Jump to
S1C2
S2C1
S2C2
Energy calculated at B97D3/6-311+G(3df,2p)
| | hartrees |
| Energy at 0K | -39.140500 |
| Energy at 298.15K | -39.140299 |
| HF Energy | -39.140500 |
| Nuclear repulsion energy | 6.129120 |
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 B97D3/6-311+G(3df,2p)
Point Group is C2v
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
0.000 |
0.000 |
0.101 |
| H2 |
0.000 |
1.004 |
-0.304 |
| H3 |
0.000 |
-1.004 |
-0.304 |
Atom - Atom Distances (Å)
| |
C1 |
H2 |
H3 |
| C1 | | 1.0826 | 1.0826 |
H2 | 1.0826 | | 2.0077 | H3 | 1.0826 | 2.0077 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| H2 |
C1 |
H3 |
136.020 |
|
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at B97D3/6-311+G(3df,2p)
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
-0.409 |
|
|
|
| 2 |
H |
0.205 |
|
|
|
| 3 |
H |
0.205 |
|
|
|
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 |
-0.607 |
0.607 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-8.304 |
0.000 |
0.000 |
| y |
0.000 |
-5.870 |
0.000 |
| z |
0.000 |
0.000 |
-7.808 |
|
| Traceless |
| | x | y | z |
| x |
-1.465 |
0.000 |
0.000 |
| y |
0.000 |
2.186 |
0.000 |
| z |
0.000 |
0.000 |
-0.721 |
|
| Polar |
| 3z2-r2 | -1.442 |
| x2-y2 | -2.434 |
| 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 |
2.175 |
0.000 |
0.000 |
| y |
0.000 |
2.296 |
0.000 |
| z |
0.000 |
0.000 |
2.042 |
<r2> (average value of r
2) Å
2
| <r2> |
6.838 |
| (<r2>)1/2 |
2.615 |
Jump to
S1C1
S2C1
S2C2
Energy calculated at B97D3/6-311+G(3df,2p)
| | hartrees |
| Energy at 0K | -39.133899 |
| Energy at 298.15K | |
| HF Energy | -39.133899 |
| Nuclear repulsion energy | 6.181068 |
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 B97D3/6-311+G(3df,2p)
| 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 |
3156 |
3115 |
0.00 |
|
|
|
| 2 |
Σu |
3491 |
3445 |
36.42 |
|
|
|
| 3 |
Πu |
874i |
862i |
102.67 |
|
|
|
| 3 |
Πu |
874i |
862i |
102.67 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 2449.8 cm
-1
Scaled (by 0.987) Zero Point Vibrational Energy (zpe) 2417.9 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 B97D3/6-311+G(3df,2p)
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 |
1.070 |
| H3 |
0.000 |
0.000 |
-1.070 |
Atom - Atom Distances (Å)
| |
C1 |
H2 |
H3 |
| C1 | | 1.0702 | 1.0702 |
H2 | 1.0702 | | 2.1403 | H3 | 1.0702 | 2.1403 | |
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 B97D3/6-311+G(3df,2p)
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
-0.510 |
|
|
|
| 2 |
H |
0.255 |
|
|
|
| 3 |
H |
0.255 |
|
|
|
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 |
-8.328 |
0.000 |
0.000 |
| y |
0.000 |
-8.328 |
0.000 |
| z |
0.000 |
0.000 |
-5.193 |
|
| Traceless |
| | x | y | z |
| x |
-1.568 |
0.000 |
0.000 |
| y |
0.000 |
-1.568 |
0.000 |
| z |
0.000 |
0.000 |
3.135 |
|
| Polar |
| 3z2-r2 | 6.270 |
| 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 |
2.252 |
0.000 |
0.000 |
| y |
0.000 |
2.252 |
0.000 |
| z |
0.000 |
0.000 |
2.277 |
<r2> (average value of r
2) Å
2
| <r2> |
6.839 |
| (<r2>)1/2 |
2.615 |
Jump to
S1C1
S1C2
S2C2
Energy calculated at B97D3/6-311+G(3df,2p)
| | hartrees |
| Energy at 0K | -39.121971 |
| Energy at 298.15K | -39.121806 |
| HF Energy | -39.121971 |
| Nuclear repulsion energy | 5.981313 |
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 B97D3/6-311+G(3df,2p)
Point Group is C2v
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
0.000 |
0.000 |
0.178 |
| H2 |
0.000 |
0.863 |
-0.534 |
| H3 |
0.000 |
-0.863 |
-0.534 |
Atom - Atom Distances (Å)
| |
C1 |
H2 |
H3 |
| C1 | | 1.1190 | 1.1190 |
H2 | 1.1190 | | 1.7260 | H3 | 1.1190 | 1.7260 | |
More geometry information
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at B97D3/6-311+G(3df,2p)
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
-0.292 |
|
|
|
| 2 |
H |
0.146 |
|
|
|
| 3 |
H |
0.146 |
|
|
|
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 |
-1.746 |
1.746 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-6.539 |
0.000 |
0.000 |
| y |
0.000 |
-7.308 |
0.000 |
| z |
0.000 |
0.000 |
-9.716 |
|
| Traceless |
| | x | y | z |
| x |
1.973 |
0.000 |
0.000 |
| y |
0.000 |
0.819 |
0.000 |
| z |
0.000 |
0.000 |
-2.792 |
|
| Polar |
| 3z2-r2 | -5.585 |
| x2-y2 | 0.769 |
| 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 |
1.944 |
0.000 |
0.000 |
| y |
0.000 |
2.555 |
0.000 |
| z |
0.000 |
0.000 |
2.790 |
<r2> (average value of r
2) Å
2
| <r2> |
7.156 |
| (<r2>)1/2 |
2.675 |
Jump to
S1C1
S1C2
S2C1
Energy calculated at B97D3/6-311+G(3df,2p)
| | hartrees |
| Energy at 0K | -39.121971 |
| Energy at 298.15K | -39.121806 |
| HF Energy | -39.121971 |
| Nuclear repulsion energy | 5.981313 |
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 B97D3/6-311+G(3df,2p)
Geometric Data calculated at B97D3/6-311+G(3df,2p)
Point Group is C2v
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability