Jump to
S1C2
Energy calculated at wB97X-D/6-311+G(3df,2p)
| | hartrees |
| Energy at 0K | -151.921642 |
| Energy at 298.15K | |
| HF Energy | -151.921642 |
| Nuclear repulsion energy | 52.803447 |
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 wB97X-D/6-311+G(3df,2p)
| 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 |
3463 |
3463 |
123.58 |
47.84 |
0.23 |
0.37 |
| 2 |
Σ |
2136 |
2136 |
312.85 |
9.92 |
0.43 |
0.61 |
| 3 |
Σ |
1332 |
1332 |
22.65 |
45.55 |
0.14 |
0.25 |
| 4 |
Π |
585 |
585 |
0.19 |
0.25 |
0.75 |
0.86 |
| 4 |
Π |
543 |
543 |
11.05 |
0.71 |
0.75 |
0.86 |
| 5 |
Π |
460 |
460 |
21.49 |
0.31 |
0.75 |
0.86 |
| 5 |
Π |
321i |
321i |
127.69 |
7.49 |
0.75 |
0.86 |
Unscaled Zero Point Vibrational Energy (zpe) 4098.7 cm
-1
Scaled (by 1) Zero Point Vibrational Energy (zpe) 4098.7 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 wB97X-D/6-311+G(3df,2p)
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 |
-1.234 |
| O3 |
0.000 |
0.000 |
1.197 |
| H4 |
0.000 |
0.000 |
-2.296 |
Atom - Atom Distances (Å)
| |
C1 |
C2 |
O3 |
H4 |
| C1 | | 1.2556 | 1.1754 | 2.3172 |
C2 | 1.2556 | | 2.4310 | 1.0617 | O3 | 1.1754 | 2.4310 | | 3.4927 | H4 | 2.3172 | 1.0617 | 3.4927 | |
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 wB97X-D/6-311+G(3df,2p)
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
0.522 |
|
|
|
| 2 |
C |
-0.158 |
|
|
|
| 3 |
O |
-0.607 |
|
|
|
| 4 |
H |
0.243 |
|
|
|
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 |
-2.187 |
2.187 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-17.997 |
0.000 |
0.000 |
| y |
0.000 |
-16.203 |
0.000 |
| z |
0.000 |
0.000 |
-14.832 |
|
| Traceless |
| | x | y | z |
| x |
-2.480 |
0.000 |
0.000 |
| y |
0.000 |
0.212 |
0.000 |
| z |
0.000 |
0.000 |
2.268 |
|
| Polar |
| 3z2-r2 | 4.537 |
| x2-y2 | -1.795 |
| 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 |
2.979 |
0.000 |
0.000 |
| y |
0.000 |
2.651 |
0.000 |
| z |
0.000 |
0.000 |
6.206 |
<r2> (average value of r
2) Å
2
| <r2> |
36.080 |
| (<r2>)1/2 |
6.007 |
Jump to
S1C1
Energy calculated at wB97X-D/6-311+G(3df,2p)
| | hartrees |
| Energy at 0K | -151.923347 |
| Energy at 298.15K | |
| HF Energy | -151.923347 |
| Nuclear repulsion energy | 52.688699 |
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 wB97X-D/6-311+G(3df,2p)
| 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' |
3353 |
3353 |
52.24 |
68.96 |
0.32 |
0.48 |
| 2 |
A' |
2131 |
2131 |
404.47 |
7.66 |
0.70 |
0.82 |
| 3 |
A' |
1282 |
1282 |
4.62 |
39.62 |
0.16 |
0.28 |
| 4 |
A' |
581 |
581 |
9.89 |
3.73 |
0.69 |
0.82 |
| 5 |
A' |
449 |
449 |
254.27 |
1.67 |
0.13 |
0.24 |
| 6 |
A" |
515 |
515 |
4.32 |
1.07 |
0.75 |
0.86 |
Unscaled Zero Point Vibrational Energy (zpe) 4156.2 cm
-1
Scaled (by 1) Zero Point Vibrational Energy (zpe) 4156.2 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 wB97X-D/6-311+G(3df,2p)
Point Group is Cs
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
0.000 |
0.043 |
0.000 |
| C2 |
0.979 |
-0.791 |
0.000 |
| O3 |
-0.991 |
0.655 |
0.000 |
| H4 |
2.049 |
-0.749 |
0.000 |
Atom - Atom Distances (Å)
| |
C1 |
C2 |
O3 |
H4 |
| C1 | | 1.2861 | 1.1647 | 2.1968 |
C2 | 1.2861 | | 2.4438 | 1.0709 | O3 | 1.1647 | 2.4438 | | 3.3484 | H4 | 2.1968 | 1.0709 | 3.3484 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| C1 |
C2 |
H4 |
137.311 |
|
C2 |
C1 |
O3 |
171.321 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at wB97X-D/6-311+G(3df,2p)
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
0.675 |
|
|
|
| 2 |
C |
-0.343 |
|
|
|
| 3 |
O |
-0.546 |
|
|
|
| 4 |
H |
0.214 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
1.707 |
0.139 |
0.000 |
1.713 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-15.031 |
0.385 |
0.000 |
| y |
0.385 |
-19.288 |
0.000 |
| z |
0.000 |
0.000 |
-16.339 |
|
| Traceless |
| | x | y | z |
| x |
2.782 |
0.385 |
0.000 |
| y |
0.385 |
-3.603 |
0.000 |
| z |
0.000 |
0.000 |
0.821 |
|
| Polar |
| 3z2-r2 | 1.641 |
| x2-y2 | 4.257 |
| xy | 0.385 |
| xz | 0.000 |
| yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
4.988 |
-1.606 |
0.000 |
| y |
-1.606 |
4.379 |
0.000 |
| z |
0.000 |
0.000 |
3.089 |
<r2> (average value of r
2) Å
2
| <r2> |
36.112 |
| (<r2>)1/2 |
6.009 |