Jump to
S1C2
S2C1
S2C2
Energy calculated at BLYP/6-31G**
| | hartrees |
| Energy at 0K | -39.126349 |
| Energy at 298.15K | -39.126155 |
| HF Energy | -39.126349 |
| Nuclear repulsion energy | 6.096280 |
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/6-31G**
Point Group is C2v
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
0.000 |
0.000 |
0.107 |
| H2 |
0.000 |
1.001 |
-0.322 |
| H3 |
0.000 |
-1.001 |
-0.322 |
Atom - Atom Distances (Å)
| |
C1 |
H2 |
H3 |
| C1 | | 1.0889 | 1.0889 |
H2 | 1.0889 | | 2.0017 | H3 | 1.0889 | 2.0017 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| H2 |
C1 |
H3 |
133.618 |
|
Electronic energy levels
Electronic state
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at BLYP/6-31G**
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
-0.240 |
|
|
|
| 2 |
H |
0.120 |
|
|
|
| 3 |
H |
0.120 |
|
|
|
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 |
-0.618 |
0.618 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-7.826 |
0.000 |
0.000 |
| y |
0.000 |
-5.754 |
0.000 |
| z |
0.000 |
0.000 |
-7.397 |
|
| Traceless |
| | x | y | z |
| x |
-1.250 |
0.000 |
0.000 |
| y |
0.000 |
1.857 |
0.000 |
| z |
0.000 |
0.000 |
-0.607 |
|
| Polar |
| 3z2-r2 | -1.214 |
| x2-y2 | -2.072 |
| 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 |
0.762 |
0.000 |
0.000 |
| y |
0.000 |
1.856 |
0.000 |
| z |
0.000 |
0.000 |
0.995 |
<r2> (average value of r
2) Å
2
| <r2> |
6.646 |
| (<r2>)1/2 |
2.578 |
Jump to
S1C1
S2C1
S2C2
Energy calculated at BLYP/6-31G**
| | hartrees |
| Energy at 0K | -39.118043 |
| Energy at 298.15K | |
| HF Energy | -39.118043 |
| Nuclear repulsion energy | 6.153222 |
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/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 |
3167 |
3143 |
0.00 |
|
|
|
| 2 |
Σu |
3503 |
3476 |
32.62 |
|
|
|
| 3 |
Πu |
933i |
926i |
105.95 |
|
|
|
| 3 |
Πu |
933i |
926i |
105.95 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 2402.3 cm
-1
Scaled (by 0.9923) Zero Point Vibrational Energy (zpe) 2383.8 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 BLYP/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 |
1.075 |
| H3 |
0.000 |
0.000 |
-1.075 |
Atom - Atom Distances (Å)
| |
C1 |
H2 |
H3 |
| C1 | | 1.0750 | 1.0750 |
H2 | 1.0750 | | 2.1500 | H3 | 1.0750 | 2.1500 | |
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/6-31G**
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
-0.257 |
|
|
|
| 2 |
H |
0.128 |
|
|
|
| 3 |
H |
0.128 |
|
|
|
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 |
-7.817 |
0.000 |
0.000 |
| y |
0.000 |
-7.817 |
0.000 |
| z |
0.000 |
0.000 |
-5.001 |
|
| Traceless |
| | x | y | z |
| x |
-1.408 |
0.000 |
0.000 |
| y |
0.000 |
-1.408 |
0.000 |
| z |
0.000 |
0.000 |
2.816 |
|
| Polar |
| 3z2-r2 | 5.632 |
| 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 |
0.796 |
0.000 |
0.000 |
| y |
0.000 |
0.796 |
0.000 |
| z |
0.000 |
0.000 |
1.675 |
<r2> (average value of r
2) Å
2
| <r2> |
6.607 |
| (<r2>)1/2 |
2.570 |
Jump to
S1C1
S1C2
S2C2
Energy calculated at BLYP/6-31G**
| | hartrees |
| Energy at 0K | -39.107057 |
| Energy at 298.15K | -39.106893 |
| HF Energy | -39.107057 |
| Nuclear repulsion energy | 5.922545 |
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/6-31G**
Point Group is C2v
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
0.000 |
0.000 |
0.184 |
| H2 |
0.000 |
0.859 |
-0.552 |
| H3 |
0.000 |
-0.859 |
-0.552 |
Atom - Atom Distances (Å)
| |
C1 |
H2 |
H3 |
| C1 | | 1.1310 | 1.1310 |
H2 | 1.1310 | | 1.7180 | H3 | 1.1310 | 1.7180 | |
More geometry information
Electronic energy levels
Electronic state
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at BLYP/6-31G**
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
-0.185 |
|
|
|
| 2 |
H |
0.092 |
|
|
|
| 3 |
H |
0.092 |
|
|
|
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 |
-1.743 |
1.743 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-6.154 |
0.000 |
0.000 |
| y |
0.000 |
-7.193 |
0.000 |
| z |
0.000 |
0.000 |
-9.000 |
|
| Traceless |
| | x | y | z |
| x |
1.942 |
0.000 |
0.000 |
| y |
0.000 |
0.384 |
0.000 |
| z |
0.000 |
0.000 |
-2.326 |
|
| Polar |
| 3z2-r2 | -4.653 |
| x2-y2 | 1.039 |
| 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 |
1.209 |
0.000 |
0.000 |
| y |
0.000 |
2.137 |
0.000 |
| z |
0.000 |
0.000 |
1.638 |
<r2> (average value of r
2) Å
2
| <r2> |
6.940 |
| (<r2>)1/2 |
2.634 |
Jump to
S1C1
S1C2
S2C1
Energy calculated at BLYP/6-31G**
| | hartrees |
| Energy at 0K | -39.107057 |
| Energy at 298.15K | -39.106893 |
| HF Energy | -39.107057 |
| Nuclear repulsion energy | 5.922545 |
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/6-31G**
Geometric Data calculated at BLYP/6-31G**
Point Group is C2v
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability