Jump to
S1C2
Energy calculated at ROMP2/cc-pVDZ
| | hartrees |
| Energy at 0K | -151.502840 |
| Energy at 298.15K | |
| HF Energy | -151.084814 |
| Nuclear repulsion energy | 51.877660 |
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/cc-pVDZ
| 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 |
3514 |
3514 |
|
|
|
|
| 2 |
Σ |
2087 |
2087 |
|
|
|
|
| 3 |
Σ |
1291 |
1291 |
|
|
|
|
| 4 |
Π |
621 |
621 |
|
|
|
|
| 4 |
Π |
565 |
565 |
|
|
|
|
| 5 |
Π |
294 |
294 |
|
|
|
|
| 5 |
Π |
459i |
459i |
|
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 3956.4 cm
-1
Scaled (by 1) Zero Point Vibrational Energy (zpe) 3956.4 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/cc-pVDZ
Point Group is C∞v
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
0.000 |
0.000 |
0.022 |
| C2 |
0.000 |
0.000 |
-1.258 |
| O3 |
0.000 |
0.000 |
1.218 |
| H4 |
0.000 |
0.000 |
-2.331 |
Atom - Atom Distances (Å)
| |
C1 |
C2 |
O3 |
H4 |
| C1 | | 1.2799 | 1.1963 | 2.3528 |
C2 | 1.2799 | | 2.4762 | 1.0729 | O3 | 1.1963 | 2.4762 | | 3.5491 | H4 | 2.3528 | 1.0729 | 3.5491 | |
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/cc-pVDZ
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
0.284 |
|
|
|
| 2 |
C |
-0.149 |
|
|
|
| 3 |
O |
-0.247 |
|
|
|
| 4 |
H |
0.112 |
|
|
|
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> |
37.108 |
| (<r2>)1/2 |
6.092 |
Jump to
S1C1
Energy calculated at ROMP2/cc-pVDZ
| | hartrees |
| Energy at 0K | -151.507856 |
| Energy at 298.15K | |
| HF Energy | -151.086882 |
| Nuclear repulsion energy | 51.662660 |
The energy at 298.15K was derived from the energy at 0K
and an integrated heat capacity that used the calculated vibrational frequencies.
Geometric Data calculated at ROMP2/cc-pVDZ
Point Group is Cs
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
0.000 |
0.063 |
0.000 |
| C2 |
1.124 |
-0.638 |
0.000 |
| O3 |
-1.112 |
0.468 |
0.000 |
| H4 |
2.154 |
-0.290 |
0.000 |
Atom - Atom Distances (Å)
| |
C1 |
C2 |
O3 |
H4 |
| C1 | | 1.3245 | 1.1836 | 2.1830 |
C2 | 1.3245 | | 2.4946 | 1.0874 | O3 | 1.1836 | 2.4946 | | 3.3533 | H4 | 2.1830 | 1.0874 | 3.3533 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| C1 |
C2 |
H4 |
129.414 |
|
C2 |
C1 |
O3 |
168.061 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at ROMP2/cc-pVDZ
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
0.308 |
|
|
|
| 2 |
C |
-0.220 |
|
|
|
| 3 |
O |
-0.220 |
|
|
|
| 4 |
H |
0.132 |
|
|
|
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> |
37.244 |
| (<r2>)1/2 |
6.103 |