Jump to
S1C2
Energy calculated at ROHF/aug-cc-pVQZ
| | hartrees |
| Energy at 0K | -151.144319 |
| Energy at 298.15K | |
| HF Energy | -151.144319 |
| Nuclear repulsion energy | 53.565488 |
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/aug-cc-pVQZ
| 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 |
3612 |
3612 |
193.74 |
|
|
|
| 2 |
Σ |
2340 |
2340 |
892.10 |
|
|
|
| 3 |
Σ |
1414 |
1414 |
16.16 |
|
|
|
| 4 |
Π |
657 |
657 |
0.65 |
|
|
|
| 4 |
Π |
613 |
613 |
12.66 |
|
|
|
| 5 |
Π |
300 |
300 |
42.48 |
|
|
|
| 5 |
Π |
304i |
304i |
160.97 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 4315.6 cm
-1
Scaled (by 1) Zero Point Vibrational Energy (zpe) 4315.6 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/aug-cc-pVQZ
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 |
1.177 |
| H4 |
0.000 |
0.000 |
-2.274 |
Atom - Atom Distances (Å)
| |
C1 |
C2 |
O3 |
H4 |
| C1 | | 1.2545 | 1.1456 | 2.3057 |
C2 | 1.2545 | | 2.4001 | 1.0512 | O3 | 1.1456 | 2.4001 | | 3.4513 | H4 | 2.3057 | 1.0512 | 3.4513 | |
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/aug-cc-pVQZ
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
0.758 |
|
|
|
| 2 |
C |
-0.669 |
|
|
|
| 3 |
O |
-0.595 |
|
|
|
| 4 |
H |
0.507 |
|
|
|
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 |
-2.433 |
2.433 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-16.260 |
0.000 |
0.000 |
| y |
0.000 |
-18.088 |
0.000 |
| z |
0.000 |
0.000 |
-15.460 |
|
| Traceless |
| | x | y | z |
| x |
0.514 |
0.000 |
0.000 |
| y |
0.000 |
-2.227 |
0.000 |
| z |
0.000 |
0.000 |
1.714 |
|
| Polar |
| 3z2-r2 | 3.427 |
| x2-y2 | 1.827 |
| 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> |
35.607 |
| (<r2>)1/2 |
5.967 |
Jump to
S1C1
Energy calculated at ROHF/aug-cc-pVQZ
| | hartrees |
| Energy at 0K | -151.146393 |
| Energy at 298.15K | |
| HF Energy | -151.146393 |
| Nuclear repulsion energy | 53.350250 |
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/aug-cc-pVQZ
| 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' |
3465 |
3465 |
60.12 |
|
|
|
| 2 |
A' |
2317 |
2317 |
973.69 |
|
|
|
| 3 |
A' |
1312 |
1312 |
0.14 |
|
|
|
| 4 |
A' |
672 |
672 |
56.62 |
|
|
|
| 5 |
A' |
452 |
452 |
369.62 |
|
|
|
| 6 |
A" |
588 |
588 |
19.54 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 4403.0 cm
-1
Scaled (by 1) Zero Point Vibrational Energy (zpe) 4403.0 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/aug-cc-pVQZ
Point Group is Cs
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
0.000 |
0.047 |
0.000 |
| C2 |
0.698 |
-1.047 |
0.000 |
| O3 |
-0.742 |
0.902 |
0.000 |
| H4 |
1.748 |
-1.215 |
0.000 |
Atom - Atom Distances (Å)
| |
C1 |
C2 |
O3 |
H4 |
| C1 | | 1.2981 | 1.1320 | 2.1560 |
C2 | 1.2981 | | 2.4235 | 1.0633 | O3 | 1.1320 | 2.4235 | | 3.2682 | H4 | 2.1560 | 1.0633 | 3.2682 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| C1 |
C2 |
H4 |
131.597 |
|
C2 |
C1 |
O3 |
171.572 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at ROHF/aug-cc-pVQZ
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
0.643 |
|
|
|
| 2 |
C |
-0.550 |
|
|
|
| 3 |
O |
-0.523 |
|
|
|
| 4 |
H |
0.430 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
1.719 |
0.002 |
0.000 |
1.719 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-15.354 |
-0.318 |
0.001 |
| y |
-0.318 |
-20.365 |
-0.003 |
| z |
0.001 |
-0.003 |
-16.469 |
|
| Traceless |
| | x | y | z |
| x |
3.063 |
-0.318 |
0.001 |
| y |
-0.318 |
-4.453 |
-0.003 |
| z |
0.001 |
-0.003 |
1.390 |
|
| Polar |
| 3z2-r2 | 2.780 |
| x2-y2 | 5.011 |
| xy | -0.318 |
| 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> |
35.828 |
| (<r2>)1/2 |
5.986 |