Jump to
S1C2
Energy calculated at B3PW91/6-31G*
| | hartrees |
| Energy at 0K | -151.858164 |
| Energy at 298.15K | |
| HF Energy | -151.858164 |
| Nuclear repulsion energy | 52.304139 |
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 B3PW91/6-31G*
| 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 |
3504 |
3353 |
108.88 |
|
|
|
| 2 |
Σ |
2139 |
2047 |
186.69 |
|
|
|
| 3 |
Σ |
1322 |
1265 |
22.62 |
|
|
|
| 4 |
Π |
562 |
538 |
0.25 |
|
|
|
| 4 |
Π |
516 |
494 |
10.55 |
|
|
|
| 5 |
Π |
418 |
400 |
26.44 |
|
|
|
| 5 |
Π |
369i |
353i |
143.33 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 4046.5 cm
-1
Scaled (by 0.9567) Zero Point Vibrational Energy (zpe) 3871.3 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 B3PW91/6-31G*
Point Group is C∞v
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
0.000 |
0.000 |
0.018 |
| C2 |
0.000 |
0.000 |
-1.245 |
| O3 |
0.000 |
0.000 |
1.209 |
| H4 |
0.000 |
0.000 |
-2.311 |
Atom - Atom Distances (Å)
| |
C1 |
C2 |
O3 |
H4 |
| C1 | | 1.2638 | 1.1906 | 2.3292 |
C2 | 1.2638 | | 2.4544 | 1.0654 | O3 | 1.1906 | 2.4544 | | 3.5198 | H4 | 2.3292 | 1.0654 | 3.5198 | |
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 B3PW91/6-31G*
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
0.300 |
|
|
|
| 2 |
C |
-0.162 |
|
|
|
| 3 |
O |
-0.389 |
|
|
|
| 4 |
H |
0.251 |
|
|
|
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 |
-2.154 |
2.154 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-15.753 |
0.000 |
0.000 |
| y |
0.000 |
-17.378 |
0.000 |
| z |
0.000 |
0.000 |
-14.293 |
|
| Traceless |
| | x | y | z |
| x |
0.083 |
0.000 |
0.000 |
| y |
0.000 |
-2.355 |
0.000 |
| z |
0.000 |
0.000 |
2.272 |
|
| Polar |
| 3z2-r2 | 4.544 |
| x2-y2 | 1.625 |
| 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 |
1.425 |
0.000 |
0.000 |
| y |
0.000 |
1.429 |
0.000 |
| z |
0.000 |
0.000 |
5.384 |
<r2> (average value of r
2) Å
2
| <r2> |
36.214 |
| (<r2>)1/2 |
6.018 |
Jump to
S1C1
Energy calculated at B3PW91/6-31G*
| | hartrees |
| Energy at 0K | -151.860477 |
| Energy at 298.15K | |
| HF Energy | -151.860477 |
| Nuclear repulsion energy | 52.177993 |
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 B3PW91/6-31G*
| 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' |
3383 |
3237 |
36.04 |
|
|
|
| 2 |
A' |
2122 |
2030 |
264.75 |
|
|
|
| 3 |
A' |
1277 |
1221 |
7.20 |
|
|
|
| 4 |
A' |
545 |
522 |
9.22 |
|
|
|
| 5 |
A' |
506 |
484 |
226.18 |
|
|
|
| 6 |
A" |
495 |
473 |
3.63 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 4163.4 cm
-1
Scaled (by 0.9567) Zero Point Vibrational Energy (zpe) 3983.1 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 B3PW91/6-31G*
Point Group is Cs
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
0.000 |
0.051 |
0.000 |
| C2 |
1.108 |
-0.619 |
0.000 |
| O3 |
-1.101 |
0.475 |
0.000 |
| H4 |
2.159 |
-0.393 |
0.000 |
Atom - Atom Distances (Å)
| |
C1 |
C2 |
O3 |
H4 |
| C1 | | 1.2951 | 1.1803 | 2.2046 |
C2 | 1.2951 | | 2.4660 | 1.0750 | O3 | 1.1803 | 2.4660 | | 3.3744 | H4 | 2.2046 | 1.0750 | 3.3744 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| C1 |
C2 |
H4 |
136.722 |
|
C2 |
C1 |
O3 |
169.944 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at B3PW91/6-31G*
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
0.409 |
|
|
|
| 2 |
C |
-0.281 |
|
|
|
| 3 |
O |
-0.358 |
|
|
|
| 4 |
H |
0.230 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
1.713 |
0.487 |
0.000 |
1.781 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-14.753 |
1.138 |
0.000 |
| y |
1.138 |
-18.510 |
0.000 |
| z |
0.000 |
0.000 |
-15.861 |
|
| Traceless |
| | x | y | z |
| x |
2.432 |
1.138 |
0.000 |
| y |
1.138 |
-3.202 |
0.000 |
| z |
0.000 |
0.000 |
0.770 |
|
| Polar |
| 3z2-r2 | 1.541 |
| x2-y2 | 3.756 |
| xy | 1.138 |
| xz | 0.000 |
| yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
4.737 |
-1.548 |
0.000 |
| y |
-1.548 |
2.529 |
0.000 |
| z |
0.000 |
0.000 |
1.883 |
<r2> (average value of r
2) Å
2
| <r2> |
36.243 |
| (<r2>)1/2 |
6.020 |