Jump to
S1C2
Energy calculated at ROHF/3-21G
| | hartrees |
| Energy at 0K | -150.227498 |
| Energy at 298.15K | |
| HF Energy | -150.227498 |
| Nuclear repulsion energy | 52.924115 |
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/3-21G
| 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 |
3667 |
3326 |
150.89 |
|
|
|
| 2 |
Σ |
2244 |
2036 |
388.55 |
|
|
|
| 3 |
Σ |
1397 |
1267 |
29.47 |
|
|
|
| 4 |
Π |
666 |
604 |
34.82 |
|
|
|
| 4 |
Π |
663 |
602 |
30.50 |
|
|
|
| 5 |
Π |
511 |
464 |
217.72 |
|
|
|
| 5 |
Π |
495 |
449 |
26.69 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 4821.5 cm
-1
Scaled (by 0.907) Zero Point Vibrational Energy (zpe) 4373.1 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/3-21G
Point Group is C∞v
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
0.000 |
0.000 |
0.018 |
| C2 |
0.000 |
0.000 |
-1.231 |
| O3 |
0.000 |
0.000 |
1.195 |
| H4 |
0.000 |
0.000 |
-2.280 |
Atom - Atom Distances (Å)
| |
C1 |
C2 |
O3 |
H4 |
| C1 | | 1.2487 | 1.1776 | 2.2971 |
C2 | 1.2487 | | 2.4263 | 1.0484 | O3 | 1.1776 | 2.4263 | | 3.4747 | H4 | 2.2971 | 1.0484 | 3.4747 | |
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/3-21G
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
0.358 |
|
|
|
| 2 |
C |
-0.164 |
|
|
|
| 3 |
O |
-0.558 |
|
|
|
| 4 |
H |
0.364 |
|
|
|
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 |
-2.512 |
2.512 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-16.175 |
0.000 |
0.000 |
| y |
0.000 |
-17.816 |
0.000 |
| z |
0.000 |
0.000 |
-16.116 |
|
| Traceless |
| | x | y | z |
| x |
0.790 |
0.000 |
0.000 |
| y |
0.000 |
-1.670 |
0.000 |
| z |
0.000 |
0.000 |
0.880 |
|
| Polar |
| 3z2-r2 | 1.760 |
| x2-y2 | 1.640 |
| 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> |
36.152 |
| (<r2>)1/2 |
6.013 |
Jump to
S1C1
Energy calculated at ROHF/3-21G
| | hartrees |
| Energy at 0K | -150.227498 |
| Energy at 298.15K | |
| HF Energy | -150.227498 |
| Nuclear repulsion energy | 52.922720 |
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/3-21G
| 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 |
3668 |
3327 |
150.86 |
|
|
|
| 2 |
Σ |
2244 |
2035 |
388.66 |
|
|
|
| 3 |
Σ |
1397 |
1267 |
29.45 |
|
|
|
| 4 |
Π |
666 |
604 |
34.73 |
|
|
|
| 4 |
Π |
664 |
602 |
30.67 |
|
|
|
| 5 |
Π |
510 |
462 |
217.56 |
|
|
|
| 5 |
Π |
494 |
448 |
26.78 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 4820.5 cm
-1
Scaled (by 0.907) Zero Point Vibrational Energy (zpe) 4372.2 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/3-21G
Point Group is C∞v
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
0.000 |
0.000 |
0.018 |
| C2 |
0.000 |
0.000 |
-1.231 |
| O3 |
0.000 |
0.000 |
1.195 |
| H4 |
0.000 |
0.000 |
-2.279 |
Atom - Atom Distances (Å)
| |
C1 |
C2 |
O3 |
H4 |
| C1 | | 1.2487 | 1.1776 | 2.2970 |
C2 | 1.2487 | | 2.4264 | 1.0483 | O3 | 1.1776 | 2.4264 | | 3.4747 | H4 | 2.2970 | 1.0483 | 3.4747 | |
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/3-21G
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
0.358 |
|
|
|
| 2 |
C |
-0.164 |
|
|
|
| 3 |
O |
-0.558 |
|
|
|
| 4 |
H |
0.364 |
|
|
|
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 |
-2.512 |
2.512 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-17.816 |
0.000 |
0.000 |
| y |
0.000 |
-16.175 |
0.000 |
| z |
0.000 |
0.000 |
-16.116 |
|
| Traceless |
| | x | y | z |
| x |
-1.670 |
0.000 |
0.000 |
| y |
0.000 |
0.791 |
0.000 |
| z |
0.000 |
0.000 |
0.879 |
|
| Polar |
| 3z2-r2 | 1.758 |
| x2-y2 | -1.640 |
| 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> |
36.153 |
| (<r2>)1/2 |
6.013 |