Jump to
S1C2
Energy calculated at ROHF/6-31G
| | hartrees |
| Energy at 0K | -150.998620 |
| Energy at 298.15K | |
| HF Energy | -150.998620 |
| Nuclear repulsion energy | 52.700181 |
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 |
3677 |
3292 |
164.00 |
|
|
|
| 2 |
Σ |
2235 |
2001 |
478.79 |
|
|
|
| 3 |
Σ |
1368 |
1224 |
45.68 |
|
|
|
| 4 |
Π |
578 |
517 |
0.15 |
|
|
|
| 4 |
Π |
536 |
480 |
9.12 |
|
|
|
| 5 |
Π |
352 |
315 |
54.08 |
|
|
|
| 5 |
Π |
320 |
287 |
235.37 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 4533.1 cm
-1
Scaled (by 0.8953) Zero Point Vibrational Energy (zpe) 4058.5 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 |
0.018 |
| C2 |
0.000 |
0.000 |
-1.237 |
| O3 |
0.000 |
0.000 |
1.200 |
| H4 |
0.000 |
0.000 |
-2.288 |
Atom - Atom Distances (Å)
| |
C1 |
C2 |
O3 |
H4 |
| C1 | | 1.2556 | 1.1816 | 2.3068 |
C2 | 1.2556 | | 2.4373 | 1.0512 | O3 | 1.1816 | 2.4373 | | 3.4885 | H4 | 2.3068 | 1.0512 | 3.4885 | |
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 |
0.265 |
|
|
|
| 2 |
C |
-0.153 |
|
|
|
| 3 |
O |
-0.458 |
|
|
|
| 4 |
H |
0.346 |
|
|
|
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 |
-2.985 |
2.985 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-17.831 |
0.000 |
0.000 |
| y |
0.000 |
-16.153 |
0.000 |
| z |
0.000 |
0.000 |
-16.380 |
|
| Traceless |
| | x | y | z |
| x |
-1.564 |
0.000 |
0.000 |
| y |
0.000 |
0.952 |
0.000 |
| z |
0.000 |
0.000 |
0.613 |
|
| Polar |
| 3z2-r2 | 1.225 |
| x2-y2 | -1.677 |
| 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> |
36.430 |
| (<r2>)1/2 |
6.036 |
Jump to
S1C1
Energy calculated at ROHF/6-31G
| | hartrees |
| Energy at 0K | -150.998620 |
| Energy at 298.15K | |
| HF Energy | -150.998620 |
| Nuclear repulsion energy | 52.700429 |
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 |
3677 |
3292 |
163.99 |
|
|
|
| 2 |
Σ |
2235 |
2001 |
478.84 |
|
|
|
| 3 |
Σ |
1368 |
1225 |
45.67 |
|
|
|
| 4 |
Π |
578 |
517 |
0.15 |
|
|
|
| 4 |
Π |
536 |
480 |
9.13 |
|
|
|
| 5 |
Π |
352 |
315 |
54.07 |
|
|
|
| 5 |
Π |
320 |
286 |
235.38 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 4532.9 cm
-1
Scaled (by 0.8953) Zero Point Vibrational Energy (zpe) 4058.3 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 C∞v
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
0.000 |
0.000 |
0.018 |
| C2 |
0.000 |
0.000 |
-1.237 |
| O3 |
0.000 |
0.000 |
1.200 |
| H4 |
0.000 |
0.000 |
-2.288 |
Atom - Atom Distances (Å)
| |
C1 |
C2 |
O3 |
H4 |
| C1 | | 1.2556 | 1.1816 | 2.3068 |
C2 | 1.2556 | | 2.4373 | 1.0512 | O3 | 1.1816 | 2.4373 | | 3.4884 | H4 | 2.3068 | 1.0512 | 3.4884 | |
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 |
0.265 |
|
|
|
| 2 |
C |
-0.153 |
|
|
|
| 3 |
O |
-0.458 |
|
|
|
| 4 |
H |
0.346 |
|
|
|
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 |
-2.985 |
2.985 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-17.831 |
0.000 |
0.000 |
| y |
0.000 |
-16.153 |
0.000 |
| z |
0.000 |
0.000 |
-16.380 |
|
| Traceless |
| | x | y | z |
| x |
-1.564 |
0.000 |
0.000 |
| y |
0.000 |
0.952 |
0.000 |
| z |
0.000 |
0.000 |
0.612 |
|
| Polar |
| 3z2-r2 | 1.225 |
| x2-y2 | -1.677 |
| 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> |
36.430 |
| (<r2>)1/2 |
6.036 |