Jump to
S1C2
Energy calculated at ROHF/6-311G**
| | hartrees |
| Energy at 0K | -151.114947 |
| Energy at 298.15K | |
| HF Energy | -151.114947 |
| Nuclear repulsion energy | 53.482668 |
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/6-311G**
| Mode Number |
Symmetry |
Frequency (cm-1) |
Scaled Frequency (cm-1) |
IR Intensities (km mol-1) |
Raman Act (Å4/u) |
Dep P |
Dep U |
| 1 |
Σ |
3622 |
3305 |
198.89 |
|
|
|
| 2 |
Σ |
2361 |
2155 |
816.07 |
|
|
|
| 3 |
Σ |
1419 |
1295 |
18.82 |
|
|
|
| 4 |
Π |
665 |
607 |
4.53 |
|
|
|
| 4 |
Π |
622 |
568 |
18.16 |
|
|
|
| 5 |
Π |
302 |
275 |
38.99 |
|
|
|
| 5 |
Π |
277i |
253i |
186.30 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 4356.7 cm
-1
Scaled (by 0.9126) Zero Point Vibrational Energy (zpe) 3975.9 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 ROHF/6-311G**
Point Group is C∞v
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
0.000 |
0.000 |
0.031 |
| C2 |
0.000 |
0.000 |
-1.224 |
| O3 |
0.000 |
0.000 |
1.179 |
| H4 |
0.000 |
0.000 |
-2.277 |
Atom - Atom Distances (Å)
| |
C1 |
C2 |
O3 |
H4 |
| C1 | | 1.2558 | 1.1478 | 2.3086 |
C2 | 1.2558 | | 2.4036 | 1.0527 | O3 | 1.1478 | 2.4036 | | 3.4564 | H4 | 2.3086 | 1.0527 | 3.4564 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| C1 |
C2 |
H4 |
180.000 |
|
C2 |
C1 |
O3 |
180.000 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at ROHF/6-311G**
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
0.365 |
|
|
|
| 2 |
C |
-0.189 |
|
|
|
| 3 |
O |
-0.347 |
|
|
|
| 4 |
H |
0.171 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
0.000 |
0.000 |
-2.370 |
2.370 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-16.097 |
0.000 |
0.000 |
| y |
0.000 |
-17.931 |
0.000 |
| z |
0.000 |
0.000 |
-15.559 |
|
| Traceless |
| | x | y | z |
| x |
0.648 |
0.000 |
0.000 |
| y |
0.000 |
-2.103 |
0.000 |
| z |
0.000 |
0.000 |
1.455 |
|
| Polar |
| 3z2-r2 | 2.910 |
| x2-y2 | 1.834 |
| xy | 0.000 |
| xz | 0.000 |
| yz | 0.000 |
|
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> |
35.636 |
| (<r2>)1/2 |
5.970 |
Jump to
S1C1
Energy calculated at ROHF/6-311G**
| | hartrees |
| Energy at 0K | -151.116230 |
| Energy at 298.15K | |
| HF Energy | -151.116230 |
| Nuclear repulsion energy | 53.297773 |
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/6-311G**
| 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' |
3498 |
3192 |
73.02 |
|
|
|
| 2 |
A' |
2337 |
2132 |
922.63 |
|
|
|
| 3 |
A' |
1336 |
1220 |
0.26 |
|
|
|
| 4 |
A' |
657 |
599 |
31.90 |
|
|
|
| 5 |
A' |
390 |
356 |
400.25 |
|
|
|
| 6 |
A" |
590 |
538 |
28.56 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 4403.7 cm
-1
Scaled (by 0.9126) Zero Point Vibrational Energy (zpe) 4018.8 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/6-311G**
Point Group is Cs
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
0.000 |
0.046 |
0.000 |
| C2 |
0.707 |
-1.036 |
0.000 |
| O3 |
-0.748 |
0.901 |
0.000 |
| H4 |
1.744 |
-1.268 |
0.000 |
Atom - Atom Distances (Å)
| |
C1 |
C2 |
O3 |
H4 |
| C1 | | 1.2925 | 1.1364 | 2.1840 |
C2 | 1.2925 | | 2.4229 | 1.0630 | O3 | 1.1364 | 2.4229 | | 3.3044 | H4 | 2.1840 | 1.0630 | 3.3044 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| C1 |
C2 |
H4 |
135.780 |
|
C2 |
C1 |
O3 |
171.977 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at ROHF/6-311G**
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
0.399 |
|
|
|
| 2 |
C |
-0.269 |
|
|
|
| 3 |
O |
-0.318 |
|
|
|
| 4 |
H |
0.188 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
1.878 |
-0.114 |
0.000 |
1.882 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-15.169 |
-0.415 |
0.001 |
| y |
-0.415 |
-20.174 |
-0.003 |
| z |
0.001 |
-0.003 |
-16.240 |
|
| Traceless |
| | x | y | z |
| x |
3.038 |
-0.415 |
0.001 |
| y |
-0.415 |
-4.469 |
-0.003 |
| z |
0.001 |
-0.003 |
1.432 |
|
| Polar |
| 3z2-r2 | 2.863 |
| x2-y2 | 5.005 |
| xy | -0.415 |
| xz | 0.001 |
| 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> |
35.817 |
| (<r2>)1/2 |
5.985 |