Jump to
S1C2
S2C1
S2C2
Energy calculated at BLYP/6-31G(2df,p)
| | hartrees |
| Energy at 0K | -39.126803 |
| Energy at 298.15K | -39.126607 |
| HF Energy | -39.126803 |
| Nuclear repulsion energy | 6.102270 |
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(2df,p)
Point Group is C2v
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
0.000 |
0.000 |
0.106 |
| H2 |
0.000 |
1.002 |
-0.317 |
| H3 |
0.000 |
-1.002 |
-0.317 |
Atom - Atom Distances (Å)
| |
C1 |
H2 |
H3 |
| C1 | | 1.0877 | 1.0877 |
H2 | 1.0877 | | 2.0039 | H3 | 1.0877 | 2.0039 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| H2 |
C1 |
H3 |
134.193 |
|
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at BLYP/6-31G(2df,p)
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
-0.294 |
|
|
|
| 2 |
H |
0.147 |
|
|
|
| 3 |
H |
0.147 |
|
|
|
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 |
-0.591 |
0.591 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-7.833 |
0.000 |
0.000 |
| y |
0.000 |
-5.715 |
0.000 |
| z |
0.000 |
0.000 |
-7.410 |
|
| Traceless |
| | x | y | z |
| x |
-1.271 |
0.000 |
0.000 |
| y |
0.000 |
1.906 |
0.000 |
| z |
0.000 |
0.000 |
-0.635 |
|
| Polar |
| 3z2-r2 | -1.271 |
| x2-y2 | -2.118 |
| 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 |
1.019 |
0.000 |
0.000 |
| y |
0.000 |
1.927 |
0.000 |
| z |
0.000 |
0.000 |
1.177 |
<r2> (average value of r
2) Å
2
| <r2> |
6.640 |
| (<r2>)1/2 |
2.577 |
Jump to
S1C1
S2C1
S2C2
Energy calculated at BLYP/6-31G(2df,p)
| | hartrees |
| Energy at 0K | -39.118928 |
| Energy at 298.15K | |
| HF Energy | -39.118928 |
| Nuclear repulsion energy | 6.166016 |
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(2df,p)
| 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 |
3160 |
3143 |
0.00 |
|
|
|
| 2 |
Σu |
3507 |
3487 |
43.82 |
|
|
|
| 3 |
Πu |
917i |
912i |
99.27 |
|
|
|
| 4 |
Πu |
917i |
912i |
99.27 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 2416.6 cm
-1
Scaled (by 0.9945) Zero Point Vibrational Energy (zpe) 2403.3 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(2df,p)
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 |
1.073 |
| H3 |
0.000 |
0.000 |
-1.073 |
Atom - Atom Distances (Å)
| |
C1 |
H2 |
H3 |
| C1 | | 1.0728 | 1.0728 |
H2 | 1.0728 | | 2.1455 | H3 | 1.0728 | 2.1455 | |
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(2df,p)
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
-0.331 |
|
|
|
| 2 |
H |
0.166 |
|
|
|
| 3 |
H |
0.166 |
|
|
|
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 |
-7.821 |
0.000 |
0.000 |
| y |
0.000 |
-7.821 |
0.000 |
| z |
0.000 |
0.000 |
-4.989 |
|
| Traceless |
| | x | y | z |
| x |
-1.416 |
0.000 |
0.000 |
| y |
0.000 |
-1.416 |
0.000 |
| z |
0.000 |
0.000 |
2.832 |
|
| Polar |
| 3z2-r2 | 5.664 |
| 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 |
1.056 |
0.000 |
0.000 |
| y |
0.000 |
1.056 |
0.000 |
| z |
0.000 |
0.000 |
1.802 |
<r2> (average value of r
2) Å
2
| <r2> |
6.597 |
| (<r2>)1/2 |
2.568 |
Jump to
S1C1
S1C2
S2C2
Energy calculated at BLYP/6-31G(2df,p)
| | hartrees |
| Energy at 0K | -39.110199 |
| Energy at 298.15K | -39.110035 |
| HF Energy | -39.110199 |
| Nuclear repulsion energy | 5.933202 |
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(2df,p)
Point Group is C2v
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
0.000 |
0.000 |
0.184 |
| H2 |
0.000 |
0.857 |
-0.551 |
| H3 |
0.000 |
-0.857 |
-0.551 |
Atom - Atom Distances (Å)
| |
C1 |
H2 |
H3 |
| C1 | | 1.1290 | 1.1290 |
H2 | 1.1290 | | 1.7150 | H3 | 1.1290 | 1.7150 | |
More geometry information
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at BLYP/6-31G(2df,p)
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
-0.272 |
|
|
|
| 2 |
H |
0.136 |
|
|
|
| 3 |
H |
0.136 |
|
|
|
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 |
-1.652 |
1.652 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-6.257 |
0.000 |
0.000 |
| y |
0.000 |
-7.142 |
0.000 |
| z |
0.000 |
0.000 |
-8.883 |
|
| Traceless |
| | x | y | z |
| x |
1.755 |
0.000 |
0.000 |
| y |
0.000 |
0.428 |
0.000 |
| z |
0.000 |
0.000 |
-2.183 |
|
| Polar |
| 3z2-r2 | -4.367 |
| x2-y2 | 0.885 |
| 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 |
1.324 |
0.000 |
0.000 |
| y |
0.000 |
2.149 |
0.000 |
| z |
0.000 |
0.000 |
1.715 |
<r2> (average value of r
2) Å
2
| <r2> |
6.919 |
| (<r2>)1/2 |
2.630 |
Jump to
S1C1
S1C2
S2C1
Energy calculated at BLYP/6-31G(2df,p)
| | hartrees |
| Energy at 0K | -39.110199 |
| Energy at 298.15K | -39.110035 |
| HF Energy | -39.110199 |
| Nuclear repulsion energy | 5.933202 |
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(2df,p)
Geometric Data calculated at BLYP/6-31G(2df,p)
Point Group is C2v
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability