<r2> (average value of r
2) Å
2
| <r2> |
6.584 |
| (<r2>)1/2 |
2.566 |
Jump to
S1C1
S1C2
S2C2
Energy calculated at B3PW91/3-21G
| | hartrees |
| Energy at 0K | -38.887083 |
| Energy at 298.15K | -38.886922 |
| HF Energy | -38.887083 |
| Nuclear repulsion energy | 5.924586 |
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 B3PW91/3-21G
Point Group is C2v
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
0.000 |
0.000 |
0.180 |
| H2 |
0.000 |
0.871 |
-0.540 |
| H3 |
0.000 |
-0.871 |
-0.540 |
Atom - Atom Distances (Å)
| |
C1 |
H2 |
H3 |
| C1 | | 1.1297 | 1.1297 |
H2 | 1.1297 | | 1.7421 | H3 | 1.1297 | 1.7421 | |
More geometry information
Electronic energy levels
Electronic state
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at B3PW91/3-21G
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
-0.338 |
|
|
|
| 2 |
H |
0.169 |
|
|
|
| 3 |
H |
0.169 |
|
|
|
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 |
-2.070 |
2.070 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-6.226 |
0.000 |
0.000 |
| y |
0.000 |
-7.130 |
0.000 |
| z |
0.000 |
0.000 |
-9.198 |
|
| Traceless |
| | x | y | z |
| x |
1.938 |
0.000 |
0.000 |
| y |
0.000 |
0.582 |
0.000 |
| z |
0.000 |
0.000 |
-2.519 |
|
| Polar |
| 3z2-r2 | -5.039 |
| x2-y2 | 0.904 |
| 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 |
1.267 |
0.000 |
0.000 |
| y |
0.000 |
2.056 |
0.000 |
| z |
0.000 |
0.000 |
1.406 |
<r2> (average value of r
2) Å
2
| <r2> |
6.989 |
| (<r2>)1/2 |
2.644 |
Jump to
S1C1
S1C2
S2C1
Energy calculated at B3PW91/3-21G
| | hartrees |
| Energy at 0K | -38.887083 |
| Energy at 298.15K | -38.886922 |
| HF Energy | -38.887083 |
| Nuclear repulsion energy | 5.924586 |
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 B3PW91/3-21G
Geometric Data calculated at B3PW91/3-21G
Point Group is C2v
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability