Jump to
S1C2
S2C1
S2C2
Energy calculated at HF/aug-cc-pVQZ
| | hartrees |
| Energy at 0K | -38.940444 |
| Energy at 298.15K | -38.940267 |
| HF Energy | -38.940444 |
| Nuclear repulsion energy | 6.209701 |
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 HF/aug-cc-pVQZ
Point Group is C2v
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
0.000 |
0.000 |
0.109 |
| H2 |
0.000 |
0.976 |
-0.327 |
| H3 |
0.000 |
-0.976 |
-0.327 |
Atom - Atom Distances (Å)
| |
C1 |
H2 |
H3 |
| C1 | | 1.0693 | 1.0693 |
H2 | 1.0693 | | 1.9524 | H3 | 1.0693 | 1.9524 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| H2 |
C1 |
H3 |
131.829 |
|
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at HF/aug-cc-pVQZ
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
-0.712 |
|
|
|
| 2 |
H |
0.356 |
|
|
|
| 3 |
H |
0.356 |
|
|
|
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 |
-0.585 |
0.585 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-8.161 |
0.000 |
0.000 |
| y |
0.000 |
-5.943 |
0.000 |
| z |
0.000 |
0.000 |
-7.614 |
|
| Traceless |
| | x | y | z |
| x |
-1.383 |
0.000 |
0.000 |
| y |
0.000 |
1.945 |
0.000 |
| z |
0.000 |
0.000 |
-0.562 |
|
| Polar |
| 3z2-r2 | -1.124 |
| x2-y2 | -2.218 |
| 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 |
1.929 |
0.000 |
0.000 |
| y |
0.000 |
2.130 |
0.000 |
| z |
0.000 |
0.000 |
1.858 |
<r2> (average value of r
2) Å
2
| <r2> |
6.713 |
| (<r2>)1/2 |
2.591 |
Jump to
S1C1
S2C1
S2C2
Energy calculated at HF/aug-cc-pVQZ
| | hartrees |
| Energy at 0K | -38.928451 |
| Energy at 298.15K | |
| HF Energy | -38.928451 |
| Nuclear repulsion energy | 6.243401 |
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 HF/aug-cc-pVQZ
| 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 |
3300 |
2998 |
0.00 |
|
|
|
| 2 |
Σu |
3637 |
3304 |
56.63 |
|
|
|
| 3 |
Πu |
1123i |
1020i |
102.62 |
|
|
|
| 4 |
Πu |
1123i |
1020i |
102.62 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 2345.9 cm
-1
Scaled (by 0.9085) Zero Point Vibrational Energy (zpe) 2131.2 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 HF/aug-cc-pVQZ
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 |
1.059 |
| H3 |
0.000 |
0.000 |
-1.059 |
Atom - Atom Distances (Å)
| |
C1 |
H2 |
H3 |
| C1 | | 1.0595 | 1.0595 |
H2 | 1.0595 | | 2.1189 | H3 | 1.0595 | 2.1189 | |
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 HF/aug-cc-pVQZ
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
-0.949 |
|
|
|
| 2 |
H |
0.474 |
|
|
|
| 3 |
H |
0.474 |
|
|
|
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 |
-8.229 |
0.000 |
0.000 |
| y |
0.000 |
-8.229 |
0.000 |
| z |
0.000 |
0.000 |
-5.130 |
|
| Traceless |
| | x | y | z |
| x |
-1.550 |
0.000 |
0.000 |
| y |
0.000 |
-1.550 |
0.000 |
| z |
0.000 |
0.000 |
3.099 |
|
| Polar |
| 3z2-r2 | 6.198 |
| 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 |
2.035 |
0.000 |
0.000 |
| y |
0.000 |
2.035 |
0.000 |
| z |
0.000 |
0.000 |
2.168 |
<r2> (average value of r
2) Å
2
| <r2> |
6.739 |
| (<r2>)1/2 |
2.596 |
Jump to
S1C1
S1C2
S2C2
Energy calculated at HF/aug-cc-pVQZ
| | hartrees |
| Energy at 0K | -38.895668 |
| Energy at 298.15K | -38.895508 |
| HF Energy | -38.895668 |
| Nuclear repulsion energy | 6.109300 |
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 HF/aug-cc-pVQZ
Point Group is C2v
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
0.000 |
0.000 |
0.169 |
| H2 |
0.000 |
0.861 |
-0.507 |
| H3 |
0.000 |
-0.861 |
-0.507 |
Atom - Atom Distances (Å)
| |
C1 |
H2 |
H3 |
| C1 | | 1.0945 | 1.0945 |
H2 | 1.0945 | | 1.7223 | H3 | 1.0945 | 1.7223 | |
More geometry information
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at HF/aug-cc-pVQZ
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
-0.550 |
|
|
|
| 2 |
H |
0.275 |
|
|
|
| 3 |
H |
0.275 |
|
|
|
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 |
-1.904 |
1.904 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-6.402 |
0.000 |
0.000 |
| y |
0.000 |
-7.081 |
0.000 |
| z |
0.000 |
0.000 |
-9.685 |
|
| Traceless |
| | x | y | z |
| x |
1.981 |
0.000 |
0.000 |
| y |
0.000 |
0.963 |
0.000 |
| z |
0.000 |
0.000 |
-2.944 |
|
| Polar |
| 3z2-r2 | -5.888 |
| x2-y2 | 0.679 |
| 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 |
2.032 |
0.000 |
0.000 |
| y |
0.000 |
2.357 |
0.000 |
| z |
0.000 |
0.000 |
2.479 |
<r2> (average value of r
2) Å
2
| <r2> |
6.991 |
| (<r2>)1/2 |
2.644 |
Jump to
S1C1
S1C2
S2C1
Energy calculated at HF/aug-cc-pVQZ
| | hartrees |
| Energy at 0K | -38.895668 |
| Energy at 298.15K | -38.895508 |
| HF Energy | -38.895668 |
| Nuclear repulsion energy | 6.109300 |
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 HF/aug-cc-pVQZ
Geometric Data calculated at HF/aug-cc-pVQZ
Point Group is C2v
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability