Jump to
S1C2
Energy calculated at wB97X-D/6-31G**
| | hartrees |
| Energy at 0K | -189.031730 |
| Energy at 298.15K | -189.032841 |
| HF Energy | -189.031730 |
| 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' |
3725 |
3725 |
30.01 |
|
|
|
| 2 |
A' |
1928 |
1928 |
304.99 |
|
|
|
| 3 |
A' |
1321 |
1321 |
0.30 |
|
|
|
| 4 |
A' |
1129 |
1129 |
181.64 |
|
|
|
| 5 |
A' |
607 |
607 |
40.03 |
|
|
|
| 6 |
A" |
615 |
615 |
131.34 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 4662.3 cm
-1
Scaled (by 1) Zero Point Vibrational Energy (zpe) 4662.3 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 |
0.447 |
0.000 |
| O2 |
-1.061 |
-0.346 |
0.000 |
| O3 |
1.156 |
0.170 |
0.000 |
| H4 |
-0.761 |
-1.272 |
0.000 |
Atom - Atom Distances (Å)
| |
C1 |
O2 |
O3 |
H4 |
| C1 | | 1.3248 | 1.1886 | 1.8807 |
O2 | 1.3248 | | 2.2758 | 0.9732 | O3 | 1.1886 | 2.2758 | | 2.3989 | H4 | 1.8807 | 0.9732 | 2.3989 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| C1 |
O2 |
H4 |
108.883 |
|
O2 |
C1 |
O3 |
129.694 |
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 |
0.452 |
|
|
|
| 2 |
O |
-0.445 |
|
|
|
| 3 |
O |
-0.352 |
|
|
|
| 4 |
H |
0.344 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
-1.026 |
-1.736 |
0.000 |
2.017 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-19.894 |
0.688 |
0.000 |
| y |
0.688 |
-13.375 |
0.000 |
| z |
0.000 |
0.000 |
-15.754 |
|
| Traceless |
| | x | y | z |
| x |
-5.330 |
0.688 |
0.000 |
| y |
0.688 |
4.449 |
0.000 |
| z |
0.000 |
0.000 |
0.880 |
|
| Polar |
| 3z2-r2 | 1.761 |
| x2-y2 | -6.519 |
| xy | 0.688 |
| xz | 0.000 |
| yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
3.033 |
0.192 |
0.000 |
| y |
0.192 |
2.349 |
0.000 |
| z |
0.000 |
0.000 |
1.391 |
<r2> (average value of r
2) Å
2
| <r2> |
34.483 |
| (<r2>)1/2 |
5.872 |
Jump to
S1C1
Energy calculated at wB97X-D/6-31G**
| | hartrees |
| Energy at 0K | -189.033711 |
| Energy at 298.15K | -189.034791 |
| HF Energy | -189.033711 |
| 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' |
3901 |
3901 |
118.18 |
|
|
|
| 2 |
A' |
1962 |
1962 |
212.26 |
|
|
|
| 3 |
A' |
1265 |
1265 |
303.24 |
|
|
|
| 4 |
A' |
1143 |
1143 |
30.43 |
|
|
|
| 5 |
A' |
625 |
625 |
3.81 |
|
|
|
| 6 |
A" |
551 |
551 |
99.84 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 4724.1 cm
-1
Scaled (by 1) Zero Point Vibrational Energy (zpe) 4724.1 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 |
0.412 |
0.000 |
| O2 |
-0.945 |
-0.535 |
0.000 |
| O3 |
1.171 |
0.240 |
0.000 |
| H4 |
-1.807 |
-0.105 |
0.000 |
Atom - Atom Distances (Å)
| |
C1 |
O2 |
O3 |
H4 |
| C1 | | 1.3383 | 1.1837 | 1.8799 |
O2 | 1.3383 | | 2.2536 | 0.9639 | O3 | 1.1837 | 2.2536 | | 2.9983 | H4 | 1.8799 | 0.9639 | 2.9983 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| C1 |
O2 |
H4 |
108.384 |
|
O2 |
C1 |
O3 |
126.542 |
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 |
0.410 |
|
|
|
| 2 |
O |
-0.437 |
|
|
|
| 3 |
O |
-0.335 |
|
|
|
| 4 |
H |
0.362 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
-3.129 |
0.451 |
0.000 |
3.161 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-13.451 |
-1.135 |
0.000 |
| y |
-1.135 |
-17.401 |
0.000 |
| z |
0.000 |
0.000 |
-15.779 |
|
| Traceless |
| | x | y | z |
| x |
3.139 |
-1.135 |
0.000 |
| y |
-1.135 |
-2.786 |
0.000 |
| z |
0.000 |
0.000 |
-0.353 |
|
| Polar |
| 3z2-r2 | -0.707 |
| x2-y2 | 3.950 |
| xy | -1.135 |
| xz | 0.000 |
| yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
3.521 |
0.166 |
0.000 |
| y |
0.166 |
1.872 |
0.000 |
| z |
0.000 |
0.000 |
1.408 |
<r2> (average value of r
2) Å
2
| <r2> |
34.874 |
| (<r2>)1/2 |
5.905 |