Jump to
S1C2
S2C1
S2C2
Energy calculated at wB97X-D/cc-pVDZ
| | hartrees |
| Energy at 0K | -39.140493 |
| Energy at 298.15K | -39.140302 |
| HF Energy | -39.140493 |
| Nuclear repulsion energy | 6.129702 |
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 wB97X-D/cc-pVDZ
Point Group is C2v
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
0.000 |
0.000 |
0.109 |
| H2 |
0.000 |
0.994 |
-0.326 |
| H3 |
0.000 |
-0.994 |
-0.326 |
Atom - Atom Distances (Å)
| |
C1 |
H2 |
H3 |
| C1 | | 1.0845 | 1.0845 |
H2 | 1.0845 | | 1.9876 | H3 | 1.0845 | 1.9876 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| H2 |
C1 |
H3 |
132.803 |
|
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at wB97X-D/cc-pVDZ
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
-0.344 |
|
|
|
| 2 |
H |
0.172 |
|
|
|
| 3 |
H |
0.172 |
|
|
|
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 |
-0.739 |
0.739 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-8.393 |
0.000 |
0.000 |
| y |
0.000 |
-5.837 |
0.000 |
| z |
0.000 |
0.000 |
-7.841 |
|
| Traceless |
| | x | y | z |
| x |
-1.554 |
0.000 |
0.000 |
| y |
0.000 |
2.281 |
0.000 |
| z |
0.000 |
0.000 |
-0.727 |
|
| Polar |
| 3z2-r2 | -1.453 |
| x2-y2 | -2.556 |
| 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 |
1.356 |
0.000 |
0.000 |
| y |
0.000 |
1.858 |
0.000 |
| z |
0.000 |
0.000 |
1.324 |
<r2> (average value of r
2) Å
2
| <r2> |
6.851 |
| (<r2>)1/2 |
2.617 |
Jump to
S1C1
S2C1
S2C2
Energy calculated at wB97X-D/cc-pVDZ
| | hartrees |
| Energy at 0K | -39.132097 |
| Energy at 298.15K | |
| HF Energy | -39.132097 |
| Nuclear repulsion energy | 6.171904 |
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 wB97X-D/cc-pVDZ
| 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 |
3235 |
3082 |
0.00 |
|
|
|
| 2 |
Σu |
3565 |
3396 |
51.35 |
|
|
|
| 3 |
Πu |
965i |
919i |
167.22 |
|
|
|
| 3 |
Πu |
965i |
919i |
167.22 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 2435.2 cm
-1
Scaled (by 0.9526) Zero Point Vibrational Energy (zpe) 2319.8 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 wB97X-D/cc-pVDZ
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 |
1.072 |
| H3 |
0.000 |
0.000 |
-1.072 |
Atom - Atom Distances (Å)
| |
C1 |
H2 |
H3 |
| C1 | | 1.0724 | 1.0724 |
H2 | 1.0724 | | 2.1448 | H3 | 1.0724 | 2.1448 | |
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 wB97X-D/cc-pVDZ
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
-0.424 |
|
|
|
| 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 |
-8.459 |
0.000 |
0.000 |
| y |
0.000 |
-8.459 |
0.000 |
| z |
0.000 |
0.000 |
-5.012 |
|
| Traceless |
| | x | y | z |
| x |
-1.723 |
0.000 |
0.000 |
| y |
0.000 |
-1.723 |
0.000 |
| z |
0.000 |
0.000 |
3.446 |
|
| Polar |
| 3z2-r2 | 6.893 |
| 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 |
1.389 |
0.000 |
0.000 |
| y |
0.000 |
1.389 |
0.000 |
| z |
0.000 |
0.000 |
1.605 |
<r2> (average value of r
2) Å
2
| <r2> |
6.863 |
| (<r2>)1/2 |
2.620 |
Jump to
S1C1
S1C2
S2C2
Energy calculated at wB97X-D/cc-pVDZ
| | hartrees |
| Energy at 0K | -39.118587 |
| Energy at 298.15K | -39.118422 |
| HF Energy | -39.118587 |
| Nuclear repulsion energy | 6.013806 |
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 wB97X-D/cc-pVDZ
Point Group is C2v
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
0.000 |
0.000 |
0.148 |
| H2 |
0.000 |
0.916 |
-0.445 |
| H3 |
0.000 |
-0.916 |
-0.445 |
Atom - Atom Distances (Å)
| |
C1 |
H2 |
H3 |
| C1 | | 1.0910 | 1.0910 |
H2 | 1.0910 | | 1.8314 | H3 | 1.0910 | 1.8314 | |
More geometry information
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at wB97X-D/cc-pVDZ
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
-0.250 |
|
|
|
| 2 |
H |
0.125 |
|
|
|
| 3 |
H |
0.125 |
|
|
|
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 |
-2.191 |
2.191 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-6.435 |
0.000 |
0.000 |
| y |
0.000 |
-7.243 |
0.000 |
| z |
0.000 |
0.000 |
-9.906 |
|
| Traceless |
| | x | y | z |
| x |
2.140 |
0.000 |
0.000 |
| y |
0.000 |
0.927 |
0.000 |
| z |
0.000 |
0.000 |
-3.067 |
|
| Polar |
| 3z2-r2 | -6.134 |
| x2-y2 | 0.808 |
| 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 |
1.475 |
0.000 |
0.000 |
| y |
0.000 |
2.252 |
0.000 |
| z |
0.000 |
0.000 |
2.093 |
<r2> (average value of r
2) Å
2
| <r2> |
7.140 |
| (<r2>)1/2 |
2.672 |
Jump to
S1C1
S1C2
S2C1
Energy calculated at wB97X-D/cc-pVDZ
| | hartrees |
| Energy at 0K | -39.118587 |
| Energy at 298.15K | -39.118422 |
| HF Energy | -39.118587 |
| Nuclear repulsion energy | 6.013806 |
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 wB97X-D/cc-pVDZ
Geometric Data calculated at wB97X-D/cc-pVDZ
Point Group is C2v
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability