Jump to
S1C2
S2C1
S2C2
Energy calculated at BLYP/cc-pVDZ
| | hartrees |
| Energy at 0K | -39.125989 |
| Energy at 298.15K | -39.125787 |
| HF Energy | -39.125989 |
| Nuclear repulsion energy | 6.044502 |
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 BLYP/cc-pVDZ
Point Group is C2v
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
0.000 |
0.000 |
0.105 |
| H2 |
0.000 |
1.014 |
-0.316 |
| H3 |
0.000 |
-1.014 |
-0.316 |
Atom - Atom Distances (Å)
| |
C1 |
H2 |
H3 |
| C1 | | 1.0980 | 1.0980 |
H2 | 1.0980 | | 2.0278 | H3 | 1.0980 | 2.0278 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| H2 |
C1 |
H3 |
134.870 |
|
Electronic energy levels
Electronic state
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at BLYP/cc-pVDZ
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
-0.124 |
|
|
|
| 2 |
H |
0.062 |
|
|
|
| 3 |
H |
0.062 |
|
|
|
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 |
-0.579 |
0.579 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-7.981 |
0.000 |
0.000 |
| y |
0.000 |
-5.847 |
0.000 |
| z |
0.000 |
0.000 |
-7.548 |
|
| Traceless |
| | x | y | z |
| x |
-1.284 |
0.000 |
0.000 |
| y |
0.000 |
1.917 |
0.000 |
| z |
0.000 |
0.000 |
-0.633 |
|
| Polar |
| 3z2-r2 | -1.267 |
| x2-y2 | -2.134 |
| 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 |
0.947 |
0.000 |
0.000 |
| y |
0.000 |
1.931 |
0.000 |
| z |
0.000 |
0.000 |
1.145 |
<r2> (average value of r
2) Å
2
| <r2> |
6.773 |
| (<r2>)1/2 |
2.602 |
Jump to
S1C1
S2C1
S2C2
Energy calculated at BLYP/cc-pVDZ
| | hartrees |
| Energy at 0K | -39.118795 |
| Energy at 298.15K | |
| HF Energy | -39.118795 |
| Nuclear repulsion energy | 6.103110 |
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 BLYP/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 |
3129 |
3134 |
0.00 |
|
|
|
| 2 |
Σu |
3484 |
3490 |
43.39 |
|
|
|
| 3 |
Πu |
878i |
879i |
85.32 |
|
|
|
| 3 |
Πu |
878i |
879i |
85.32 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 2428.7 cm
-1
Scaled (by 1.0016) Zero Point Vibrational Energy (zpe) 2432.6 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 BLYP/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 |
1.084 |
| H3 |
0.000 |
0.000 |
-1.084 |
Atom - Atom Distances (Å)
| |
C1 |
H2 |
H3 |
| C1 | | 1.0838 | 1.0838 |
H2 | 1.0838 | | 2.1677 | H3 | 1.0838 | 2.1677 | |
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 BLYP/cc-pVDZ
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
-0.102 |
|
|
|
| 2 |
H |
0.051 |
|
|
|
| 3 |
H |
0.051 |
|
|
|
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 |
-7.978 |
0.000 |
0.000 |
| y |
0.000 |
-7.978 |
0.000 |
| z |
0.000 |
0.000 |
-5.178 |
|
| Traceless |
| | x | y | z |
| x |
-1.400 |
0.000 |
0.000 |
| y |
0.000 |
-1.400 |
0.000 |
| z |
0.000 |
0.000 |
2.800 |
|
| Polar |
| 3z2-r2 | 5.600 |
| 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 |
0.972 |
0.000 |
0.000 |
| y |
0.000 |
0.972 |
0.000 |
| z |
0.000 |
0.000 |
1.811 |
<r2> (average value of r
2) Å
2
| <r2> |
6.749 |
| (<r2>)1/2 |
2.598 |
Jump to
S1C1
S1C2
S2C2
Energy calculated at BLYP/cc-pVDZ
| | hartrees |
| Energy at 0K | -39.108394 |
| Energy at 298.15K | -39.108229 |
| HF Energy | -39.108394 |
| Nuclear repulsion energy | 5.881443 |
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 BLYP/cc-pVDZ
Point Group is C2v
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
0.000 |
0.000 |
0.184 |
| H2 |
0.000 |
0.867 |
-0.553 |
| H3 |
0.000 |
-0.867 |
-0.553 |
Atom - Atom Distances (Å)
| |
C1 |
H2 |
H3 |
| C1 | | 1.1388 | 1.1388 |
H2 | 1.1388 | | 1.7347 | H3 | 1.1388 | 1.7347 | |
More geometry information
Electronic energy levels
Electronic state
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at BLYP/cc-pVDZ
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
-0.094 |
|
|
|
| 2 |
H |
0.047 |
|
|
|
| 3 |
H |
0.047 |
|
|
|
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 |
-1.699 |
1.699 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-6.206 |
0.000 |
0.000 |
| y |
0.000 |
-7.248 |
0.000 |
| z |
0.000 |
0.000 |
-9.128 |
|
| Traceless |
| | x | y | z |
| x |
1.982 |
0.000 |
0.000 |
| y |
0.000 |
0.419 |
0.000 |
| z |
0.000 |
0.000 |
-2.401 |
|
| Polar |
| 3z2-r2 | -4.802 |
| x2-y2 | 1.042 |
| 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 |
1.265 |
0.000 |
0.000 |
| y |
0.000 |
2.230 |
0.000 |
| z |
0.000 |
0.000 |
1.857 |
<r2> (average value of r
2) Å
2
| <r2> |
7.023 |
| (<r2>)1/2 |
2.650 |
Jump to
S1C1
S1C2
S2C1
Energy calculated at BLYP/cc-pVDZ
| | hartrees |
| Energy at 0K | -39.108394 |
| Energy at 298.15K | -39.108229 |
| HF Energy | -39.108394 |
| Nuclear repulsion energy | 5.881443 |
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 BLYP/cc-pVDZ
Geometric Data calculated at BLYP/cc-pVDZ
Point Group is C2v
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability