Jump to
S1C2
Energy calculated at B1B95/daug-cc-pVDZ
| | hartrees |
| Energy at 0K | -151.887434 |
| Energy at 298.15K | |
| HF Energy | -151.887434 |
| Nuclear repulsion energy | 52.445660 |
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/daug-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 |
3483 |
3483 |
124.51 |
50.48 |
0.23 |
0.38 |
| 2 |
Σ |
2124 |
2124 |
255.24 |
13.95 |
0.32 |
0.48 |
| 3 |
Σ |
1321 |
1321 |
25.55 |
46.69 |
0.13 |
0.24 |
| 4 |
Π |
563 |
563 |
0.75 |
0.24 |
0.75 |
0.86 |
| 4 |
Π |
511 |
511 |
4.39 |
0.59 |
0.75 |
0.86 |
| 5 |
Π |
385 |
385 |
25.34 |
0.31 |
0.75 |
0.86 |
| 5 |
Π |
429i |
429i |
116.18 |
6.28 |
0.75 |
0.86 |
Unscaled Zero Point Vibrational Energy (zpe) 3978.6 cm
-1
Scaled (by 1) Zero Point Vibrational Energy (zpe) 3978.6 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 B1B95/daug-cc-pVDZ
Point Group is C∞v
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
0.000 |
0.000 |
0.021 |
| C2 |
0.000 |
0.000 |
-1.243 |
| O3 |
0.000 |
0.000 |
1.205 |
| H4 |
0.000 |
0.000 |
-2.309 |
Atom - Atom Distances (Å)
| |
C1 |
C2 |
O3 |
H4 |
| C1 | | 1.2636 | 1.1842 | 2.3303 |
C2 | 1.2636 | | 2.4478 | 1.0667 | O3 | 1.1842 | 2.4478 | | 3.5145 | H4 | 2.3303 | 1.0667 | 3.5145 | |
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/daug-cc-pVDZ
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
0.507 |
|
|
|
| 2 |
C |
0.187 |
|
|
|
| 3 |
O |
-0.202 |
|
|
|
| 4 |
H |
-0.492 |
|
|
|
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 |
-2.168 |
2.168 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-18.049 |
0.000 |
0.000 |
| y |
0.000 |
-16.248 |
0.000 |
| z |
0.000 |
0.000 |
-14.828 |
|
| Traceless |
| | x | y | z |
| x |
-2.512 |
0.000 |
0.000 |
| y |
0.000 |
0.191 |
0.000 |
| z |
0.000 |
0.000 |
2.321 |
|
| Polar |
| 3z2-r2 | 4.642 |
| x2-y2 | -1.802 |
| 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 |
3.099 |
0.000 |
0.000 |
| y |
0.000 |
2.764 |
0.000 |
| z |
0.000 |
0.000 |
6.329 |
<r2> (average value of r
2) Å
2
| <r2> |
36.448 |
| (<r2>)1/2 |
6.037 |
Jump to
S1C1
Energy calculated at B1B95/daug-cc-pVDZ
| | hartrees |
| Energy at 0K | -151.890365 |
| Energy at 298.15K | |
| HF Energy | -151.890365 |
| Nuclear repulsion energy | 52.302778 |
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/daug-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' |
3349 |
3349 |
39.17 |
83.50 |
0.30 |
0.46 |
| 2 |
A' |
2109 |
2109 |
352.62 |
9.19 |
0.64 |
0.78 |
| 3 |
A' |
1265 |
1265 |
5.63 |
40.20 |
0.14 |
0.25 |
| 4 |
A' |
572 |
572 |
34.78 |
2.63 |
0.75 |
0.86 |
| 5 |
A' |
491 |
491 |
209.26 |
0.81 |
0.18 |
0.30 |
| 6 |
A" |
494 |
494 |
1.84 |
0.47 |
0.75 |
0.86 |
Unscaled Zero Point Vibrational Energy (zpe) 4140.8 cm
-1
Scaled (by 1) Zero Point Vibrational Energy (zpe) 4140.8 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/daug-cc-pVDZ
Point Group is Cs
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
0.000 |
0.052 |
0.000 |
| C2 |
1.071 |
-0.685 |
0.000 |
| O3 |
-1.069 |
0.532 |
0.000 |
| H4 |
2.126 |
-0.458 |
0.000 |
Atom - Atom Distances (Å)
| |
C1 |
C2 |
O3 |
H4 |
| C1 | | 1.3000 | 1.1721 | 2.1865 |
C2 | 1.3000 | | 2.4620 | 1.0793 | O3 | 1.1721 | 2.4620 | | 3.3452 | H4 | 2.1865 | 1.0793 | 3.3452 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| C1 |
C2 |
H4 |
133.344 |
|
C2 |
C1 |
O3 |
169.674 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at B1B95/daug-cc-pVDZ
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
0.887 |
|
|
|
| 2 |
C |
0.036 |
|
|
|
| 3 |
O |
-0.232 |
|
|
|
| 4 |
H |
-0.691 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
1.592 |
0.418 |
0.000 |
1.646 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-15.327 |
1.020 |
0.000 |
| y |
1.020 |
-19.234 |
0.000 |
| z |
0.000 |
0.000 |
-16.413 |
|
| Traceless |
| | x | y | z |
| x |
2.496 |
1.020 |
0.000 |
| y |
1.020 |
-3.364 |
0.000 |
| z |
0.000 |
0.000 |
0.868 |
|
| Polar |
| 3z2-r2 | 1.736 |
| x2-y2 | 3.907 |
| xy | 1.020 |
| xz | 0.000 |
| yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
5.482 |
-1.466 |
0.000 |
| y |
-1.466 |
4.121 |
0.000 |
| z |
0.000 |
0.000 |
3.129 |
<r2> (average value of r
2) Å
2
| <r2> |
36.466 |
| (<r2>)1/2 |
6.039 |