Jump to
S1C2
Energy calculated at wB97X-D/6-311G*
| | hartrees |
| Energy at 0K | -189.078874 |
| Energy at 298.15K | -189.079999 |
| HF Energy | -189.078874 |
| 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/6-311G*
| 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' |
3669 |
3669 |
12.51 |
|
|
|
| 2 |
A' |
1922 |
1922 |
340.09 |
|
|
|
| 3 |
A' |
1323 |
1323 |
0.98 |
|
|
|
| 4 |
A' |
1127 |
1127 |
184.48 |
|
|
|
| 5 |
A' |
613 |
613 |
40.56 |
|
|
|
| 6 |
A" |
631 |
631 |
142.00 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 4641.6 cm
-1
Scaled (by 1) Zero Point Vibrational Energy (zpe) 4641.6 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 wB97X-D/6-311G*
Point Group is Cs
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
0.000 |
0.444 |
0.000 |
| O2 |
-1.054 |
-0.352 |
0.000 |
| O3 |
1.150 |
0.179 |
0.000 |
| H4 |
-0.766 |
-1.280 |
0.000 |
Atom - Atom Distances (Å)
| |
C1 |
O2 |
O3 |
H4 |
| C1 | | 1.3205 | 1.1801 | 1.8862 |
O2 | 1.3205 | | 2.2670 | 0.9717 | O3 | 1.1801 | 2.2670 | | 2.4083 | H4 | 1.8862 | 0.9717 | 2.4083 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| C1 |
O2 |
H4 |
109.810 |
|
O2 |
C1 |
O3 |
129.995 |
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 |
0.299 |
|
|
|
| 2 |
O |
-0.449 |
|
|
|
| 3 |
O |
-0.252 |
|
|
|
| 4 |
H |
0.402 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
-0.926 |
-1.861 |
0.000 |
2.079 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-20.341 |
0.740 |
0.000 |
| y |
0.740 |
-13.564 |
0.000 |
| z |
0.000 |
0.000 |
-15.993 |
|
| Traceless |
| | x | y | z |
| x |
-5.563 |
0.740 |
0.000 |
| y |
0.740 |
4.603 |
0.000 |
| z |
0.000 |
0.000 |
0.960 |
|
| Polar |
| 3z2-r2 | 1.920 |
| x2-y2 | -6.777 |
| xy | 0.740 |
| xz | 0.000 |
| yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
3.117 |
0.199 |
0.000 |
| y |
0.199 |
2.534 |
0.000 |
| z |
0.000 |
0.000 |
1.490 |
<r2> (average value of r
2) Å
2
| <r2> |
34.509 |
| (<r2>)1/2 |
5.874 |
Jump to
S1C1
Energy calculated at wB97X-D/6-311G*
| | hartrees |
| Energy at 0K | -189.081230 |
| Energy at 298.15K | -189.082326 |
| HF Energy | -189.081230 |
| 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/6-311G*
| 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' |
3867 |
3867 |
95.39 |
|
|
|
| 2 |
A' |
1959 |
1959 |
231.71 |
|
|
|
| 3 |
A' |
1285 |
1285 |
295.53 |
|
|
|
| 4 |
A' |
1122 |
1122 |
53.82 |
|
|
|
| 5 |
A' |
633 |
633 |
4.61 |
|
|
|
| 6 |
A" |
567 |
567 |
112.78 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 4716.8 cm
-1
Scaled (by 1) Zero Point Vibrational Energy (zpe) 4716.8 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/6-311G*
Point Group is Cs
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
0.000 |
0.409 |
0.000 |
| O2 |
-0.938 |
-0.542 |
0.000 |
| O3 |
1.164 |
0.251 |
0.000 |
| H4 |
-1.806 |
-0.130 |
0.000 |
Atom - Atom Distances (Å)
| |
C1 |
O2 |
O3 |
H4 |
| C1 | | 1.3359 | 1.1744 | 1.8852 |
O2 | 1.3359 | | 2.2465 | 0.9611 | O3 | 1.1744 | 2.2465 | | 2.9945 | H4 | 1.8852 | 0.9611 | 2.9945 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| C1 |
O2 |
H4 |
109.226 |
|
O2 |
C1 |
O3 |
126.877 |
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 |
0.247 |
|
|
|
| 2 |
O |
-0.443 |
|
|
|
| 3 |
O |
-0.232 |
|
|
|
| 4 |
H |
0.427 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
-3.135 |
0.443 |
0.000 |
3.166 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-13.482 |
-1.101 |
0.000 |
| y |
-1.101 |
-17.843 |
0.000 |
| z |
0.000 |
0.000 |
-16.037 |
|
| Traceless |
| | x | y | z |
| x |
3.458 |
-1.101 |
0.000 |
| y |
-1.101 |
-3.083 |
0.000 |
| z |
0.000 |
0.000 |
-0.375 |
|
| Polar |
| 3z2-r2 | -0.750 |
| x2-y2 | 4.361 |
| xy | -1.101 |
| xz | 0.000 |
| yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
3.612 |
0.168 |
0.000 |
| y |
0.168 |
1.982 |
0.000 |
| z |
0.000 |
0.000 |
1.519 |
<r2> (average value of r
2) Å
2
| <r2> |
34.874 |
| (<r2>)1/2 |
5.905 |