Jump to
S1C2
Energy calculated at ROHF/6-31+G**
| | hartrees |
| Energy at 0K | -151.078629 |
| Energy at 298.15K | |
| HF Energy | -151.078629 |
| Nuclear repulsion energy | 53.199321 |
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/6-31+G**
| 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 |
3656 |
3129 |
192.16 |
|
|
|
| 2 |
Σ |
2350 |
2011 |
864.74 |
|
|
|
| 3 |
Σ |
1424 |
1219 |
20.91 |
|
|
|
| 4 |
Π |
628 |
537 |
1.73 |
|
|
|
| 4 |
Π |
596 |
510 |
18.13 |
|
|
|
| 5 |
Π |
308 |
264 |
52.63 |
|
|
|
| 5 |
Π |
242i |
207i |
223.01 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 4359.5 cm
-1
Scaled (by 0.8559) Zero Point Vibrational Energy (zpe) 3731.3 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/6-31+G**
Point Group is C∞v
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
0.000 |
0.000 |
0.029 |
| C2 |
0.000 |
0.000 |
-1.230 |
| O3 |
0.000 |
0.000 |
1.186 |
| H4 |
0.000 |
0.000 |
-2.285 |
Atom - Atom Distances (Å)
| |
C1 |
C2 |
O3 |
H4 |
| C1 | | 1.2589 | 1.1571 | 2.3141 |
C2 | 1.2589 | | 2.4160 | 1.0552 | O3 | 1.1571 | 2.4160 | | 3.4712 | H4 | 2.3141 | 1.0552 | 3.4712 | |
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/6-31+G**
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
0.216 |
|
|
|
| 2 |
C |
-0.039 |
|
|
|
| 3 |
O |
-0.526 |
|
|
|
| 4 |
H |
0.349 |
|
|
|
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 |
-2.589 |
2.589 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-16.306 |
0.000 |
0.000 |
| y |
0.000 |
-18.231 |
0.000 |
| z |
0.000 |
0.000 |
-15.781 |
|
| Traceless |
| | x | y | z |
| x |
0.701 |
0.000 |
0.000 |
| y |
0.000 |
-2.188 |
0.000 |
| z |
0.000 |
0.000 |
1.487 |
|
| Polar |
| 3z2-r2 | 2.974 |
| x2-y2 | 1.926 |
| 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> |
36.033 |
| (<r2>)1/2 |
6.003 |
Jump to
S1C1
Energy calculated at ROHF/6-31+G**
| | hartrees |
| Energy at 0K | -151.079827 |
| Energy at 298.15K | |
| HF Energy | -151.079827 |
| Nuclear repulsion energy | 53.046276 |
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/6-31+G**
| 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' |
3555 |
3043 |
77.52 |
|
|
|
| 2 |
A' |
2323 |
1988 |
983.21 |
|
|
|
| 3 |
A' |
1350 |
1155 |
0.44 |
|
|
|
| 4 |
A' |
619 |
530 |
21.53 |
|
|
|
| 5 |
A' |
405 |
347 |
438.05 |
|
|
|
| 6 |
A" |
561 |
481 |
22.94 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 4406.8 cm
-1
Scaled (by 0.8559) Zero Point Vibrational Energy (zpe) 3771.8 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/6-31+G**
Point Group is Cs
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
0.000 |
0.047 |
0.000 |
| C2 |
0.811 |
-0.960 |
0.000 |
| O3 |
-0.841 |
0.825 |
0.000 |
| H4 |
1.861 |
-1.122 |
0.000 |
Atom - Atom Distances (Å)
| |
C1 |
C2 |
O3 |
H4 |
| C1 | | 1.2933 | 1.1457 | 2.1978 |
C2 | 1.2933 | | 2.4325 | 1.0622 | O3 | 1.1457 | 2.4325 | | 3.3306 | H4 | 2.1978 | 1.0622 | 3.3306 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| C1 |
C2 |
H4 |
137.617 |
|
C2 |
C1 |
O3 |
171.620 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at ROHF/6-31+G**
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
0.409 |
|
|
|
| 2 |
C |
-0.235 |
|
|
|
| 3 |
O |
-0.437 |
|
|
|
| 4 |
H |
0.264 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
2.100 |
-0.070 |
0.000 |
2.101 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-15.278 |
-0.030 |
0.002 |
| y |
-0.030 |
-20.521 |
-0.004 |
| z |
0.002 |
-0.004 |
-16.442 |
|
| Traceless |
| | x | y | z |
| x |
3.204 |
-0.030 |
0.002 |
| y |
-0.030 |
-4.661 |
-0.004 |
| z |
0.002 |
-0.004 |
1.458 |
|
| Polar |
| 3z2-r2 | 2.915 |
| x2-y2 | 5.243 |
| xy | -0.030 |
| xz | 0.002 |
| yz | -0.004 |
|
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> |
36.198 |
| (<r2>)1/2 |
6.016 |