Jump to
S1C2
Energy calculated at PBE1PBE/cc-pVTZ
| | hartrees |
| Energy at 0K | -188.966840 |
| Energy at 298.15K | -188.967950 |
| HF Energy | -188.966840 |
| Nuclear repulsion energy | 63.524992 |
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-pVTZ
| 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' |
3645 |
3503 |
22.52 |
|
|
|
| 2 |
A' |
1913 |
1838 |
329.23 |
|
|
|
| 3 |
A' |
1312 |
1261 |
0.05 |
|
|
|
| 4 |
A' |
1110 |
1067 |
159.41 |
|
|
|
| 5 |
A' |
608 |
584 |
33.51 |
|
|
|
| 6 |
A" |
605 |
581 |
107.62 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 4596.2 cm
-1
Scaled (by 0.961) Zero Point Vibrational Energy (zpe) 4416.9 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-pVTZ
Point Group is Cs
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
0.000 |
0.437 |
0.000 |
| O2 |
-1.056 |
-0.350 |
0.000 |
| O3 |
1.152 |
0.182 |
0.000 |
| H4 |
-0.762 |
-1.278 |
0.000 |
Atom - Atom Distances (Å)
| |
C1 |
O2 |
O3 |
H4 |
| C1 | | 1.3175 | 1.1796 | 1.8768 |
O2 | 1.3175 | | 2.2710 | 0.9737 | O3 | 1.1796 | 2.2710 | | 2.4063 | H4 | 1.8768 | 0.9737 | 2.4063 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| C1 |
O2 |
H4 |
109.074 |
|
O2 |
C1 |
O3 |
130.780 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at PBE1PBE/cc-pVTZ
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
0.167 |
|
|
|
| 2 |
O |
-0.190 |
|
|
|
| 3 |
O |
-0.186 |
|
|
|
| 4 |
H |
0.209 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
-1.078 |
-1.707 |
0.000 |
2.019 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-19.889 |
0.688 |
0.000 |
| y |
0.688 |
-13.856 |
0.000 |
| z |
0.000 |
0.000 |
-16.102 |
|
| Traceless |
| | x | y | z |
| x |
-4.910 |
0.688 |
0.000 |
| y |
0.688 |
4.139 |
0.000 |
| z |
0.000 |
0.000 |
0.771 |
|
| Polar |
| 3z2-r2 | 1.542 |
| x2-y2 | -6.033 |
| 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 |
3.429 |
0.232 |
0.000 |
| y |
0.232 |
2.925 |
0.000 |
| z |
0.000 |
0.000 |
1.872 |
<r2> (average value of r
2) Å
2
| <r2> |
34.518 |
| (<r2>)1/2 |
5.875 |
Jump to
S1C1
Energy calculated at PBE1PBE/cc-pVTZ
| | hartrees |
| Energy at 0K | -188.969097 |
| Energy at 298.15K | -188.970188 |
| HF Energy | -188.969097 |
| Nuclear repulsion energy | 63.266371 |
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-pVTZ
| 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' |
3854 |
3704 |
128.00 |
|
|
|
| 2 |
A' |
1946 |
1871 |
237.52 |
|
|
|
| 3 |
A' |
1256 |
1207 |
269.37 |
|
|
|
| 4 |
A' |
1128 |
1084 |
44.50 |
|
|
|
| 5 |
A' |
630 |
606 |
4.07 |
|
|
|
| 6 |
A" |
555 |
533 |
86.31 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 4684.9 cm
-1
Scaled (by 0.961) Zero Point Vibrational Energy (zpe) 4502.2 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-pVTZ
Point Group is Cs
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
0.000 |
0.405 |
0.000 |
| O2 |
-0.939 |
-0.540 |
0.000 |
| O3 |
1.164 |
0.250 |
0.000 |
| H4 |
-1.801 |
-0.111 |
0.000 |
Atom - Atom Distances (Å)
| |
C1 |
O2 |
O3 |
H4 |
| C1 | | 1.3325 | 1.1748 | 1.8735 |
O2 | 1.3325 | | 2.2469 | 0.9625 | O3 | 1.1748 | 2.2469 | | 2.9872 | H4 | 1.8735 | 0.9625 | 2.9872 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| C1 |
O2 |
H4 |
108.358 |
|
O2 |
C1 |
O3 |
127.199 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at PBE1PBE/cc-pVTZ
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
0.094 |
|
|
|
| 2 |
O |
-0.157 |
|
|
|
| 3 |
O |
-0.161 |
|
|
|
| 4 |
H |
0.224 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
-3.015 |
0.278 |
0.000 |
3.028 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-13.766 |
-0.979 |
0.000 |
| y |
-0.979 |
-17.734 |
0.000 |
| z |
0.000 |
0.000 |
-16.141 |
|
| Traceless |
| | x | y | z |
| x |
3.172 |
-0.979 |
0.000 |
| y |
-0.979 |
-2.781 |
0.000 |
| z |
0.000 |
0.000 |
-0.391 |
|
| Polar |
| 3z2-r2 | -0.782 |
| x2-y2 | 3.968 |
| xy | -0.979 |
| xz | 0.000 |
| yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
3.866 |
0.162 |
0.000 |
| y |
0.162 |
2.383 |
0.000 |
| z |
0.000 |
0.000 |
1.891 |
<r2> (average value of r
2) Å
2
| <r2> |
34.894 |
| (<r2>)1/2 |
5.907 |