Jump to
S1C2
Energy calculated at ROHF/6-311G*
| | hartrees |
| Energy at 0K | -151.111952 |
| Energy at 298.15K | |
| HF Energy | -151.111952 |
| Nuclear repulsion energy | 53.480270 |
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 ROHF/6-311G*
| Mode Number |
Symmetry |
Frequency (cm-1) |
Scaled Frequency (cm-1) |
IR Intensities (km mol-1) |
Raman Act (Å4/u) |
Dep P |
Dep U |
| 1 |
Σ |
3634 |
3109 |
176.13 |
|
|
|
| 2 |
Σ |
2363 |
2022 |
807.47 |
|
|
|
| 3 |
Σ |
1419 |
1214 |
19.63 |
|
|
|
| 4 |
Π |
665 |
569 |
4.67 |
|
|
|
| 4 |
Π |
622 |
532 |
18.29 |
|
|
|
| 5 |
Π |
270 |
231 |
42.95 |
|
|
|
| 5 |
Π |
327i |
280i |
194.57 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 4322.8 cm
-1
Scaled (by 0.8556) Zero Point Vibrational Energy (zpe) 3698.6 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 ROHF/6-311G*
Point Group is C∞v
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
0.000 |
0.000 |
0.031 |
| C2 |
0.000 |
0.000 |
-1.224 |
| O3 |
0.000 |
0.000 |
1.179 |
| H4 |
0.000 |
0.000 |
-2.277 |
Atom - Atom Distances (Å)
| |
C1 |
C2 |
O3 |
H4 |
| C1 | | 1.2559 | 1.1479 | 2.3087 |
C2 | 1.2559 | | 2.4037 | 1.0529 | O3 | 1.1479 | 2.4037 | | 3.4566 | H4 | 2.3087 | 1.0529 | 3.4566 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| C1 |
C2 |
H4 |
180.000 |
|
C2 |
C1 |
O3 |
180.000 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at ROHF/6-311G*
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
0.357 |
|
|
|
| 2 |
C |
-0.321 |
|
|
|
| 3 |
O |
-0.349 |
|
|
|
| 4 |
H |
0.313 |
|
|
|
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 |
-2.402 |
2.402 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-17.975 |
0.000 |
0.000 |
| y |
0.000 |
-16.130 |
0.000 |
| z |
0.000 |
0.000 |
-15.460 |
|
| Traceless |
| | x | y | z |
| x |
-2.179 |
0.000 |
0.000 |
| y |
0.000 |
0.587 |
0.000 |
| z |
0.000 |
0.000 |
1.592 |
|
| Polar |
| 3z2-r2 | 3.185 |
| x2-y2 | -1.844 |
| 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 |
0.000 |
0.000 |
0.000 |
| y |
0.000 |
0.000 |
0.000 |
| z |
0.000 |
0.000 |
0.000 |
<r2> (average value of r
2) Å
2
| <r2> |
35.633 |
| (<r2>)1/2 |
5.969 |
Jump to
S1C1
Energy calculated at ROHF/6-311G*
| | hartrees |
| Energy at 0K | -151.113976 |
| Energy at 298.15K | |
| HF Energy | -151.113976 |
| Nuclear repulsion energy | 53.274850 |
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 ROHF/6-311G*
| Mode Number |
Symmetry |
Frequency (cm-1) |
Scaled Frequency (cm-1) |
IR Intensities (km mol-1) |
Raman Act (Å4/u) |
Dep P |
Dep U |
| 1 |
A' |
3501 |
2995 |
54.10 |
|
|
|
| 2 |
A' |
2336 |
1998 |
924.20 |
|
|
|
| 3 |
A' |
1328 |
1136 |
0.17 |
|
|
|
| 4 |
A' |
662 |
566 |
48.86 |
|
|
|
| 5 |
A' |
454 |
389 |
400.20 |
|
|
|
| 6 |
A" |
589 |
504 |
27.97 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 4434.5 cm
-1
Scaled (by 0.8556) Zero Point Vibrational Energy (zpe) 3794.2 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 ROHF/6-311G*
Point Group is Cs
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
0.000 |
0.047 |
0.000 |
| C2 |
0.719 |
-1.032 |
0.000 |
| O3 |
-0.760 |
0.891 |
0.000 |
| H4 |
1.766 |
-1.217 |
0.000 |
Atom - Atom Distances (Å)
| |
C1 |
C2 |
O3 |
H4 |
| C1 | | 1.2961 | 1.1355 | 2.1716 |
C2 | 1.2961 | | 2.4252 | 1.0637 | O3 | 1.1355 | 2.4252 | | 3.2896 | H4 | 2.1716 | 1.0637 | 3.2896 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| C1 |
C2 |
H4 |
133.677 |
|
C2 |
C1 |
O3 |
171.675 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at ROHF/6-311G*
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
0.419 |
|
|
|
| 2 |
C |
-0.396 |
|
|
|
| 3 |
O |
-0.316 |
|
|
|
| 4 |
H |
0.294 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
1.877 |
0.024 |
0.000 |
1.878 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-15.105 |
-0.275 |
0.001 |
| y |
-0.275 |
-20.414 |
-0.003 |
| z |
0.001 |
-0.003 |
-16.288 |
|
| Traceless |
| | x | y | z |
| x |
3.246 |
-0.275 |
0.001 |
| y |
-0.275 |
-4.717 |
-0.003 |
| z |
0.001 |
-0.003 |
1.472 |
|
| Polar |
| 3z2-r2 | 2.943 |
| x2-y2 | 5.309 |
| xy | -0.275 |
| xz | 0.001 |
| yz | -0.003 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
0.000 |
0.000 |
0.000 |
| y |
0.000 |
0.000 |
0.000 |
| z |
0.000 |
0.000 |
0.000 |
<r2> (average value of r
2) Å
2
| <r2> |
35.850 |
| (<r2>)1/2 |
5.987 |