Jump to
S1C2
Energy calculated at wB97X-D/6-31G
| | hartrees |
| Energy at 0K | -188.949044 |
| Energy at 298.15K | -188.950101 |
| HF Energy | -188.949044 |
| Nuclear repulsion energy | |
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/6-31G
| 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' |
3547 |
3547 |
14.71 |
|
|
|
| 2 |
A' |
1799 |
1799 |
294.22 |
|
|
|
| 3 |
A' |
1294 |
1294 |
3.09 |
|
|
|
| 4 |
A' |
1034 |
1034 |
200.77 |
|
|
|
| 5 |
A' |
582 |
582 |
46.06 |
|
|
|
| 6 |
A" |
577 |
577 |
195.13 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 4416.8 cm
-1
Scaled (by 1) Zero Point Vibrational Energy (zpe) 4416.8 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 wB97X-D/6-31G
Point Group is Cs
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
0.000 |
0.449 |
0.000 |
| O2 |
-1.072 |
-0.363 |
0.000 |
| O3 |
1.181 |
0.192 |
0.000 |
| H4 |
-0.867 |
-1.325 |
0.000 |
Atom - Atom Distances (Å)
| |
C1 |
O2 |
O3 |
H4 |
| C1 | | 1.3450 | 1.2085 | 1.9744 |
O2 | 1.3450 | | 2.3204 | 0.9840 | O3 | 1.2085 | 2.3204 | | 2.5479 | H4 | 1.9744 | 0.9840 | 2.5479 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| C1 |
O2 |
H4 |
115.054 |
|
O2 |
C1 |
O3 |
130.579 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at wB97X-D/6-31G
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
0.490 |
|
|
|
| 2 |
O |
-0.551 |
|
|
|
| 3 |
O |
-0.345 |
|
|
|
| 4 |
H |
0.406 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
-0.993 |
-2.101 |
0.000 |
2.324 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-21.439 |
1.019 |
0.000 |
| y |
1.019 |
-13.309 |
0.000 |
| z |
0.000 |
0.000 |
-15.966 |
|
| Traceless |
| | x | y | z |
| x |
-6.802 |
1.019 |
0.000 |
| y |
1.019 |
5.393 |
0.000 |
| z |
0.000 |
0.000 |
1.408 |
|
| Polar |
| 3z2-r2 | 2.817 |
| x2-y2 | -8.130 |
| xy | 1.019 |
| xz | 0.000 |
| yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
3.122 |
0.286 |
0.000 |
| y |
0.286 |
2.297 |
0.000 |
| z |
0.000 |
0.000 |
1.166 |
<r2> (average value of r
2) Å
2
| <r2> |
35.975 |
| (<r2>)1/2 |
5.998 |
Jump to
S1C1
Energy calculated at wB97X-D/6-31G
| | hartrees |
| Energy at 0K | -188.953585 |
| Energy at 298.15K | -188.954637 |
| HF Energy | -188.953585 |
| Nuclear repulsion energy | |
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/6-31G
| 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' |
3768 |
3768 |
106.17 |
|
|
|
| 2 |
A' |
1859 |
1859 |
184.93 |
|
|
|
| 3 |
A' |
1201 |
1201 |
238.99 |
|
|
|
| 4 |
A' |
1067 |
1067 |
109.29 |
|
|
|
| 5 |
A' |
608 |
608 |
7.53 |
|
|
|
| 6 |
A" |
547 |
547 |
150.78 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 4524.8 cm
-1
Scaled (by 1) Zero Point Vibrational Energy (zpe) 4524.8 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 wB97X-D/6-31G
Point Group is Cs
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
0.000 |
0.420 |
0.000 |
| O2 |
-0.958 |
-0.550 |
0.000 |
| O3 |
1.190 |
0.257 |
0.000 |
| H4 |
-1.855 |
-0.177 |
0.000 |
Atom - Atom Distances (Å)
| |
C1 |
O2 |
O3 |
H4 |
| C1 | | 1.3626 | 1.2007 | 1.9488 |
O2 | 1.3626 | | 2.2938 | 0.9720 | O3 | 1.2007 | 2.2938 | | 3.0757 | H4 | 1.9488 | 0.9720 | 3.0757 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| C1 |
O2 |
H4 |
112.097 |
|
O2 |
C1 |
O3 |
126.861 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at wB97X-D/6-31G
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
0.444 |
|
|
|
| 2 |
O |
-0.542 |
|
|
|
| 3 |
O |
-0.327 |
|
|
|
| 4 |
H |
0.425 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
-3.424 |
0.586 |
0.000 |
3.474 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-13.712 |
-1.206 |
0.000 |
| y |
-1.206 |
-18.204 |
0.000 |
| z |
0.000 |
0.000 |
-15.982 |
|
| Traceless |
| | x | y | z |
| x |
3.381 |
-1.206 |
0.000 |
| y |
-1.206 |
-3.357 |
0.000 |
| z |
0.000 |
0.000 |
-0.024 |
|
| Polar |
| 3z2-r2 | -0.049 |
| x2-y2 | 4.492 |
| xy | -1.206 |
| xz | 0.000 |
| yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
3.639 |
0.227 |
0.000 |
| y |
0.227 |
1.771 |
0.000 |
| z |
0.000 |
0.000 |
1.181 |
<r2> (average value of r
2) Å
2
| <r2> |
36.106 |
| (<r2>)1/2 |
6.009 |