Jump to
S1C2
Energy calculated at B1B95/6-311G**
| | hartrees |
| Energy at 0K | -151.906450 |
| Energy at 298.15K | |
| HF Energy | -151.906450 |
| Nuclear repulsion energy | 52.747694 |
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 B1B95/6-311G**
| 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 |
3493 |
3353 |
120.14 |
43.71 |
0.27 |
0.43 |
| 2 |
Σ |
2134 |
2049 |
228.13 |
2.62 |
0.67 |
0.80 |
| 3 |
Σ |
1329 |
1276 |
25.30 |
32.61 |
0.23 |
0.38 |
| 4 |
Π |
584 |
561 |
0.08 |
1.38 |
0.75 |
0.86 |
| 4 |
Π |
539 |
518 |
15.41 |
1.71 |
0.75 |
0.86 |
| 5 |
Π |
466 |
447 |
19.11 |
0.12 |
0.75 |
0.86 |
| 5 |
Π |
304i |
292i |
139.81 |
6.25 |
0.75 |
0.86 |
Unscaled Zero Point Vibrational Energy (zpe) 4120.9 cm
-1
Scaled (by 0.9601) Zero Point Vibrational Energy (zpe) 3956.5 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 B1B95/6-311G**
Point Group is C∞v
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
0.000 |
0.000 |
0.020 |
| C2 |
0.000 |
0.000 |
-1.235 |
| O3 |
0.000 |
0.000 |
1.198 |
| H4 |
0.000 |
0.000 |
-2.295 |
Atom - Atom Distances (Å)
| |
C1 |
C2 |
O3 |
H4 |
| C1 | | 1.2549 | 1.1786 | 2.3152 |
C2 | 1.2549 | | 2.4335 | 1.0603 | O3 | 1.1786 | 2.4335 | | 3.4938 | H4 | 2.3152 | 1.0603 | 3.4938 | |
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 B1B95/6-311G**
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
0.207 |
|
|
|
| 2 |
C |
-0.139 |
|
|
|
| 3 |
O |
-0.229 |
|
|
|
| 4 |
H |
0.162 |
|
|
|
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 |
-2.065 |
2.065 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-17.688 |
0.000 |
0.000 |
| y |
0.000 |
-15.992 |
0.000 |
| z |
0.000 |
0.000 |
-14.646 |
|
| Traceless |
| | x | y | z |
| x |
-2.369 |
0.000 |
0.000 |
| y |
0.000 |
0.175 |
0.000 |
| z |
0.000 |
0.000 |
2.194 |
|
| Polar |
| 3z2-r2 | 4.389 |
| x2-y2 | -1.696 |
| 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 |
1.707 |
0.000 |
0.000 |
| y |
0.000 |
1.606 |
0.000 |
| z |
0.000 |
0.000 |
5.534 |
<r2> (average value of r
2) Å
2
| <r2> |
35.975 |
| (<r2>)1/2 |
5.998 |
Jump to
S1C1
Energy calculated at B1B95/6-311G**
| | hartrees |
| Energy at 0K | -151.907805 |
| Energy at 298.15K | |
| HF Energy | -151.907805 |
| Nuclear repulsion energy | 52.637318 |
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 B1B95/6-311G**
| 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' |
3382 |
3247 |
50.66 |
70.07 |
0.35 |
0.52 |
| 2 |
A' |
2127 |
2042 |
309.52 |
3.16 |
0.50 |
0.67 |
| 3 |
A' |
1289 |
1238 |
8.59 |
29.35 |
0.29 |
0.44 |
| 4 |
A' |
572 |
549 |
6.01 |
4.29 |
0.75 |
0.85 |
| 5 |
A' |
422 |
405 |
235.94 |
6.48 |
0.15 |
0.27 |
| 6 |
A" |
513 |
492 |
4.62 |
1.03 |
0.75 |
0.86 |
Unscaled Zero Point Vibrational Energy (zpe) 4151.9 cm
-1
Scaled (by 0.9601) Zero Point Vibrational Energy (zpe) 3986.3 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 B1B95/6-311G**
Point Group is Cs
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
0.000 |
0.043 |
0.000 |
| C2 |
1.024 |
-0.729 |
0.000 |
| O3 |
-1.029 |
0.598 |
0.000 |
| H4 |
2.091 |
-0.664 |
0.000 |
Atom - Atom Distances (Å)
| |
C1 |
C2 |
O3 |
H4 |
| C1 | | 1.2825 | 1.1691 | 2.2074 |
C2 | 1.2825 | | 2.4445 | 1.0695 | O3 | 1.1691 | 2.4445 | | 3.3657 | H4 | 2.2074 | 1.0695 | 3.3657 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| C1 |
C2 |
H4 |
139.446 |
|
C2 |
C1 |
O3 |
171.274 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at B1B95/6-311G**
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
0.237 |
|
|
|
| 2 |
C |
-0.207 |
|
|
|
| 3 |
O |
-0.213 |
|
|
|
| 4 |
H |
0.184 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
1.730 |
0.241 |
0.000 |
1.747 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-14.753 |
0.549 |
0.000 |
| y |
0.549 |
-18.944 |
0.000 |
| z |
0.000 |
0.000 |
-16.090 |
|
| Traceless |
| | x | y | z |
| x |
2.764 |
0.549 |
0.000 |
| y |
0.549 |
-3.523 |
0.000 |
| z |
0.000 |
0.000 |
0.759 |
|
| Polar |
| 3z2-r2 | 1.517 |
| x2-y2 | 4.191 |
| xy | 0.549 |
| xz | 0.000 |
| yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
4.466 |
-1.739 |
0.000 |
| y |
-1.739 |
3.131 |
0.000 |
| z |
0.000 |
0.000 |
2.082 |
<r2> (average value of r
2) Å
2
| <r2> |
36.002 |
| (<r2>)1/2 |
6.000 |