Jump to
S1C2
S2C1
S2C2
Energy calculated at B3PW91/6-31G*
| | hartrees |
| Energy at 0K | -39.136888 |
| Energy at 298.15K | -39.136698 |
| HF Energy | -39.136888 |
| Nuclear repulsion energy | 6.138123 |
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 B3PW91/6-31G*
Point Group is C2v
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
0.000 |
0.000 |
0.108 |
| H2 |
0.000 |
0.992 |
-0.323 |
| H3 |
0.000 |
-0.992 |
-0.323 |
Atom - Atom Distances (Å)
| |
C1 |
H2 |
H3 |
| C1 | | 1.0815 | 1.0815 |
H2 | 1.0815 | | 1.9843 | H3 | 1.0815 | 1.9843 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| H2 |
C1 |
H3 |
133.085 |
|
Electronic energy levels
Electronic state
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at B3PW91/6-31G*
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
-0.368 |
|
|
|
| 2 |
H |
0.184 |
|
|
|
| 3 |
H |
0.184 |
|
|
|
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 |
-0.649 |
0.649 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
0.000 |
0.000 |
-0.707 |
0.707 |
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-7.857 |
0.000 |
0.000 |
| y |
0.000 |
-5.673 |
0.000 |
| z |
0.000 |
0.000 |
-7.398 |
|
| Traceless |
| | x | y | z |
| x |
-1.322 |
0.000 |
0.000 |
| y |
0.000 |
1.954 |
0.000 |
| z |
0.000 |
0.000 |
-0.633 |
|
| Polar |
| 3z2-r2 | -1.265 |
| x2-y2 | -2.184 |
| 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 |
0.722 |
0.000 |
0.000 |
| y |
0.000 |
1.768 |
0.000 |
| z |
0.000 |
0.000 |
0.955 |
<r2> (average value of r
2) Å
2
| <r2> |
6.604 |
| (<r2>)1/2 |
2.570 |
Jump to
S1C1
S2C1
S2C2
Energy calculated at B3PW91/6-31G*
| | hartrees |
| Energy at 0K | -39.127662 |
| Energy at 298.15K | |
| HF Energy | -39.127662 |
| Nuclear repulsion energy | 6.183636 |
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 B3PW91/6-31G*
| 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 |
3257 |
3116 |
0.00 |
|
|
|
| 2 |
Σu |
3585 |
3430 |
39.24 |
|
|
|
| 3 |
Πu |
979i |
936i |
122.96 |
|
|
|
| 3 |
Πu |
979i |
936i |
122.96 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 2442.7 cm
-1
Scaled (by 0.9567) Zero Point Vibrational Energy (zpe) 2336.9 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 B3PW91/6-31G*
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 |
1.070 |
| H3 |
0.000 |
0.000 |
-1.070 |
Atom - Atom Distances (Å)
| |
C1 |
H2 |
H3 |
| C1 | | 1.0697 | 1.0697 |
H2 | 1.0697 | | 2.1394 | H3 | 1.0697 | 2.1394 | |
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 B3PW91/6-31G*
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
-0.425 |
|
|
|
| 2 |
H |
0.212 |
|
|
|
| 3 |
H |
0.212 |
|
|
|
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 |
-7.866 |
0.000 |
0.000 |
| y |
0.000 |
-7.866 |
0.000 |
| z |
0.000 |
0.000 |
-4.831 |
|
| Traceless |
| | x | y | z |
| x |
-1.518 |
0.000 |
0.000 |
| y |
0.000 |
-1.518 |
0.000 |
| z |
0.000 |
0.000 |
3.035 |
|
| Polar |
| 3z2-r2 | 6.070 |
| 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 |
0.764 |
0.000 |
0.000 |
| y |
0.000 |
0.764 |
0.000 |
| z |
0.000 |
0.000 |
1.571 |
<r2> (average value of r
2) Å
2
| <r2> |
6.570 |
| (<r2>)1/2 |
2.563 |
Jump to
S1C1
S1C2
S2C2
Energy calculated at B3PW91/6-31G*
| | hartrees |
| Energy at 0K | -39.107148 |
| Energy at 298.15K | -39.106986 |
| HF Energy | -39.107148 |
| Nuclear repulsion energy | 5.980550 |
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 B3PW91/6-31G*
Point Group is C2v
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
0.000 |
0.000 |
0.179 |
| H2 |
0.000 |
0.860 |
-0.538 |
| H3 |
0.000 |
-0.860 |
-0.538 |
Atom - Atom Distances (Å)
| |
C1 |
H2 |
H3 |
| C1 | | 1.1194 | 1.1194 |
H2 | 1.1194 | | 1.7192 | H3 | 1.1194 | 1.7192 | |
More geometry information
Electronic energy levels
Electronic state
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at B3PW91/6-31G*
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
-0.300 |
|
|
|
| 2 |
H |
0.150 |
|
|
|
| 3 |
H |
0.150 |
|
|
|
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 |
-1.916 |
1.916 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-6.141 |
0.000 |
0.000 |
| y |
0.000 |
-7.062 |
0.000 |
| z |
0.000 |
0.000 |
-9.055 |
|
| Traceless |
| | x | y | z |
| x |
1.917 |
0.000 |
0.000 |
| y |
0.000 |
0.536 |
0.000 |
| z |
0.000 |
0.000 |
-2.453 |
|
| Polar |
| 3z2-r2 | -4.907 |
| x2-y2 | 0.920 |
| 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 |
1.214 |
0.000 |
0.000 |
| y |
0.000 |
2.087 |
0.000 |
| z |
0.000 |
0.000 |
1.526 |
<r2> (average value of r
2) Å
2
| <r2> |
6.883 |
| (<r2>)1/2 |
2.624 |
Jump to
S1C1
S1C2
S2C1
Energy calculated at B3PW91/6-31G*
| | hartrees |
| Energy at 0K | -39.107148 |
| Energy at 298.15K | -39.106986 |
| HF Energy | -39.107148 |
| Nuclear repulsion energy | 5.980550 |
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 B3PW91/6-31G*
Geometric Data calculated at B3PW91/6-31G*
Point Group is C2v
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability