Jump to
S1C2
S2C1
S2C2
Energy calculated at mPW1PW91/3-21G*
| | hartrees |
| Energy at 0K | -38.926908 |
| Energy at 298.15K | -38.926719 |
| HF Energy | -38.926908 |
| Nuclear repulsion energy | 6.143699 |
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 mPW1PW91/3-21G*
Point Group is C2v
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
0.000 |
0.000 |
0.108 |
| H2 |
0.000 |
0.990 |
-0.325 |
| H3 |
0.000 |
-0.990 |
-0.325 |
Atom - Atom Distances (Å)
| |
C1 |
H2 |
H3 |
| C1 | | 1.0806 | 1.0806 |
H2 | 1.0806 | | 1.9796 | H3 | 1.0806 | 1.9796 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| H2 |
C1 |
H3 |
132.681 |
|
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at mPW1PW91/3-21G*
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
-0.420 |
|
|
|
| 2 |
H |
0.210 |
|
|
|
| 3 |
H |
0.210 |
|
|
|
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 |
-0.690 |
0.690 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-7.922 |
0.000 |
0.000 |
| y |
0.000 |
-5.705 |
0.000 |
| z |
0.000 |
0.000 |
-7.460 |
|
| Traceless |
| | x | y | z |
| x |
-1.340 |
0.000 |
0.000 |
| y |
0.000 |
1.986 |
0.000 |
| z |
0.000 |
0.000 |
-0.647 |
|
| Polar |
| 3z2-r2 | -1.293 |
| x2-y2 | -2.217 |
| 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 |
0.563 |
0.000 |
0.000 |
| y |
0.000 |
1.648 |
0.000 |
| z |
0.000 |
0.000 |
0.819 |
<r2> (average value of r
2) Å
2
| <r2> |
6.632 |
| (<r2>)1/2 |
2.575 |
Jump to
S1C1
S2C1
S2C2
Energy calculated at mPW1PW91/3-21G*
| | hartrees |
| Energy at 0K | -38.917769 |
| Energy at 298.15K | |
| HF Energy | -38.917769 |
| Nuclear repulsion energy | 6.188666 |
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 mPW1PW91/3-21G*
| 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 |
3227 |
3065 |
0.00 |
|
|
|
| 2 |
Σu |
3572 |
3392 |
27.67 |
|
|
|
| 3 |
Πu |
958i |
910i |
148.42 |
|
|
|
| 3 |
Πu |
958i |
910i |
148.42 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 2442.1 cm
-1
Scaled (by 0.9496) Zero Point Vibrational Energy (zpe) 2319.1 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 mPW1PW91/3-21G*
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 |
1.069 |
| H3 |
0.000 |
0.000 |
-1.069 |
Atom - Atom Distances (Å)
| |
C1 |
H2 |
H3 |
| C1 | | 1.0688 | 1.0688 |
H2 | 1.0688 | | 2.1377 | H3 | 1.0688 | 2.1377 | |
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 mPW1PW91/3-21G*
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
-0.511 |
|
|
|
| 2 |
H |
0.256 |
|
|
|
| 3 |
H |
0.256 |
|
|
|
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 |
-7.927 |
0.000 |
0.000 |
| y |
0.000 |
-7.927 |
0.000 |
| z |
0.000 |
0.000 |
-4.769 |
|
| Traceless |
| | x | y | z |
| x |
-1.579 |
0.000 |
0.000 |
| y |
0.000 |
-1.579 |
0.000 |
| z |
0.000 |
0.000 |
3.158 |
|
| Polar |
| 3z2-r2 | 6.316 |
| 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 |
0.610 |
0.000 |
0.000 |
| y |
0.000 |
0.610 |
0.000 |
| z |
0.000 |
0.000 |
1.431 |
<r2> (average value of r
2) Å
2
| <r2> |
6.578 |
| (<r2>)1/2 |
2.565 |
Jump to
S1C1
S1C2
S2C2
Energy calculated at mPW1PW91/3-21G*
| | hartrees |
| Energy at 0K | -38.889150 |
| Energy at 298.15K | -38.888989 |
| HF Energy | -38.889150 |
| Nuclear repulsion energy | 5.940914 |
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 mPW1PW91/3-21G*
Point Group is C2v
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
0.000 |
0.000 |
0.179 |
| H2 |
0.000 |
0.871 |
-0.536 |
| H3 |
0.000 |
-0.871 |
-0.536 |
Atom - Atom Distances (Å)
| |
C1 |
H2 |
H3 |
| C1 | | 1.1265 | 1.1265 |
H2 | 1.1265 | | 1.7410 | H3 | 1.1265 | 1.7410 | |
More geometry information
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at mPW1PW91/3-21G*
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
-0.343 |
|
|
|
| 2 |
H |
0.171 |
|
|
|
| 3 |
H |
0.171 |
|
|
|
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 |
-2.092 |
2.092 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-6.220 |
0.000 |
0.000 |
| y |
0.000 |
-7.111 |
0.000 |
| z |
0.000 |
0.000 |
-9.209 |
|
| Traceless |
| | x | y | z |
| x |
1.940 |
0.000 |
0.000 |
| y |
0.000 |
0.603 |
0.000 |
| z |
0.000 |
0.000 |
-2.544 |
|
| Polar |
| 3z2-r2 | -5.088 |
| x2-y2 | 0.891 |
| 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 |
1.272 |
0.000 |
0.000 |
| y |
0.000 |
2.039 |
0.000 |
| z |
0.000 |
0.000 |
1.380 |
<r2> (average value of r
2) Å
2
| <r2> |
6.975 |
| (<r2>)1/2 |
2.641 |
Jump to
S1C1
S1C2
S2C1
Energy calculated at mPW1PW91/3-21G*
| | hartrees |
| Energy at 0K | -38.889150 |
| Energy at 298.15K | -38.888989 |
| HF Energy | -38.889150 |
| Nuclear repulsion energy | 5.940914 |
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 mPW1PW91/3-21G*
Geometric Data calculated at mPW1PW91/3-21G*
Point Group is C2v
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability