Jump to
S1C2
Energy calculated at ROHF/daug-cc-pVDZ
| | hartrees |
| Energy at 0K | -151.097410 |
| Energy at 298.15K | |
| HF Energy | -151.097410 |
| Nuclear repulsion energy | 53.177654 |
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/daug-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 |
3615 |
3615 |
202.61 |
|
|
|
| 2 |
Σ |
2340 |
2340 |
879.20 |
|
|
|
| 3 |
Σ |
1409 |
1409 |
19.70 |
|
|
|
| 4 |
Π |
649 |
649 |
0.44 |
|
|
|
| 4 |
Π |
607 |
607 |
10.42 |
|
|
|
| 5 |
Π |
209 |
209 |
39.33 |
|
|
|
| 5 |
Π |
393i |
393i |
157.75 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 4217.9 cm
-1
Scaled (by 1) Zero Point Vibrational Energy (zpe) 4217.9 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/daug-cc-pVDZ
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 |
-1.232 |
| O3 |
0.000 |
0.000 |
1.186 |
| H4 |
0.000 |
0.000 |
-2.290 |
Atom - Atom Distances (Å)
| |
C1 |
C2 |
O3 |
H4 |
| C1 | | 1.2642 | 1.1536 | 2.3228 |
C2 | 1.2642 | | 2.4178 | 1.0586 | O3 | 1.1536 | 2.4178 | | 3.4764 | H4 | 2.3228 | 1.0586 | 3.4764 | |
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/daug-cc-pVDZ
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
0.321 |
|
|
|
| 2 |
C |
0.302 |
|
|
|
| 3 |
O |
-0.293 |
|
|
|
| 4 |
H |
-0.329 |
|
|
|
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 |
-2.472 |
2.472 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-18.301 |
0.000 |
0.000 |
| y |
0.000 |
-16.334 |
0.000 |
| z |
0.000 |
0.000 |
-15.486 |
|
| Traceless |
| | x | y | z |
| x |
-2.391 |
0.000 |
0.000 |
| y |
0.000 |
0.560 |
0.000 |
| z |
0.000 |
0.000 |
1.832 |
|
| Polar |
| 3z2-r2 | 3.663 |
| x2-y2 | -1.967 |
| 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> |
36.044 |
| (<r2>)1/2 |
6.004 |
Jump to
S1C1
Energy calculated at ROHF/daug-cc-pVDZ
| | hartrees |
| Energy at 0K | -151.100798 |
| Energy at 298.15K | |
| HF Energy | -151.100798 |
| Nuclear repulsion energy | 52.928753 |
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/daug-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 |
A' |
3450 |
3450 |
47.26 |
|
|
|
| 2 |
A' |
2306 |
2306 |
966.67 |
|
|
|
| 3 |
A' |
1291 |
1291 |
0.24 |
|
|
|
| 4 |
A' |
686 |
686 |
104.50 |
|
|
|
| 5 |
A' |
486 |
486 |
311.32 |
|
|
|
| 6 |
A" |
577 |
577 |
17.79 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 4397.8 cm
-1
Scaled (by 1) Zero Point Vibrational Energy (zpe) 4397.8 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/daug-cc-pVDZ
Point Group is Cs
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
0.000 |
0.049 |
0.000 |
| C2 |
0.724 |
-1.048 |
0.000 |
| O3 |
-0.768 |
0.890 |
0.000 |
| H4 |
1.795 |
-1.127 |
0.000 |
Atom - Atom Distances (Å)
| |
C1 |
C2 |
O3 |
H4 |
| C1 | | 1.3145 | 1.1383 | 2.1464 |
C2 | 1.3145 | | 2.4453 | 1.0739 | O3 | 1.1383 | 2.4453 | | 3.2614 | H4 | 2.1464 | 1.0739 | 3.2614 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| C1 |
C2 |
H4 |
127.685 |
|
C2 |
C1 |
O3 |
171.032 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at ROHF/daug-cc-pVDZ
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
0.802 |
|
|
|
| 2 |
C |
-0.026 |
|
|
|
| 3 |
O |
-0.303 |
|
|
|
| 4 |
H |
-0.473 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
1.675 |
0.210 |
0.000 |
1.688 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-15.432 |
-0.048 |
0.001 |
| y |
-0.048 |
-20.813 |
-0.003 |
| z |
0.001 |
-0.003 |
-16.608 |
|
| Traceless |
| | x | y | z |
| x |
3.278 |
-0.048 |
0.001 |
| y |
-0.048 |
-4.793 |
-0.003 |
| z |
0.001 |
-0.003 |
1.515 |
|
| Polar |
| 3z2-r2 | 3.030 |
| x2-y2 | 5.381 |
| xy | -0.048 |
| 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> |
36.293 |
| (<r2>)1/2 |
6.024 |