Jump to
S1C2
Energy calculated at ROHF/6-31G**
| | hartrees |
| Energy at 0K | -151.075502 |
| Energy at 298.15K | |
| HF Energy | -151.075502 |
| Nuclear repulsion energy | 53.219524 |
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/6-31G**
| 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 |
3650 |
3120 |
194.21 |
|
|
|
| 2 |
Σ |
2371 |
2027 |
725.21 |
|
|
|
| 3 |
Σ |
1429 |
1221 |
21.76 |
|
|
|
| 4 |
Π |
642 |
549 |
5.56 |
|
|
|
| 4 |
Π |
600 |
513 |
19.19 |
|
|
|
| 5 |
Π |
283 |
242 |
43.42 |
|
|
|
| 5 |
Π |
270i |
231i |
191.95 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 4352.9 cm
-1
Scaled (by 0.8546) Zero Point Vibrational Energy (zpe) 3720.0 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/6-31G**
Point Group is C∞v
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
0.000 |
0.000 |
0.029 |
| C2 |
0.000 |
0.000 |
-1.229 |
| O3 |
0.000 |
0.000 |
1.186 |
| H4 |
0.000 |
0.000 |
-2.283 |
Atom - Atom Distances (Å)
| |
C1 |
C2 |
O3 |
H4 |
| C1 | | 1.2578 | 1.1573 | 2.3113 |
C2 | 1.2578 | | 2.4151 | 1.0535 | O3 | 1.1573 | 2.4151 | | 3.4686 | H4 | 2.3113 | 1.0535 | 3.4686 | |
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/6-31G**
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
0.419 |
|
|
|
| 2 |
C |
-0.220 |
|
|
|
| 3 |
O |
-0.461 |
|
|
|
| 4 |
H |
0.263 |
|
|
|
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 |
-2.519 |
2.519 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-17.632 |
0.000 |
0.000 |
| y |
0.000 |
-15.901 |
0.000 |
| z |
0.000 |
0.000 |
-15.340 |
|
| Traceless |
| | x | y | z |
| x |
-2.012 |
0.000 |
0.000 |
| y |
0.000 |
0.585 |
0.000 |
| z |
0.000 |
0.000 |
1.427 |
|
| Polar |
| 3z2-r2 | 2.854 |
| x2-y2 | -1.731 |
| 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> |
35.708 |
| (<r2>)1/2 |
5.976 |
Jump to
S1C1
Energy calculated at ROHF/6-31G**
| | hartrees |
| Energy at 0K | -151.076654 |
| Energy at 298.15K | |
| HF Energy | -151.076654 |
| Nuclear repulsion energy | 53.072936 |
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/6-31G**
| 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' |
3548 |
3033 |
78.40 |
|
|
|
| 2 |
A' |
2342 |
2001 |
843.47 |
|
|
|
| 3 |
A' |
1360 |
1162 |
1.20 |
|
|
|
| 4 |
A' |
633 |
541 |
27.56 |
|
|
|
| 5 |
A' |
394 |
337 |
384.96 |
|
|
|
| 6 |
A" |
571 |
488 |
27.66 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 4423.4 cm
-1
Scaled (by 0.8546) Zero Point Vibrational Energy (zpe) 3780.3 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 ROHF/6-31G**
Point Group is Cs
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
0.000 |
0.047 |
0.000 |
| C2 |
0.830 |
-0.941 |
0.000 |
| O3 |
-0.858 |
0.808 |
0.000 |
| H4 |
1.880 |
-1.095 |
0.000 |
Atom - Atom Distances (Å)
| |
C1 |
C2 |
O3 |
H4 |
| C1 | | 1.2902 | 1.1467 | 2.1999 |
C2 | 1.2902 | | 2.4304 | 1.0615 | O3 | 1.1467 | 2.4304 | | 3.3344 | H4 | 2.1999 | 1.0615 | 3.3344 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| C1 |
C2 |
H4 |
138.405 |
|
C2 |
C1 |
O3 |
171.635 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at ROHF/6-31G**
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
0.521 |
|
|
|
| 2 |
C |
-0.291 |
|
|
|
| 3 |
O |
-0.437 |
|
|
|
| 4 |
H |
0.207 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
2.025 |
-0.140 |
0.000 |
2.030 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-14.975 |
0.077 |
0.002 |
| y |
0.077 |
-19.646 |
-0.003 |
| z |
0.002 |
-0.003 |
-16.016 |
|
| Traceless |
| | x | y | z |
| x |
2.856 |
0.077 |
0.002 |
| y |
0.077 |
-4.150 |
-0.003 |
| z |
0.002 |
-0.003 |
1.294 |
|
| Polar |
| 3z2-r2 | 2.589 |
| x2-y2 | 4.671 |
| xy | 0.077 |
| xz | 0.002 |
| 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> |
35.842 |
| (<r2>)1/2 |
5.987 |