Jump to
S1C2
Energy calculated at B3PW91/3-21G*
| | hartrees |
| Energy at 0K | -151.023081 |
| Energy at 298.15K | |
| HF Energy | -151.023081 |
| Nuclear repulsion energy | 51.979503 |
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 B3PW91/3-21G*
| 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 |
3505 |
3362 |
92.95 |
|
|
|
| 2 |
Σ |
2065 |
1981 |
74.76 |
|
|
|
| 3 |
Σ |
1287 |
1235 |
19.84 |
|
|
|
| 4 |
Π |
694 |
666 |
30.84 |
|
|
|
| 4 |
Π |
613 |
589 |
16.35 |
|
|
|
| 5 |
Π |
523 |
502 |
5.93 |
|
|
|
| 5 |
Π |
434 |
416 |
156.72 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 4560.6 cm
-1
Scaled (by 0.9594) Zero Point Vibrational Energy (zpe) 4375.4 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 B3PW91/3-21G*
Point Group is C∞v
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
0.000 |
0.000 |
0.007 |
| C2 |
0.000 |
0.000 |
-1.248 |
| O3 |
0.000 |
0.000 |
1.220 |
| H4 |
0.000 |
0.000 |
-2.309 |
Atom - Atom Distances (Å)
| |
C1 |
C2 |
O3 |
H4 |
| C1 | | 1.2550 | 1.2127 | 2.3164 |
C2 | 1.2550 | | 2.4677 | 1.0614 | O3 | 1.2127 | 2.4677 | | 3.5291 | H4 | 2.3164 | 1.0614 | 3.5291 | |
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 B3PW91/3-21G*
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
0.214 |
|
|
|
| 2 |
C |
-0.086 |
|
|
|
| 3 |
O |
-0.435 |
|
|
|
| 4 |
H |
0.307 |
|
|
|
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 |
-2.033 |
2.033 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-17.597 |
0.000 |
0.000 |
| y |
0.000 |
-16.016 |
0.000 |
| z |
0.000 |
0.000 |
-14.798 |
|
| Traceless |
| | x | y | z |
| x |
-2.190 |
0.000 |
0.000 |
| y |
0.000 |
0.181 |
0.000 |
| z |
0.000 |
0.000 |
2.009 |
|
| Polar |
| 3z2-r2 | 4.017 |
| x2-y2 | -1.581 |
| 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 |
0.957 |
0.000 |
0.000 |
| y |
0.000 |
1.098 |
0.000 |
| z |
0.000 |
0.000 |
5.020 |
<r2> (average value of r
2) Å
2
| <r2> |
36.659 |
| (<r2>)1/2 |
6.055 |
Jump to
S1C1
Energy calculated at B3PW91/3-21G*
| | hartrees |
| Energy at 0K | -151.023081 |
| Energy at 298.15K | |
| HF Energy | -151.023081 |
| Nuclear repulsion energy | 51.978856 |
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 B3PW91/3-21G*
| 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' |
3504 |
3362 |
92.91 |
|
|
|
| 2 |
A' |
2065 |
1981 |
74.49 |
|
|
|
| 3 |
A' |
1287 |
1235 |
19.87 |
|
|
|
| 4 |
A' |
613 |
589 |
16.36 |
|
|
|
| 5 |
A' |
434 |
417 |
156.65 |
|
|
|
| 6 |
A" |
638 |
612 |
8.91 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 4271.1 cm
-1
Scaled (by 0.9594) Zero Point Vibrational Energy (zpe) 4097.7 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 B3PW91/3-21G*
Point Group is Cs
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
0.000 |
0.007 |
0.000 |
| C2 |
0.003 |
-1.248 |
0.000 |
| O3 |
-0.003 |
1.220 |
0.000 |
| H4 |
0.005 |
-2.309 |
0.000 |
Atom - Atom Distances (Å)
| |
C1 |
C2 |
O3 |
H4 |
| C1 | | 1.2549 | 1.2128 | 2.3163 |
C2 | 1.2549 | | 2.4677 | 1.0614 | O3 | 1.2128 | 2.4677 | | 3.5291 | H4 | 2.3163 | 1.0614 | 3.5291 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| C1 |
C2 |
H4 |
179.972 |
|
C2 |
C1 |
O3 |
179.999 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at B3PW91/3-21G*
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
0.214 |
|
|
|
| 2 |
C |
-0.085 |
|
|
|
| 3 |
O |
-0.435 |
|
|
|
| 4 |
H |
0.307 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
0.004 |
-2.034 |
0.000 |
2.034 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-17.597 |
-0.005 |
0.000 |
| y |
-0.005 |
-14.797 |
0.000 |
| z |
0.000 |
0.000 |
-16.016 |
|
| Traceless |
| | x | y | z |
| x |
-2.190 |
-0.005 |
0.000 |
| y |
-0.005 |
2.009 |
0.000 |
| z |
0.000 |
0.000 |
0.181 |
|
| Polar |
| 3z2-r2 | 0.362 |
| x2-y2 | -2.800 |
| xy | -0.005 |
| xz | 0.000 |
| yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
0.957 |
-0.010 |
0.000 |
| y |
-0.010 |
5.020 |
0.000 |
| z |
0.000 |
0.000 |
1.097 |
<r2> (average value of r
2) Å
2
| <r2> |
36.659 |
| (<r2>)1/2 |
6.055 |