Jump to
S1C2
Energy calculated at B1B95/6-31+G**
| | hartrees |
| Energy at 0K | -151.871273 |
| Energy at 298.15K | |
| HF Energy | -151.871273 |
| Nuclear repulsion energy | 52.421774 |
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 B1B95/6-31+G**
| 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 |
3501 |
3349 |
125.63 |
49.82 |
0.23 |
0.37 |
| 2 |
Σ |
2130 |
2038 |
245.49 |
8.02 |
0.54 |
0.70 |
| 3 |
Σ |
1330 |
1272 |
26.54 |
41.15 |
0.20 |
0.33 |
| 4 |
Π |
559 |
535 |
0.14 |
0.79 |
0.75 |
0.86 |
| 4 |
Π |
521 |
498 |
16.15 |
2.56 |
0.75 |
0.86 |
| 5 |
Π |
454 |
434 |
24.77 |
0.68 |
0.75 |
0.86 |
| 5 |
Π |
312i |
298i |
161.58 |
14.49 |
0.75 |
0.86 |
Unscaled Zero Point Vibrational Energy (zpe) 4091.5 cm
-1
Scaled (by 0.9566) Zero Point Vibrational Energy (zpe) 3913.9 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 B1B95/6-31+G**
Point Group is C∞v
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
0.000 |
0.000 |
0.019 |
| C2 |
0.000 |
0.000 |
-1.243 |
| O3 |
0.000 |
0.000 |
1.206 |
| H4 |
0.000 |
0.000 |
-2.306 |
Atom - Atom Distances (Å)
| |
C1 |
C2 |
O3 |
H4 |
| C1 | | 1.2611 | 1.1877 | 2.3246 |
C2 | 1.2611 | | 2.4488 | 1.0636 | O3 | 1.1877 | 2.4488 | | 3.5124 | H4 | 2.3246 | 1.0636 | 3.5124 | |
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 B1B95/6-31+G**
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
0.123 |
|
|
|
| 2 |
C |
0.115 |
|
|
|
| 3 |
O |
-0.475 |
|
|
|
| 4 |
H |
0.237 |
|
|
|
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 |
-2.251 |
2.251 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-18.037 |
0.000 |
0.000 |
| y |
0.000 |
-16.226 |
0.000 |
| z |
0.000 |
0.000 |
-14.961 |
|
| Traceless |
| | x | y | z |
| x |
-2.444 |
0.000 |
0.000 |
| y |
0.000 |
0.273 |
0.000 |
| z |
0.000 |
0.000 |
2.170 |
|
| Polar |
| 3z2-r2 | 4.341 |
| x2-y2 | -1.811 |
| 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 |
2.156 |
0.000 |
0.000 |
| y |
0.000 |
1.795 |
0.000 |
| z |
0.000 |
0.000 |
6.204 |
<r2> (average value of r
2) Å
2
| <r2> |
36.472 |
| (<r2>)1/2 |
6.039 |
Jump to
S1C1
Energy calculated at B1B95/6-31+G**
| | hartrees |
| Energy at 0K | -151.872872 |
| Energy at 298.15K | |
| HF Energy | -151.872872 |
| Nuclear repulsion energy | 52.314794 |
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 B1B95/6-31+G**
| 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' |
3397 |
3250 |
52.44 |
74.41 |
0.34 |
0.50 |
| 2 |
A' |
2115 |
2024 |
331.95 |
6.70 |
0.72 |
0.84 |
| 3 |
A' |
1289 |
1233 |
8.43 |
36.50 |
0.23 |
0.38 |
| 4 |
A' |
541 |
518 |
5.61 |
5.50 |
0.70 |
0.82 |
| 5 |
A' |
448 |
428 |
245.41 |
6.72 |
0.14 |
0.25 |
| 6 |
A" |
492 |
471 |
2.18 |
1.05 |
0.75 |
0.86 |
Unscaled Zero Point Vibrational Energy (zpe) 4141.4 cm
-1
Scaled (by 0.9566) Zero Point Vibrational Energy (zpe) 3961.7 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 B1B95/6-31+G**
Point Group is Cs
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
0.000 |
0.048 |
0.000 |
| C2 |
1.092 |
-0.638 |
0.000 |
| O3 |
-1.088 |
0.501 |
0.000 |
| H4 |
2.151 |
-0.470 |
0.000 |
Atom - Atom Distances (Å)
| |
C1 |
C2 |
O3 |
H4 |
| C1 | | 1.2895 | 1.1780 | 2.2121 |
C2 | 1.2895 | | 2.4589 | 1.0720 | O3 | 1.1780 | 2.4589 | | 3.3805 | H4 | 2.2121 | 1.0720 | 3.3805 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| C1 |
C2 |
H4 |
138.833 |
|
C2 |
C1 |
O3 |
170.445 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at B1B95/6-31+G**
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
0.245 |
|
|
|
| 2 |
C |
-0.079 |
|
|
|
| 3 |
O |
-0.366 |
|
|
|
| 4 |
H |
0.200 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
1.886 |
0.404 |
0.000 |
1.929 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-15.112 |
1.036 |
0.000 |
| y |
1.036 |
-19.279 |
0.000 |
| z |
0.000 |
0.000 |
-16.328 |
|
| Traceless |
| | x | y | z |
| x |
2.691 |
1.036 |
0.000 |
| y |
1.036 |
-3.559 |
0.000 |
| z |
0.000 |
0.000 |
0.868 |
|
| Polar |
| 3z2-r2 | 1.735 |
| x2-y2 | 4.167 |
| xy | 1.036 |
| xz | 0.000 |
| yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
5.246 |
-1.790 |
0.000 |
| y |
-1.790 |
3.428 |
0.000 |
| z |
0.000 |
0.000 |
2.378 |
<r2> (average value of r
2) Å
2
| <r2> |
36.482 |
| (<r2>)1/2 |
6.040 |