Jump to
S1C2
Energy calculated at ROHF/3-21G*
| | hartrees |
| Energy at 0K | -187.063372 |
| Energy at 298.15K | -187.064489 |
| HF Energy | -187.063372 |
| Nuclear repulsion energy | 62.929492 |
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 ROHF/3-21G*
| 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' |
3769 |
3424 |
71.76 |
|
|
|
| 2 |
A' |
1989 |
1807 |
353.49 |
|
|
|
| 3 |
A' |
1402 |
1274 |
14.77 |
|
|
|
| 4 |
A' |
1124 |
1021 |
246.73 |
|
|
|
| 5 |
A' |
645 |
586 |
66.82 |
|
|
|
| 6 |
A" |
582 |
528 |
238.83 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 4755.4 cm
-1
Scaled (by 0.9085) Zero Point Vibrational Energy (zpe) 4320.3 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 ROHF/3-21G*
Point Group is Cs
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
0.000 |
0.438 |
0.000 |
| O2 |
-1.056 |
-0.378 |
0.000 |
| O3 |
1.161 |
0.216 |
0.000 |
| H4 |
-0.839 |
-1.328 |
0.000 |
Atom - Atom Distances (Å)
| |
C1 |
O2 |
O3 |
H4 |
| C1 | | 1.3342 | 1.1819 | 1.9549 |
O2 | 1.3342 | | 2.2950 | 0.9745 | O3 | 1.1819 | 2.2950 | | 2.5267 | H4 | 1.9549 | 0.9745 | 2.5267 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| C1 |
O2 |
H4 |
114.829 |
|
O2 |
C1 |
O3 |
131.506 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at ROHF/3-21G*
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
0.818 |
|
|
|
| 2 |
O |
-0.692 |
|
|
|
| 3 |
O |
-0.551 |
|
|
|
| 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 |
| |
-1.180 |
-1.810 |
0.000 |
2.160 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-21.940 |
0.623 |
-0.002 |
| y |
0.623 |
-12.844 |
-0.003 |
| z |
-0.002 |
-0.003 |
-15.627 |
|
| Traceless |
| | x | y | z |
| x |
-7.705 |
0.623 |
-0.002 |
| y |
0.623 |
5.940 |
-0.003 |
| z |
-0.002 |
-0.003 |
1.764 |
|
| Polar |
| 3z2-r2 | 3.529 |
| x2-y2 | -9.097 |
| xy | 0.623 |
| xz | -0.002 |
| yz | -0.003 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
0.000 |
0.000 |
0.000 |
| y |
0.000 |
0.000 |
0.000 |
| z |
0.000 |
0.000 |
0.000 |
<r2> (average value of r
2) Å
2
| <r2> |
35.330 |
| (<r2>)1/2 |
5.944 |
Jump to
S1C1
Energy calculated at ROHF/3-21G*
| | hartrees |
| Energy at 0K | -187.063095 |
| Energy at 298.15K | -187.064157 |
| HF Energy | -187.063095 |
| Nuclear repulsion energy | 62.761316 |
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 ROHF/3-21G*
| 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' |
3897 |
3541 |
139.22 |
|
|
|
| 2 |
A' |
2057 |
1868 |
264.02 |
|
|
|
| 3 |
A' |
1281 |
1164 |
297.27 |
|
|
|
| 4 |
A' |
1151 |
1046 |
100.59 |
|
|
|
| 5 |
A' |
671 |
610 |
9.65 |
|
|
|
| 6 |
A" |
490 |
445 |
145.44 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 4773.4 cm
-1
Scaled (by 0.9085) Zero Point Vibrational Energy (zpe) 4336.7 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 ROHF/3-21G*
Point Group is Cs
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
0.000 |
0.398 |
0.000 |
| O2 |
-0.941 |
-0.564 |
0.000 |
| O3 |
1.171 |
0.292 |
0.000 |
| H4 |
-1.842 |
-0.218 |
0.000 |
Atom - Atom Distances (Å)
| |
C1 |
O2 |
O3 |
H4 |
| C1 | | 1.3451 | 1.1755 | 1.9425 |
O2 | 1.3451 | | 2.2782 | 0.9657 | O3 | 1.1755 | 2.2782 | | 3.0560 | H4 | 1.9425 | 0.9657 | 3.0560 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| C1 |
O2 |
H4 |
113.401 |
|
O2 |
C1 |
O3 |
129.207 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at ROHF/3-21G*
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
0.778 |
|
|
|
| 2 |
O |
-0.683 |
|
|
|
| 3 |
O |
-0.531 |
|
|
|
| 4 |
H |
0.437 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
-3.685 |
0.858 |
0.000 |
3.783 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-14.243 |
-1.490 |
-0.004 |
| y |
-1.490 |
-17.887 |
-0.001 |
| z |
-0.004 |
-0.001 |
-15.636 |
|
| Traceless |
| | x | y | z |
| x |
2.518 |
-1.490 |
-0.004 |
| y |
-1.490 |
-2.947 |
-0.001 |
| z |
-0.004 |
-0.001 |
0.429 |
|
| Polar |
| 3z2-r2 | 0.857 |
| x2-y2 | 3.644 |
| xy | -1.490 |
| xz | -0.004 |
| yz | -0.001 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
0.000 |
0.000 |
0.000 |
| y |
0.000 |
0.000 |
0.000 |
| z |
0.000 |
0.000 |
0.000 |
<r2> (average value of r
2) Å
2
| <r2> |
35.603 |
| (<r2>)1/2 |
5.967 |