Jump to
S1C2
Energy calculated at ROHF/6-311+G(3df,2p)
| | hartrees |
| Energy at 0K | -151.131779 |
| Energy at 298.15K | |
| HF Energy | -151.131779 |
| Nuclear repulsion energy | 53.549624 |
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/6-311+G(3df,2p)
| 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 |
3610 |
3279 |
196.37 |
|
|
|
| 2 |
Σ |
2345 |
2130 |
890.66 |
|
|
|
| 3 |
Σ |
1415 |
1285 |
15.79 |
|
|
|
| 4 |
Π |
662 |
602 |
0.92 |
|
|
|
| 4 |
Π |
622 |
565 |
13.32 |
|
|
|
| 5 |
Π |
321 |
292 |
38.82 |
|
|
|
| 5 |
Π |
299i |
272i |
163.38 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 4337.7 cm
-1
Scaled (by 0.9085) Zero Point Vibrational Energy (zpe) 3940.8 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/6-311+G(3df,2p)
Point Group is C∞v
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
0.000 |
0.000 |
0.032 |
| C2 |
0.000 |
0.000 |
-1.223 |
| O3 |
0.000 |
0.000 |
1.178 |
| H4 |
0.000 |
0.000 |
-2.275 |
Atom - Atom Distances (Å)
| |
C1 |
C2 |
O3 |
H4 |
| C1 | | 1.2548 | 1.1459 | 2.3067 |
C2 | 1.2548 | | 2.4007 | 1.0519 | O3 | 1.1459 | 2.4007 | | 3.4527 | H4 | 2.3067 | 1.0519 | 3.4527 | |
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/6-311+G(3df,2p)
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
0.762 |
|
|
|
| 2 |
C |
-0.238 |
|
|
|
| 3 |
O |
-0.788 |
|
|
|
| 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 |
-2.454 |
2.454 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-16.258 |
0.000 |
0.000 |
| y |
0.000 |
-18.172 |
0.000 |
| z |
0.000 |
0.000 |
-15.475 |
|
| Traceless |
| | x | y | z |
| x |
0.565 |
0.000 |
0.000 |
| y |
0.000 |
-2.306 |
0.000 |
| z |
0.000 |
0.000 |
1.740 |
|
| Polar |
| 3z2-r2 | 3.481 |
| x2-y2 | 1.914 |
| 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> |
35.642 |
| (<r2>)1/2 |
5.970 |
Jump to
S1C1
Energy calculated at ROHF/6-311+G(3df,2p)
| | hartrees |
| Energy at 0K | -151.133888 |
| Energy at 298.15K | |
| HF Energy | -151.133888 |
| Nuclear repulsion energy | 53.332656 |
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/6-311+G(3df,2p)
| 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' |
3463 |
3146 |
61.29 |
|
|
|
| 2 |
A' |
2322 |
2110 |
973.28 |
|
|
|
| 3 |
A' |
1312 |
1192 |
0.16 |
|
|
|
| 4 |
A' |
676 |
614 |
58.92 |
|
|
|
| 5 |
A' |
456 |
414 |
368.96 |
|
|
|
| 6 |
A" |
591 |
537 |
20.43 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 4409.7 cm
-1
Scaled (by 0.9085) Zero Point Vibrational Energy (zpe) 4006.2 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/6-311+G(3df,2p)
Point Group is Cs
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
0.000 |
0.047 |
0.000 |
| C2 |
0.687 |
-1.055 |
0.000 |
| O3 |
-0.733 |
0.910 |
0.000 |
| H4 |
1.737 |
-1.230 |
0.000 |
Atom - Atom Distances (Å)
| |
C1 |
C2 |
O3 |
H4 |
| C1 | | 1.2987 | 1.1322 | 2.1556 |
C2 | 1.2987 | | 2.4244 | 1.0641 | O3 | 1.1322 | 2.4244 | | 3.2676 | H4 | 2.1556 | 1.0641 | 3.2676 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| C1 |
C2 |
H4 |
131.403 |
|
C2 |
C1 |
O3 |
171.634 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at ROHF/6-311+G(3df,2p)
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
0.936 |
|
|
|
| 2 |
C |
-0.456 |
|
|
|
| 3 |
O |
-0.698 |
|
|
|
| 4 |
H |
0.219 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
1.733 |
-0.014 |
0.000 |
1.733 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-15.401 |
-0.374 |
0.001 |
| y |
-0.374 |
-20.420 |
-0.003 |
| z |
0.001 |
-0.003 |
-16.483 |
|
| Traceless |
| | x | y | z |
| x |
3.051 |
-0.374 |
0.001 |
| y |
-0.374 |
-4.479 |
-0.003 |
| z |
0.001 |
-0.003 |
1.428 |
|
| Polar |
| 3z2-r2 | 2.855 |
| x2-y2 | 5.020 |
| xy | -0.374 |
| 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> |
35.865 |
| (<r2>)1/2 |
5.989 |