Jump to
S1C2
Energy calculated at ROHF/TZVP
| | hartrees |
| Energy at 0K | -151.127358 |
| Energy at 298.15K | |
| HF Energy | -151.127358 |
| Nuclear repulsion energy | 53.542193 |
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/TZVP
| 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 |
3624 |
3624 |
207.09 |
|
|
|
| 2 |
Σ |
2351 |
2351 |
878.28 |
|
|
|
| 3 |
Σ |
1424 |
1424 |
19.03 |
|
|
|
| 4 |
Π |
641 |
641 |
2.16 |
|
|
|
| 4 |
Π |
596 |
596 |
15.53 |
|
|
|
| 5 |
Π |
254 |
254 |
48.91 |
|
|
|
| 5 |
Π |
301i |
301i |
206.81 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 4294.5 cm
-1
Scaled (by 1) Zero Point Vibrational Energy (zpe) 4294.5 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/TZVP
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 |
-1.222 |
| O3 |
0.000 |
0.000 |
1.178 |
| H4 |
0.000 |
0.000 |
-2.275 |
Atom - Atom Distances (Å)
| |
C1 |
C2 |
O3 |
H4 |
| C1 | | 1.2530 | 1.1475 | 2.3054 |
C2 | 1.2530 | | 2.4004 | 1.0524 | O3 | 1.1475 | 2.4004 | | 3.4528 | H4 | 2.3054 | 1.0524 | 3.4528 | |
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/TZVP
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
0.412 |
|
|
|
| 2 |
C |
-0.296 |
|
|
|
| 3 |
O |
-0.356 |
|
|
|
| 4 |
H |
0.240 |
|
|
|
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 |
-2.479 |
2.479 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-18.080 |
0.000 |
0.000 |
| y |
0.000 |
-16.176 |
0.000 |
| z |
0.000 |
0.000 |
-15.877 |
|
| Traceless |
| | x | y | z |
| x |
-2.054 |
0.000 |
0.000 |
| y |
0.000 |
0.802 |
0.000 |
| z |
0.000 |
0.000 |
1.252 |
|
| Polar |
| 3z2-r2 | 2.503 |
| x2-y2 | -1.904 |
| 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> |
35.686 |
| (<r2>)1/2 |
5.974 |
Jump to
S1C1
Energy calculated at ROHF/TZVP
| | hartrees |
| Energy at 0K | -151.128174 |
| Energy at 298.15K | |
| HF Energy | -151.128174 |
| Nuclear repulsion energy | 53.418999 |
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/TZVP
| 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' |
3538 |
3538 |
103.78 |
|
|
|
| 2 |
A' |
2330 |
2330 |
978.41 |
|
|
|
| 3 |
A' |
1367 |
1367 |
1.26 |
|
|
|
| 4 |
A' |
642 |
642 |
17.18 |
|
|
|
| 5 |
A' |
336 |
336 |
409.41 |
|
|
|
| 6 |
A" |
577 |
577 |
26.01 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 4394.9 cm
-1
Scaled (by 1) Zero Point Vibrational Energy (zpe) 4394.9 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/TZVP
Point Group is Cs
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
0.000 |
0.044 |
0.000 |
| C2 |
0.734 |
-1.004 |
0.000 |
| O3 |
-0.769 |
0.884 |
0.000 |
| H4 |
1.747 |
-1.315 |
0.000 |
Atom - Atom Distances (Å)
| |
C1 |
C2 |
O3 |
H4 |
| C1 | | 1.2798 | 1.1386 | 2.2131 |
C2 | 1.2798 | | 2.4133 | 1.0590 | O3 | 1.1386 | 2.4133 | | 3.3411 | H4 | 2.2131 | 1.0590 | 3.3411 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| C1 |
C2 |
H4 |
142.089 |
|
C2 |
C1 |
O3 |
172.526 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at ROHF/TZVP
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
0.498 |
|
|
|
| 2 |
C |
-0.343 |
|
|
|
| 3 |
O |
-0.329 |
|
|
|
| 4 |
H |
0.174 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
2.035 |
-0.424 |
0.000 |
2.079 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-15.397 |
-0.538 |
0.001 |
| y |
-0.538 |
-19.941 |
-0.004 |
| z |
0.001 |
-0.004 |
-16.276 |
|
| Traceless |
| | x | y | z |
| x |
2.712 |
-0.538 |
0.001 |
| y |
-0.538 |
-4.105 |
-0.004 |
| z |
0.001 |
-0.004 |
1.393 |
|
| Polar |
| 3z2-r2 | 2.785 |
| x2-y2 | 4.544 |
| xy | -0.538 |
| xz | 0.001 |
| 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> |
35.801 |
| (<r2>)1/2 |
5.983 |