Jump to
S1C2
S2C1
S2C2
Energy calculated at mPW1PW91/6-311G*
| | hartrees |
| Energy at 0K | -39.149570 |
| Energy at 298.15K | -39.149379 |
| HF Energy | -39.149570 |
| Nuclear repulsion energy | 6.149890 |
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 mPW1PW91/6-311G*
Point Group is C2v
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
0.000 |
0.000 |
0.107 |
| H2 |
0.000 |
0.992 |
-0.320 |
| H3 |
0.000 |
-0.992 |
-0.320 |
Atom - Atom Distances (Å)
| |
C1 |
H2 |
H3 |
| C1 | | 1.0794 | 1.0794 |
H2 | 1.0794 | | 1.9835 | H3 | 1.0794 | 1.9835 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| H2 |
C1 |
H3 |
133.508 |
|
Electronic energy levels
Electronic state
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at mPW1PW91/6-311G*
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
-0.473 |
|
|
|
| 2 |
H |
0.236 |
|
|
|
| 3 |
H |
0.236 |
|
|
|
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 |
-0.675 |
0.675 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-8.141 |
0.000 |
0.000 |
| y |
0.000 |
-5.741 |
0.000 |
| z |
0.000 |
0.000 |
-7.632 |
|
| Traceless |
| | x | y | z |
| x |
-1.454 |
0.000 |
0.000 |
| y |
0.000 |
2.145 |
0.000 |
| z |
0.000 |
0.000 |
-0.691 |
|
| Polar |
| 3z2-r2 | -1.382 |
| x2-y2 | -2.399 |
| 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 |
1.010 |
0.000 |
0.000 |
| y |
0.000 |
1.801 |
0.000 |
| z |
0.000 |
0.000 |
1.152 |
<r2> (average value of r
2) Å
2
| <r2> |
6.718 |
| (<r2>)1/2 |
2.592 |
Jump to
S1C1
S2C1
S2C2
Energy calculated at mPW1PW91/6-311G*
| | hartrees |
| Energy at 0K | -39.141588 |
| Energy at 298.15K | |
| HF Energy | -39.141588 |
| Nuclear repulsion energy | 6.195002 |
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 mPW1PW91/6-311G*
| 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 |
3231 |
3084 |
0.00 |
|
|
|
| 2 |
Σu |
3570 |
3407 |
43.51 |
|
|
|
| 3 |
Πu |
953i |
910i |
130.35 |
|
|
|
| 3 |
Πu |
953i |
910i |
130.35 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 2447.2 cm
-1
Scaled (by 0.9544) Zero Point Vibrational Energy (zpe) 2335.6 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 mPW1PW91/6-311G*
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 |
1.068 |
| H3 |
0.000 |
0.000 |
-1.068 |
Atom - Atom Distances (Å)
| |
C1 |
H2 |
H3 |
| C1 | | 1.0678 | 1.0678 |
H2 | 1.0678 | | 2.1355 | H3 | 1.0678 | 2.1355 | |
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 mPW1PW91/6-311G*
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
-0.535 |
|
|
|
| 2 |
H |
0.268 |
|
|
|
| 3 |
H |
0.268 |
|
|
|
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 |
-8.168 |
0.000 |
0.000 |
| y |
0.000 |
-8.168 |
0.000 |
| z |
0.000 |
0.000 |
-4.903 |
|
| Traceless |
| | x | y | z |
| x |
-1.633 |
0.000 |
0.000 |
| y |
0.000 |
-1.633 |
0.000 |
| z |
0.000 |
0.000 |
3.265 |
|
| Polar |
| 3z2-r2 | 6.530 |
| 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 |
1.060 |
0.000 |
0.000 |
| y |
0.000 |
1.060 |
0.000 |
| z |
0.000 |
0.000 |
1.592 |
<r2> (average value of r
2) Å
2
| <r2> |
6.702 |
| (<r2>)1/2 |
2.589 |
Jump to
S1C1
S1C2
S2C2
Energy calculated at mPW1PW91/6-311G*
| | hartrees |
| Energy at 0K | -39.121158 |
| Energy at 298.15K | -39.120995 |
| HF Energy | -39.121158 |
| Nuclear repulsion energy | 6.010914 |
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 mPW1PW91/6-311G*
Point Group is C2v
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
0.000 |
0.000 |
0.177 |
| H2 |
0.000 |
0.860 |
-0.531 |
| H3 |
0.000 |
-0.860 |
-0.531 |
Atom - Atom Distances (Å)
| |
C1 |
H2 |
H3 |
| C1 | | 1.1134 | 1.1134 |
H2 | 1.1134 | | 1.7195 | H3 | 1.1134 | 1.7195 | |
More geometry information
Electronic energy levels
Electronic state
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at mPW1PW91/6-311G*
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
-0.404 |
|
|
|
| 2 |
H |
0.202 |
|
|
|
| 3 |
H |
0.202 |
|
|
|
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 |
-2.012 |
2.012 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-6.285 |
0.000 |
0.000 |
| y |
0.000 |
-7.117 |
0.000 |
| z |
0.000 |
0.000 |
-9.371 |
|
| Traceless |
| | x | y | z |
| x |
1.959 |
0.000 |
0.000 |
| y |
0.000 |
0.711 |
0.000 |
| z |
0.000 |
0.000 |
-2.670 |
|
| Polar |
| 3z2-r2 | -5.339 |
| x2-y2 | 0.832 |
| 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 |
1.291 |
0.000 |
0.000 |
| y |
0.000 |
2.148 |
0.000 |
| z |
0.000 |
0.000 |
1.747 |
<r2> (average value of r
2) Å
2
| <r2> |
6.970 |
| (<r2>)1/2 |
2.640 |
Jump to
S1C1
S1C2
S2C1
Energy calculated at mPW1PW91/6-311G*
| | hartrees |
| Energy at 0K | -39.121158 |
| Energy at 298.15K | -39.120995 |
| HF Energy | -39.121158 |
| Nuclear repulsion energy | 6.010914 |
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 mPW1PW91/6-311G*
Geometric Data calculated at mPW1PW91/6-311G*
Point Group is C2v
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability