Jump to
S1C2
S2C1
S2C2
Energy calculated at mPW1PW91/6-31G(2df,p)
| | hartrees |
| Energy at 0K | -39.145740 |
| Energy at 298.15K | -39.145550 |
| HF Energy | -39.145740 |
| Nuclear repulsion energy | 6.149256 |
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 mPW1PW91/6-31G(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 |
0.992 |
-0.319 |
| H3 |
0.000 |
-0.992 |
-0.319 |
Atom - Atom Distances (Å)
| |
C1 |
H2 |
H3 |
| C1 | | 1.0795 | 1.0795 |
H2 | 1.0795 | | 1.9842 | H3 | 1.0795 | 1.9842 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| H2 |
C1 |
H3 |
133.570 |
|
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at mPW1PW91/6-31G(2df,p)
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
-0.366 |
|
|
|
| 2 |
H |
0.183 |
|
|
|
| 3 |
H |
0.183 |
|
|
|
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 |
-0.602 |
0.602 |
| 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 |
-5.626 |
0.000 |
| z |
0.000 |
0.000 |
-7.369 |
|
| Traceless |
| | x | y | z |
| x |
-1.323 |
0.000 |
0.000 |
| y |
0.000 |
1.969 |
0.000 |
| z |
0.000 |
0.000 |
-0.646 |
|
| Polar |
| 3z2-r2 | -1.291 |
| x2-y2 | -2.194 |
| 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 |
1.018 |
0.000 |
0.000 |
| y |
0.000 |
1.856 |
0.000 |
| z |
0.000 |
0.000 |
1.166 |
<r2> (average value of r
2) Å
2
| <r2> |
6.574 |
| (<r2>)1/2 |
2.564 |
Jump to
S1C1
S2C1
S2C2
Energy calculated at mPW1PW91/6-31G(2df,p)
| | hartrees |
| Energy at 0K | -39.136948 |
| Energy at 298.15K | |
| HF Energy | -39.136948 |
| Nuclear repulsion energy | 6.200793 |
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 mPW1PW91/6-31G(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 |
3251 |
3104 |
0.00 |
|
|
|
| 2 |
Σu |
3594 |
3431 |
52.78 |
|
|
|
| 3 |
Πu |
970i |
926i |
102.84 |
|
|
|
| 4 |
Πu |
970i |
926i |
102.84 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 2452.7 cm
-1
Scaled (by 0.9547) Zero Point Vibrational Energy (zpe) 2341.6 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 mPW1PW91/6-31G(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 |
1.067 |
| H3 |
0.000 |
0.000 |
-1.067 |
Atom - Atom Distances (Å)
| |
C1 |
H2 |
H3 |
| C1 | | 1.0668 | 1.0668 |
H2 | 1.0668 | | 2.1335 | H3 | 1.0668 | 2.1335 | |
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 mPW1PW91/6-31G(2df,p)
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
-0.427 |
|
|
|
| 2 |
H |
0.213 |
|
|
|
| 3 |
H |
0.213 |
|
|
|
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 |
-4.835 |
|
| Traceless |
| | x | y | z |
| x |
-1.493 |
0.000 |
0.000 |
| y |
0.000 |
-1.493 |
0.000 |
| z |
0.000 |
0.000 |
2.986 |
|
| Polar |
| 3z2-r2 | 5.973 |
| 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 |
1.734 |
<r2> (average value of r
2) Å
2
| <r2> |
6.539 |
| (<r2>)1/2 |
2.557 |
Jump to
S1C1
S1C2
S2C2
Energy calculated at mPW1PW91/6-31G(2df,p)
| | hartrees |
| Energy at 0K | -39.116831 |
| Energy at 298.15K | -39.116668 |
| HF Energy | -39.116831 |
| Nuclear repulsion energy | 5.998498 |
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 mPW1PW91/6-31G(2df,p)
Point Group is C2v
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
0.000 |
0.000 |
0.179 |
| H2 |
0.000 |
0.855 |
-0.538 |
| H3 |
0.000 |
-0.855 |
-0.538 |
Atom - Atom Distances (Å)
| |
C1 |
H2 |
H3 |
| C1 | | 1.1162 | 1.1162 |
H2 | 1.1162 | | 1.7102 | H3 | 1.1162 | 1.7102 | |
More geometry information
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at mPW1PW91/6-31G(2df,p)
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
-0.332 |
|
|
|
| 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 |
-1.774 |
1.774 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-6.208 |
0.000 |
0.000 |
| y |
0.000 |
-6.992 |
0.000 |
| z |
0.000 |
0.000 |
-8.892 |
|
| Traceless |
| | x | y | z |
| x |
1.734 |
0.000 |
0.000 |
| y |
0.000 |
0.558 |
0.000 |
| z |
0.000 |
0.000 |
-2.292 |
|
| Polar |
| 3z2-r2 | -4.584 |
| x2-y2 | 0.784 |
| 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 |
1.345 |
0.000 |
0.000 |
| y |
0.000 |
2.092 |
0.000 |
| z |
0.000 |
0.000 |
1.646 |
<r2> (average value of r
2) Å
2
| <r2> |
6.834 |
| (<r2>)1/2 |
2.614 |
Jump to
S1C1
S1C2
S2C1
Energy calculated at mPW1PW91/6-31G(2df,p)
| | hartrees |
| Energy at 0K | -39.116831 |
| Energy at 298.15K | -39.116668 |
| HF Energy | -39.116831 |
| Nuclear repulsion energy | 5.998498 |
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 mPW1PW91/6-31G(2df,p)
Geometric Data calculated at mPW1PW91/6-31G(2df,p)
Point Group is C2v
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability