Jump to
S1C2
Energy calculated at wB97X-D/6-311G**
| | hartrees |
| Energy at 0K | -151.907897 |
| Energy at 298.15K | |
| HF Energy | -151.907897 |
| Nuclear repulsion energy | 52.726753 |
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/6-311G**
| 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 |
3478 |
3327 |
124.64 |
41.04 |
0.27 |
0.43 |
| 2 |
Σ |
2147 |
2054 |
271.70 |
2.42 |
0.67 |
0.80 |
| 3 |
Σ |
1332 |
1274 |
24.14 |
32.73 |
0.23 |
0.38 |
| 4 |
Π |
588 |
563 |
0.28 |
1.50 |
0.75 |
0.86 |
| 4 |
Π |
544 |
520 |
15.76 |
1.74 |
0.75 |
0.86 |
| 5 |
Π |
467 |
447 |
20.76 |
0.19 |
0.75 |
0.86 |
| 5 |
Π |
286i |
274i |
146.91 |
7.00 |
0.75 |
0.86 |
Unscaled Zero Point Vibrational Energy (zpe) 4135.4 cm
-1
Scaled (by 0.9565) Zero Point Vibrational Energy (zpe) 3955.5 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/6-311G**
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 |
-1.236 |
| O3 |
0.000 |
0.000 |
1.199 |
| H4 |
0.000 |
0.000 |
-2.298 |
Atom - Atom Distances (Å)
| |
C1 |
C2 |
O3 |
H4 |
| C1 | | 1.2570 | 1.1776 | 2.3193 |
C2 | 1.2570 | | 2.4346 | 1.0624 | O3 | 1.1776 | 2.4346 | | 3.4969 | H4 | 2.3193 | 1.0624 | 3.4969 | |
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/6-311G**
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
0.227 |
|
|
|
| 2 |
C |
-0.166 |
|
|
|
| 3 |
O |
-0.232 |
|
|
|
| 4 |
H |
0.171 |
|
|
|
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 |
-2.100 |
2.100 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-16.021 |
0.000 |
0.000 |
| y |
0.000 |
-17.754 |
0.000 |
| z |
0.000 |
0.000 |
-14.737 |
|
| Traceless |
| | x | y | z |
| x |
0.224 |
0.000 |
0.000 |
| y |
0.000 |
-2.375 |
0.000 |
| z |
0.000 |
0.000 |
2.151 |
|
| Polar |
| 3z2-r2 | 4.301 |
| x2-y2 | 1.732 |
| 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 |
1.615 |
0.000 |
0.000 |
| y |
0.000 |
1.714 |
0.000 |
| z |
0.000 |
0.000 |
5.567 |
<r2> (average value of r
2) Å
2
| <r2> |
36.044 |
| (<r2>)1/2 |
6.004 |
Jump to
S1C1
Energy calculated at wB97X-D/6-311G**
| | hartrees |
| Energy at 0K | -151.908997 |
| Energy at 298.15K | |
| HF Energy | -151.908997 |
| Nuclear repulsion energy | 52.623255 |
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/6-311G**
| 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' |
3380 |
3233 |
57.62 |
64.36 |
0.35 |
0.52 |
| 2 |
A' |
2140 |
2047 |
352.00 |
2.87 |
0.45 |
0.62 |
| 3 |
A' |
1293 |
1237 |
7.78 |
29.86 |
0.29 |
0.45 |
| 4 |
A' |
577 |
552 |
6.96 |
5.02 |
0.73 |
0.84 |
| 5 |
A' |
396 |
379 |
251.03 |
6.37 |
0.14 |
0.24 |
| 6 |
A" |
517 |
494 |
6.05 |
1.56 |
0.75 |
0.86 |
Unscaled Zero Point Vibrational Energy (zpe) 4151.5 cm
-1
Scaled (by 0.9565) Zero Point Vibrational Energy (zpe) 3970.9 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 wB97X-D/6-311G**
Point Group is Cs
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
0.000 |
0.041 |
0.000 |
| C2 |
0.978 |
-0.788 |
0.000 |
| O3 |
-0.990 |
0.662 |
0.000 |
| H4 |
2.049 |
-0.814 |
0.000 |
Atom - Atom Distances (Å)
| |
C1 |
C2 |
O3 |
H4 |
| C1 | | 1.2825 | 1.1688 | 2.2197 |
C2 | 1.2825 | | 2.4451 | 1.0705 | O3 | 1.1688 | 2.4451 | | 3.3780 | H4 | 2.2197 | 1.0705 | 3.3780 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| C1 |
C2 |
H4 |
141.078 |
|
C2 |
C1 |
O3 |
171.845 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at wB97X-D/6-311G**
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
0.252 |
|
|
|
| 2 |
C |
-0.228 |
|
|
|
| 3 |
O |
-0.217 |
|
|
|
| 4 |
H |
0.192 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
1.797 |
0.096 |
0.000 |
1.799 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-14.710 |
0.238 |
0.000 |
| y |
0.238 |
-19.055 |
0.000 |
| z |
0.000 |
0.000 |
-16.110 |
|
| Traceless |
| | x | y | z |
| x |
2.873 |
0.238 |
0.000 |
| y |
0.238 |
-3.645 |
0.000 |
| z |
0.000 |
0.000 |
0.772 |
|
| Polar |
| 3z2-r2 | 1.544 |
| x2-y2 | 4.345 |
| xy | 0.238 |
| xz | 0.000 |
| yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
4.253 |
-1.835 |
0.000 |
| y |
-1.835 |
3.366 |
0.000 |
| z |
0.000 |
0.000 |
2.136 |
<r2> (average value of r
2) Å
2
| <r2> |
36.074 |
| (<r2>)1/2 |
6.006 |