Jump to
S1C2
Energy calculated at B97D3/6-311G*
| | hartrees |
| Energy at 0K | -151.872493 |
| Energy at 298.15K | |
| HF Energy | -151.872493 |
| Nuclear repulsion energy | 52.253255 |
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 B97D3/6-311G*
| 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 |
3421 |
3421 |
88.29 |
43.94 |
0.28 |
0.43 |
| 2 |
Σ |
2086 |
2086 |
197.89 |
1.12 |
0.75 |
0.86 |
| 3 |
Σ |
1272 |
1272 |
22.46 |
31.95 |
0.24 |
0.38 |
| 4 |
Π |
555 |
555 |
0.03 |
1.26 |
0.75 |
0.86 |
| 4 |
Π |
509 |
509 |
7.19 |
1.53 |
0.75 |
0.86 |
| 5 |
Π |
402 |
402 |
28.27 |
0.52 |
0.75 |
0.86 |
| 5 |
Π |
435i |
435i |
141.43 |
7.34 |
0.75 |
0.86 |
Unscaled Zero Point Vibrational Energy (zpe) 3905.8 cm
-1
Scaled (by 1) Zero Point Vibrational Energy (zpe) 3905.8 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 B97D3/6-311G*
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 |
-1.247 |
| O3 |
0.000 |
0.000 |
1.210 |
| H4 |
0.000 |
0.000 |
-2.313 |
Atom - Atom Distances (Å)
| |
C1 |
C2 |
O3 |
H4 |
| C1 | | 1.2661 | 1.1909 | 2.3324 |
C2 | 1.2661 | | 2.4570 | 1.0663 | O3 | 1.1909 | 2.4570 | | 3.5233 | H4 | 2.3324 | 1.0663 | 3.5233 | |
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 B97D3/6-311G*
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
0.208 |
|
|
|
| 2 |
C |
-0.248 |
|
|
|
| 3 |
O |
-0.215 |
|
|
|
| 4 |
H |
0.255 |
|
|
|
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 |
-2.012 |
2.012 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-16.014 |
0.000 |
0.000 |
| y |
0.000 |
-17.775 |
0.000 |
| z |
0.000 |
0.000 |
-14.521 |
|
| Traceless |
| | x | y | z |
| x |
0.134 |
0.000 |
0.000 |
| y |
0.000 |
-2.507 |
0.000 |
| z |
0.000 |
0.000 |
2.373 |
|
| Polar |
| 3z2-r2 | 4.747 |
| x2-y2 | 1.761 |
| 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 |
1.624 |
0.000 |
0.000 |
| y |
0.000 |
1.736 |
0.000 |
| z |
0.000 |
0.000 |
5.626 |
<r2> (average value of r
2) Å
2
| <r2> |
36.455 |
| (<r2>)1/2 |
6.038 |
Jump to
S1C1
Energy calculated at B97D3/6-311G*
| | hartrees |
| Energy at 0K | -151.876281 |
| Energy at 298.15K | |
| HF Energy | -151.876281 |
| Nuclear repulsion energy | 52.060997 |
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 B97D3/6-311G*
| 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' |
3258 |
3258 |
14.93 |
85.32 |
0.35 |
0.52 |
| 2 |
A' |
2053 |
2053 |
255.56 |
2.81 |
0.44 |
0.61 |
| 3 |
A' |
1215 |
1215 |
7.31 |
28.33 |
0.28 |
0.44 |
| 4 |
A' |
582 |
582 |
155.73 |
10.10 |
0.30 |
0.46 |
| 5 |
A' |
527 |
527 |
61.86 |
2.36 |
0.39 |
0.56 |
| 6 |
A" |
486 |
486 |
1.95 |
0.40 |
0.75 |
0.86 |
Unscaled Zero Point Vibrational Energy (zpe) 4060.6 cm
-1
Scaled (by 1) Zero Point Vibrational Energy (zpe) 4060.6 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 B97D3/6-311G*
Point Group is Cs
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
0.000 |
0.055 |
0.000 |
| C2 |
1.122 |
-0.610 |
0.000 |
| O3 |
-1.111 |
0.453 |
0.000 |
| H4 |
2.154 |
-0.291 |
0.000 |
Atom - Atom Distances (Å)
| |
C1 |
C2 |
O3 |
H4 |
| C1 | | 1.3041 | 1.1802 | 2.1819 |
C2 | 1.3041 | | 2.4731 | 1.0800 | O3 | 1.1802 | 2.4731 | | 3.3490 | H4 | 2.1819 | 1.0800 | 3.3490 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| C1 |
C2 |
H4 |
132.235 |
|
C2 |
C1 |
O3 |
169.093 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at B97D3/6-311G*
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
0.253 |
|
|
|
| 2 |
C |
-0.318 |
|
|
|
| 3 |
O |
-0.192 |
|
|
|
| 4 |
H |
0.257 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
1.480 |
0.677 |
0.000 |
1.627 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-15.232 |
1.436 |
0.000 |
| y |
1.436 |
-18.916 |
0.000 |
| z |
0.000 |
0.000 |
-16.154 |
|
| Traceless |
| | x | y | z |
| x |
2.302 |
1.436 |
0.000 |
| y |
1.436 |
-3.222 |
0.000 |
| z |
0.000 |
0.000 |
0.920 |
|
| Polar |
| 3z2-r2 | 1.840 |
| x2-y2 | 3.683 |
| xy | 1.436 |
| xz | 0.000 |
| yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
5.043 |
-1.516 |
0.000 |
| y |
-1.516 |
2.845 |
0.000 |
| z |
0.000 |
0.000 |
2.053 |
<r2> (average value of r
2) Å
2
| <r2> |
36.517 |
| (<r2>)1/2 |
6.043 |