Jump to
S1C2
Energy calculated at ROMP2/6-311+G(3df,2p)
| hartrees |
Energy at 0K | -151.644015 |
Energy at 298.15K | |
HF Energy | -151.128551 |
Nuclear repulsion energy | 52.453605 |
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 ROMP2/6-311+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 |
3496 |
3496 |
|
|
|
|
2 |
Σ |
2080 |
2080 |
|
|
|
|
3 |
Σ |
1292 |
1292 |
|
|
|
|
4 |
Π |
565 |
565 |
|
|
|
|
4 |
Π |
508 |
508 |
|
|
|
|
5 |
Π |
463 |
463 |
|
|
|
|
5 |
Π |
417i |
417i |
|
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 3993.3 cm
-1
Scaled (by 1) Zero Point Vibrational Energy (zpe) 3993.3 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 ROMP2/6-311+G(3df,2p)
Point Group is C∞v
Cartesians (Å)
Atom |
x (Å) |
y (Å) |
z (Å) |
C1 |
0.000 |
0.000 |
0.020 |
C2 |
0.000 |
0.000 |
-1.243 |
O3 |
0.000 |
0.000 |
1.205 |
H4 |
0.000 |
0.000 |
-2.304 |
Atom - Atom Distances (Å)
|
C1 |
C2 |
O3 |
H4 |
C1 | | 1.2625 | 1.1857 | 2.3232 |
C2 | 1.2625 | | 2.4482 | 1.0607 | O3 | 1.1857 | 2.4482 | | 3.5090 | H4 | 2.3232 | 1.0607 | 3.5090 | |
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 ROMP2/6-311+G(3df,2p)
Charges (e)
Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
1 |
C |
0.704 |
|
|
|
2 |
C |
-0.201 |
|
|
|
3 |
O |
-0.769 |
|
|
|
4 |
H |
0.266 |
|
|
|
Electric dipole moments
Electric Quadrupole moment
Quadrupole components in D Å
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> |
36.611 |
(<r2>)1/2 |
6.051 |
Jump to
S1C1
Energy calculated at ROMP2/6-311+G(3df,2p)
| hartrees |
Energy at 0K | -151.647366 |
Energy at 298.15K | |
HF Energy | -151.130118 |
Nuclear repulsion energy | 52.263939 |
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 ROMP2/6-311+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' |
3370 |
3370 |
|
|
|
|
2 |
A' |
2093 |
2093 |
|
|
|
|
3 |
A' |
1232 |
1232 |
|
|
|
|
4 |
A' |
575 |
575 |
|
|
|
|
5 |
A' |
531 |
531 |
|
|
|
|
6 |
A" |
494 |
494 |
|
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 4147.5 cm
-1
Scaled (by 1) Zero Point Vibrational Energy (zpe) 4147.5 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 ROMP2/6-311+G(3df,2p)
Point Group is Cs
Cartesians (Å)
Atom |
x (Å) |
y (Å) |
z (Å) |
C1 |
0.000 |
0.055 |
0.000 |
C2 |
1.102 |
-0.636 |
0.000 |
O3 |
-1.094 |
0.482 |
0.000 |
H4 |
2.140 |
-0.368 |
0.000 |
Atom - Atom Distances (Å)
|
C1 |
C2 |
O3 |
H4 |
C1 | | 1.3006 | 1.1746 | 2.1813 |
C2 | 1.3006 | | 2.4644 | 1.0715 | O3 | 1.1746 | 2.4644 | | 3.3439 | H4 | 2.1813 | 1.0715 | 3.3439 | |
More geometry information
Calculated Bond Angles
atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
C1 |
C2 |
H4 |
133.489 |
|
C2 |
C1 |
O3 |
169.263 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at ROMP2/6-311+G(3df,2p)
Charges (e)
Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
1 |
C |
0.874 |
|
|
|
2 |
C |
-0.412 |
|
|
|
3 |
O |
-0.685 |
|
|
|
4 |
H |
0.222 |
|
|
|
Electric dipole moments
Electric Quadrupole moment
Quadrupole components in D Å
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> |
36.737 |
(<r2>)1/2 |
6.061 |