Jump to
S1C2
Energy calculated at PBE1PBE/6-31G
| | hartrees |
| Energy at 0K | -188.809864 |
| Energy at 298.15K | -188.810923 |
| HF Energy | -188.809864 |
| Nuclear repulsion energy | 62.040217 |
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/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' |
3473 |
3320 |
5.73 |
|
|
|
| 2 |
A' |
1801 |
1721 |
294.88 |
|
|
|
| 3 |
A' |
1290 |
1233 |
3.04 |
|
|
|
| 4 |
A' |
1033 |
987 |
176.92 |
|
|
|
| 5 |
A' |
578 |
552 |
43.32 |
|
|
|
| 6 |
A" |
584 |
559 |
186.44 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 4379.0 cm
-1
Scaled (by 0.9559) Zero Point Vibrational Energy (zpe) 4185.9 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/6-31G
Point Group is Cs
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
0.000 |
0.444 |
0.000 |
| O2 |
-1.074 |
-0.361 |
0.000 |
| O3 |
1.183 |
0.194 |
0.000 |
| H4 |
-0.871 |
-1.328 |
0.000 |
Atom - Atom Distances (Å)
| |
C1 |
O2 |
O3 |
H4 |
| C1 | | 1.3426 | 1.2094 | 1.9744 |
O2 | 1.3426 | | 2.3246 | 0.9879 | O3 | 1.2094 | 2.3246 | | 2.5561 | H4 | 1.9744 | 0.9879 | 2.5561 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| C1 |
O2 |
H4 |
114.967 |
|
O2 |
C1 |
O3 |
131.189 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at PBE1PBE/6-31G
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
0.499 |
|
|
|
| 2 |
O |
-0.551 |
|
|
|
| 3 |
O |
-0.351 |
|
|
|
| 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 |
| |
-1.002 |
-2.090 |
0.000 |
2.317 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-21.374 |
1.016 |
0.000 |
| y |
1.016 |
-13.406 |
0.000 |
| z |
0.000 |
0.000 |
-16.011 |
|
| Traceless |
| | x | y | z |
| x |
-6.665 |
1.016 |
0.000 |
| y |
1.016 |
5.287 |
0.000 |
| z |
0.000 |
0.000 |
1.379 |
|
| Polar |
| 3z2-r2 | 2.757 |
| x2-y2 | -7.968 |
| xy | 1.016 |
| xz | 0.000 |
| yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
3.154 |
0.339 |
0.000 |
| y |
0.339 |
2.382 |
0.000 |
| z |
0.000 |
0.000 |
1.162 |
<r2> (average value of r
2) Å
2
| <r2> |
36.054 |
| (<r2>)1/2 |
6.005 |
Jump to
S1C1
Energy calculated at PBE1PBE/6-31G
| | hartrees |
| Energy at 0K | -188.813736 |
| Energy at 298.15K | -188.814785 |
| HF Energy | -188.813736 |
| Nuclear repulsion energy | 61.880000 |
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/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' |
3727 |
3563 |
98.53 |
|
|
|
| 2 |
A' |
1856 |
1774 |
185.65 |
|
|
|
| 3 |
A' |
1192 |
1139 |
235.67 |
|
|
|
| 4 |
A' |
1069 |
1022 |
100.01 |
|
|
|
| 5 |
A' |
605 |
579 |
7.92 |
|
|
|
| 6 |
A" |
546 |
522 |
147.06 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 4497.5 cm
-1
Scaled (by 0.9559) Zero Point Vibrational Energy (zpe) 4299.2 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/6-31G
Point Group is Cs
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
0.000 |
0.418 |
0.000 |
| O2 |
-0.959 |
-0.549 |
0.000 |
| O3 |
1.191 |
0.257 |
0.000 |
| H4 |
-1.856 |
-0.170 |
0.000 |
Atom - Atom Distances (Å)
| |
C1 |
O2 |
O3 |
H4 |
| C1 | | 1.3621 | 1.2019 | 1.9471 |
O2 | 1.3621 | | 2.2966 | 0.9742 | O3 | 1.2019 | 2.2966 | | 3.0773 | H4 | 1.9471 | 0.9742 | 3.0773 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| C1 |
O2 |
H4 |
111.831 |
|
O2 |
C1 |
O3 |
127.088 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at PBE1PBE/6-31G
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
0.453 |
|
|
|
| 2 |
O |
-0.543 |
|
|
|
| 3 |
O |
-0.335 |
|
|
|
| 4 |
H |
0.425 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
-3.399 |
0.566 |
0.000 |
3.446 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-13.737 |
-1.208 |
0.000 |
| y |
-1.208 |
-18.223 |
0.000 |
| z |
0.000 |
0.000 |
-16.026 |
|
| Traceless |
| | x | y | z |
| x |
3.387 |
-1.208 |
0.000 |
| y |
-1.208 |
-3.341 |
0.000 |
| z |
0.000 |
0.000 |
-0.046 |
|
| Polar |
| 3z2-r2 | -0.092 |
| x2-y2 | 4.486 |
| xy | -1.208 |
| xz | 0.000 |
| yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
3.684 |
0.238 |
0.000 |
| y |
0.238 |
1.782 |
0.000 |
| z |
0.000 |
0.000 |
1.180 |
<r2> (average value of r
2) Å
2
| <r2> |
36.167 |
| (<r2>)1/2 |
6.014 |