Jump to
S1C2
Energy calculated at B3PW91/cc-pVDZ
| | hartrees |
| Energy at 0K | -151.872877 |
| Energy at 298.15K | |
| HF Energy | -151.872877 |
| Nuclear repulsion energy | 52.272195 |
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 B3PW91/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 |
3488 |
3366 |
126.72 |
|
|
|
| 2 |
Σ |
2133 |
2058 |
221.25 |
|
|
|
| 3 |
Σ |
1317 |
1271 |
24.58 |
|
|
|
| 4 |
Π |
571 |
551 |
0.02 |
|
|
|
| 4 |
Π |
526 |
508 |
10.45 |
|
|
|
| 5 |
Π |
439 |
424 |
21.02 |
|
|
|
| 5 |
Π |
354i |
342i |
128.37 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 4060.1 cm
-1
Scaled (by 0.965) Zero Point Vibrational Energy (zpe) 3918.0 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 B3PW91/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 |
-1.247 |
| O3 |
0.000 |
0.000 |
1.209 |
| H4 |
0.000 |
0.000 |
-2.318 |
Atom - Atom Distances (Å)
| |
C1 |
C2 |
O3 |
H4 |
| C1 | | 1.2691 | 1.1871 | 2.3401 |
C2 | 1.2691 | | 2.4561 | 1.0710 | O3 | 1.1871 | 2.4561 | | 3.5272 | H4 | 2.3401 | 1.0710 | 3.5272 | |
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 B3PW91/cc-pVDZ
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
0.137 |
|
|
|
| 2 |
C |
-0.087 |
|
|
|
| 3 |
O |
-0.112 |
|
|
|
| 4 |
H |
0.062 |
|
|
|
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 |
-1.942 |
1.942 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-15.932 |
0.000 |
0.000 |
| y |
0.000 |
-17.607 |
0.000 |
| z |
0.000 |
0.000 |
-14.373 |
|
| Traceless |
| | x | y | z |
| x |
0.059 |
0.000 |
0.000 |
| y |
0.000 |
-2.455 |
0.000 |
| z |
0.000 |
0.000 |
2.396 |
|
| Polar |
| 3z2-r2 | 4.793 |
| x2-y2 | 1.676 |
| 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 |
1.562 |
0.000 |
0.000 |
| y |
0.000 |
1.594 |
0.000 |
| z |
0.000 |
0.000 |
5.472 |
<r2> (average value of r
2) Å
2
| <r2> |
36.377 |
| (<r2>)1/2 |
6.031 |
Jump to
S1C1
Energy calculated at B3PW91/cc-pVDZ
| | hartrees |
| Energy at 0K | -151.875526 |
| Energy at 298.15K | |
| HF Energy | -151.875526 |
| Nuclear repulsion energy | 52.129340 |
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 B3PW91/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' |
3339 |
3223 |
39.96 |
|
|
|
| 2 |
A' |
2115 |
2041 |
306.42 |
|
|
|
| 3 |
A' |
1262 |
1218 |
6.10 |
|
|
|
| 4 |
A' |
569 |
549 |
31.78 |
|
|
|
| 5 |
A' |
499 |
481 |
198.68 |
|
|
|
| 6 |
A" |
500 |
483 |
3.78 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 4142.3 cm
-1
Scaled (by 0.965) Zero Point Vibrational Energy (zpe) 3997.3 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 B3PW91/cc-pVDZ
Point Group is Cs
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
0.000 |
0.051 |
0.000 |
| C2 |
1.068 |
-0.698 |
0.000 |
| O3 |
-1.067 |
0.545 |
0.000 |
| H4 |
2.131 |
-0.484 |
0.000 |
Atom - Atom Distances (Å)
| |
C1 |
C2 |
O3 |
H4 |
| C1 | | 1.3042 | 1.1756 | 2.1970 |
C2 | 1.3042 | | 2.4700 | 1.0846 | O3 | 1.1756 | 2.4700 | | 3.3592 | H4 | 2.1970 | 1.0846 | 3.3592 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| C1 |
C2 |
H4 |
133.559 |
|
C2 |
C1 |
O3 |
169.765 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at B3PW91/cc-pVDZ
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
0.155 |
|
|
|
| 2 |
C |
-0.174 |
|
|
|
| 3 |
O |
-0.094 |
|
|
|
| 4 |
H |
0.113 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
1.476 |
0.541 |
0.000 |
1.572 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-14.838 |
0.988 |
0.000 |
| y |
0.988 |
-18.891 |
0.000 |
| z |
0.000 |
0.000 |
-16.061 |
|
| Traceless |
| | x | y | z |
| x |
2.638 |
0.988 |
0.000 |
| y |
0.988 |
-3.441 |
0.000 |
| z |
0.000 |
0.000 |
0.804 |
|
| Polar |
| 3z2-r2 | 1.607 |
| x2-y2 | 4.053 |
| xy | 0.988 |
| xz | 0.000 |
| yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
4.634 |
-1.611 |
0.000 |
| y |
-1.611 |
2.922 |
0.000 |
| z |
0.000 |
0.000 |
1.986 |
<r2> (average value of r
2) Å
2
| <r2> |
36.399 |
| (<r2>)1/2 |
6.033 |