Jump to
S1C2
Energy calculated at HF/6-31G(2df,p)
| | hartrees |
| Energy at 0K | -151.101201 |
| Energy at 298.15K | |
| HF Energy | -151.101201 |
| Nuclear repulsion energy | 53.343160 |
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 HF/6-31G(2df,p)
| 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 |
3280 |
121.33 |
55.44 |
0.25 |
0.40 |
| 2 |
Σ |
2128 |
1927 |
135.89 |
97.64 |
0.34 |
0.51 |
| 3 |
Σ |
1403 |
1270 |
16.82 |
67.28 |
0.25 |
0.39 |
| 4 |
Π |
653 |
591 |
2.69 |
1.50 |
0.75 |
0.86 |
| 4 |
Π |
591 |
535 |
13.22 |
0.16 |
0.75 |
0.86 |
| 5 |
Π |
416 |
377 |
31.06 |
0.05 |
0.75 |
0.86 |
| 5 |
Π |
131i |
118i |
149.89 |
3.82 |
0.75 |
0.86 |
Unscaled Zero Point Vibrational Energy (zpe) 4341.4 cm
-1
Scaled (by 0.9055) Zero Point Vibrational Energy (zpe) 3931.1 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 HF/6-31G(2df,p)
Point Group is C∞v
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
0.000 |
0.000 |
0.023 |
| C2 |
0.000 |
0.000 |
-1.222 |
| O3 |
0.000 |
0.000 |
1.184 |
| H4 |
0.000 |
0.000 |
-2.275 |
Atom - Atom Distances (Å)
| |
C1 |
C2 |
O3 |
H4 |
| C1 | | 1.2448 | 1.1618 | 2.2979 |
C2 | 1.2448 | | 2.4066 | 1.0531 | O3 | 1.1618 | 2.4066 | | 3.4596 | H4 | 2.2979 | 1.0531 | 3.4596 | |
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 HF/6-31G(2df,p)
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
0.474 |
|
|
|
| 2 |
C |
-0.453 |
|
|
|
| 3 |
O |
-0.305 |
|
|
|
| 4 |
H |
0.284 |
|
|
|
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 |
-2.227 |
2.227 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-15.924 |
0.000 |
0.000 |
| y |
0.000 |
-17.532 |
0.000 |
| z |
0.000 |
0.000 |
-14.622 |
|
| Traceless |
| | x | y | z |
| x |
0.153 |
0.000 |
0.000 |
| y |
0.000 |
-2.258 |
0.000 |
| z |
0.000 |
0.000 |
2.106 |
|
| Polar |
| 3z2-r2 | 4.211 |
| x2-y2 | 1.608 |
| 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 |
1.779 |
0.000 |
0.000 |
| y |
0.000 |
1.811 |
0.000 |
| z |
0.000 |
0.000 |
5.501 |
<r2> (average value of r
2) Å
2
| <r2> |
35.374 |
| (<r2>)1/2 |
5.948 |
Jump to
S1C1
Energy calculated at HF/6-31G(2df,p)
| | hartrees |
| Energy at 0K | -151.101357 |
| Energy at 298.15K | |
| HF Energy | -151.101357 |
| Nuclear repulsion energy | 53.303685 |
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 HF/6-31G(2df,p)
| 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' |
3564 |
3227 |
85.44 |
63.70 |
0.29 |
0.45 |
| 2 |
A' |
2168 |
1963 |
296.36 |
79.18 |
0.22 |
0.36 |
| 3 |
A' |
1381 |
1250 |
7.27 |
46.39 |
0.27 |
0.43 |
| 4 |
A' |
646 |
585 |
10.96 |
15.00 |
0.51 |
0.68 |
| 5 |
A' |
207 |
188 |
286.42 |
4.09 |
0.47 |
0.64 |
| 6 |
A" |
573 |
519 |
17.65 |
23.70 |
0.75 |
0.86 |
Unscaled Zero Point Vibrational Energy (zpe) 4268.9 cm
-1
Scaled (by 0.9055) Zero Point Vibrational Energy (zpe) 3865.5 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 HF/6-31G(2df,p)
Point Group is Cs
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
0.000 |
0.037 |
0.000 |
| C2 |
0.800 |
-0.944 |
0.000 |
| O3 |
-0.825 |
0.841 |
0.000 |
| H4 |
1.799 |
-1.290 |
0.000 |
Atom - Atom Distances (Å)
| |
C1 |
C2 |
O3 |
H4 |
| C1 | | 1.2658 | 1.1517 | 2.2358 |
C2 | 1.2658 | | 2.4135 | 1.0580 | O3 | 1.1517 | 2.4135 | | 3.3803 | H4 | 2.2358 | 1.0580 | 3.3803 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| C1 |
C2 |
H4 |
148.241 |
|
C2 |
C1 |
O3 |
173.449 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at HF/6-31G(2df,p)
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
0.516 |
|
|
|
| 2 |
C |
-0.471 |
|
|
|
| 3 |
O |
-0.292 |
|
|
|
| 4 |
H |
0.248 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
1.810 |
-0.576 |
0.000 |
1.900 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-14.972 |
-0.750 |
0.000 |
| y |
-0.750 |
-18.310 |
0.000 |
| z |
0.000 |
0.000 |
-15.981 |
|
| Traceless |
| | x | y | z |
| x |
2.174 |
-0.750 |
0.000 |
| y |
-0.750 |
-2.834 |
0.000 |
| z |
0.000 |
0.000 |
0.660 |
|
| Polar |
| 3z2-r2 | 1.319 |
| x2-y2 | 3.339 |
| xy | -0.750 |
| xz | 0.000 |
| yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
3.499 |
-1.788 |
0.000 |
| y |
-1.788 |
4.005 |
0.000 |
| z |
0.000 |
0.000 |
2.465 |
<r2> (average value of r
2) Å
2
| <r2> |
35.450 |
| (<r2>)1/2 |
5.954 |