Jump to
S1C2
Energy calculated at PBE1PBE/cc-pVDZ
| | hartrees |
| Energy at 0K | -188.908262 |
| Energy at 298.15K | -188.909381 |
| HF Energy | -188.908262 |
| Nuclear repulsion energy | 63.308222 |
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 PBE1PBE/cc-pVDZ
| 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' |
3610 |
3471 |
23.39 |
|
|
|
| 2 |
A' |
1921 |
1847 |
315.90 |
|
|
|
| 3 |
A' |
1319 |
1268 |
0.45 |
|
|
|
| 4 |
A' |
1128 |
1085 |
148.63 |
|
|
|
| 5 |
A' |
609 |
585 |
33.37 |
|
|
|
| 6 |
A" |
618 |
594 |
108.92 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 4601.9 cm
-1
Scaled (by 0.9615) Zero Point Vibrational Energy (zpe) 4424.7 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 PBE1PBE/cc-pVDZ
Point Group is Cs
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
0.000 |
0.443 |
0.000 |
| O2 |
-1.061 |
-0.344 |
0.000 |
| O3 |
1.155 |
0.172 |
0.000 |
| H4 |
-0.748 |
-1.273 |
0.000 |
Atom - Atom Distances (Å)
| |
C1 |
O2 |
O3 |
H4 |
| C1 | | 1.3213 | 1.1862 | 1.8718 |
O2 | 1.3213 | | 2.2755 | 0.9799 | O3 | 1.1862 | 2.2755 | | 2.3894 | H4 | 1.8718 | 0.9799 | 2.3894 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| C1 |
O2 |
H4 |
107.937 |
|
O2 |
C1 |
O3 |
130.231 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at PBE1PBE/cc-pVDZ
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
0.144 |
|
|
|
| 2 |
O |
-0.139 |
|
|
|
| 3 |
O |
-0.167 |
|
|
|
| 4 |
H |
0.161 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
-0.989 |
-1.721 |
0.000 |
1.985 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-19.619 |
0.614 |
0.000 |
| y |
0.614 |
-13.688 |
0.000 |
| z |
0.000 |
0.000 |
-15.811 |
|
| Traceless |
| | x | y | z |
| x |
-4.869 |
0.614 |
0.000 |
| y |
0.614 |
4.027 |
0.000 |
| z |
0.000 |
0.000 |
0.842 |
|
| Polar |
| 3z2-r2 | 1.684 |
| x2-y2 | -5.930 |
| xy | 0.614 |
| xz | 0.000 |
| yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
3.026 |
0.238 |
0.000 |
| y |
0.238 |
2.515 |
0.000 |
| z |
0.000 |
0.000 |
1.422 |
<r2> (average value of r
2) Å
2
| <r2> |
34.448 |
| (<r2>)1/2 |
5.869 |
Jump to
S1C1
Energy calculated at PBE1PBE/cc-pVDZ
| | hartrees |
| Energy at 0K | -188.909800 |
| Energy at 298.15K | -188.910887 |
| HF Energy | -188.909800 |
| Nuclear repulsion energy | 63.014819 |
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 PBE1PBE/cc-pVDZ
| 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' |
3826 |
3678 |
128.03 |
|
|
|
| 2 |
A' |
1950 |
1875 |
226.58 |
|
|
|
| 3 |
A' |
1264 |
1215 |
278.25 |
|
|
|
| 4 |
A' |
1135 |
1092 |
27.69 |
|
|
|
| 5 |
A' |
627 |
602 |
3.92 |
|
|
|
| 6 |
A" |
554 |
533 |
87.59 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 4678.0 cm
-1
Scaled (by 0.9615) Zero Point Vibrational Energy (zpe) 4497.9 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 PBE1PBE/cc-pVDZ
Point Group is Cs
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
0.000 |
0.410 |
0.000 |
| O2 |
-0.944 |
-0.537 |
0.000 |
| O3 |
1.169 |
0.241 |
0.000 |
| H4 |
-1.803 |
-0.090 |
0.000 |
Atom - Atom Distances (Å)
| |
C1 |
O2 |
O3 |
H4 |
| C1 | | 1.3373 | 1.1815 | 1.8709 |
O2 | 1.3373 | | 2.2522 | 0.9683 | O3 | 1.1815 | 2.2522 | | 2.9906 | H4 | 1.8709 | 0.9683 | 2.9906 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| C1 |
O2 |
H4 |
107.402 |
|
O2 |
C1 |
O3 |
126.688 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at PBE1PBE/cc-pVDZ
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
0.090 |
|
|
|
| 2 |
O |
-0.128 |
|
|
|
| 3 |
O |
-0.146 |
|
|
|
| 4 |
H |
0.184 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
-2.964 |
0.330 |
0.000 |
2.983 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-13.515 |
-1.065 |
0.000 |
| y |
-1.065 |
-17.410 |
0.000 |
| z |
0.000 |
0.000 |
-15.839 |
|
| Traceless |
| | x | y | z |
| x |
3.110 |
-1.065 |
0.000 |
| y |
-1.065 |
-2.733 |
0.000 |
| z |
0.000 |
0.000 |
-0.376 |
|
| Polar |
| 3z2-r2 | -0.753 |
| x2-y2 | 3.896 |
| xy | -1.065 |
| xz | 0.000 |
| yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
3.529 |
0.166 |
0.000 |
| y |
0.166 |
1.911 |
0.000 |
| z |
0.000 |
0.000 |
1.440 |
<r2> (average value of r
2) Å
2
| <r2> |
34.846 |
| (<r2>)1/2 |
5.903 |