Jump to
S1C2
Energy calculated at B2PLYP/aug-cc-pVTZ
| | hartrees |
| Energy at 0K | -189.053919 |
| Energy at 298.15K | -189.055003 |
| HF Energy | -188.851884 |
| Nuclear repulsion energy | 63.128906 |
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 B2PLYP/aug-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' |
3616 |
3475 |
28.73 |
|
|
|
| 2 |
A' |
1841 |
1769 |
313.76 |
|
|
|
| 3 |
A' |
1299 |
1248 |
0.28 |
|
|
|
| 4 |
A' |
1069 |
1027 |
178.50 |
|
|
|
| 5 |
A' |
599 |
576 |
31.30 |
|
|
|
| 6 |
A" |
580 |
558 |
105.61 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 4501.2 cm
-1
Scaled (by 0.961) Zero Point Vibrational Energy (zpe) 4325.6 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 B2PLYP/aug-cc-pVTZ
Point Group is Cs
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
0.000 |
0.442 |
0.000 |
| O2 |
-1.062 |
-0.357 |
0.000 |
| O3 |
1.158 |
0.186 |
0.000 |
| H4 |
-0.763 |
-1.285 |
0.000 |
Atom - Atom Distances (Å)
| |
C1 |
O2 |
O3 |
H4 |
| C1 | | 1.3288 | 1.1857 | 1.8873 |
O2 | 1.3288 | | 2.2856 | 0.9753 | O3 | 1.1857 | 2.2856 | | 2.4191 | H4 | 1.8873 | 0.9753 | 2.4191 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| C1 |
O2 |
H4 |
109.023 |
|
O2 |
C1 |
O3 |
130.642 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at B2PLYP/aug-cc-pVTZ
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
0.234 |
|
|
|
| 2 |
O |
-0.170 |
|
|
|
| 3 |
O |
-0.257 |
|
|
|
| 4 |
H |
0.193 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
-1.000 |
-1.646 |
0.000 |
1.926 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-20.382 |
0.753 |
0.000 |
| y |
0.753 |
-14.253 |
0.000 |
| z |
0.000 |
0.000 |
-16.526 |
|
| Traceless |
| | x | y | z |
| x |
-4.992 |
0.753 |
0.000 |
| y |
0.753 |
4.201 |
0.000 |
| z |
0.000 |
0.000 |
0.791 |
|
| Polar |
| 3z2-r2 | 1.583 |
| x2-y2 | -6.129 |
| xy | 0.753 |
| xz | 0.000 |
| yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
4.028 |
0.193 |
0.000 |
| y |
0.193 |
3.460 |
0.000 |
| z |
0.000 |
0.000 |
2.441 |
<r2> (average value of r
2) Å
2
| <r2> |
35.102 |
| (<r2>)1/2 |
5.925 |
Jump to
S1C1
Energy calculated at B2PLYP/aug-cc-pVTZ
| | hartrees |
| Energy at 0K | -189.057039 |
| Energy at 298.15K | -189.058108 |
| HF Energy | -188.854241 |
| Nuclear repulsion energy | 62.889900 |
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 B2PLYP/aug-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' |
3801 |
3653 |
130.72 |
|
|
|
| 2 |
A' |
1878 |
1805 |
226.45 |
|
|
|
| 3 |
A' |
1244 |
1195 |
236.63 |
|
|
|
| 4 |
A' |
1080 |
1038 |
79.28 |
|
|
|
| 5 |
A' |
618 |
594 |
4.90 |
|
|
|
| 6 |
A" |
544 |
523 |
85.44 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 4582.0 cm
-1
Scaled (by 0.961) Zero Point Vibrational Energy (zpe) 4403.3 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 B2PLYP/aug-cc-pVTZ
Point Group is Cs
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
0.000 |
0.410 |
0.000 |
| O2 |
-0.944 |
-0.546 |
0.000 |
| O3 |
1.170 |
0.253 |
0.000 |
| H4 |
-1.809 |
-0.118 |
0.000 |
Atom - Atom Distances (Å)
| |
C1 |
O2 |
O3 |
H4 |
| C1 | | 1.3434 | 1.1806 | 1.8846 |
O2 | 1.3434 | | 2.2599 | 0.9651 | O3 | 1.1806 | 2.2599 | | 3.0022 | H4 | 1.8846 | 0.9651 | 3.0022 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| C1 |
O2 |
H4 |
108.333 |
|
O2 |
C1 |
O3 |
126.990 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at B2PLYP/aug-cc-pVTZ
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
0.204 |
|
|
|
| 2 |
O |
-0.195 |
|
|
|
| 3 |
O |
-0.246 |
|
|
|
| 4 |
H |
0.237 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
-2.922 |
0.329 |
0.000 |
2.940 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-14.232 |
-0.957 |
0.000 |
| y |
-0.957 |
-18.282 |
0.000 |
| z |
0.000 |
0.000 |
-16.587 |
|
| Traceless |
| | x | y | z |
| x |
3.202 |
-0.957 |
0.000 |
| y |
-0.957 |
-2.873 |
0.000 |
| z |
0.000 |
0.000 |
-0.329 |
|
| Polar |
| 3z2-r2 | -0.659 |
| x2-y2 | 4.050 |
| xy | -0.957 |
| xz | 0.000 |
| yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
4.431 |
0.166 |
0.000 |
| y |
0.166 |
3.057 |
0.000 |
| z |
0.000 |
0.000 |
2.483 |
<r2> (average value of r
2) Å
2
| <r2> |
35.495 |
| (<r2>)1/2 |
5.958 |