Jump to
S1C2
Energy calculated at B2PLYP/6-311G*
| | hartrees |
| Energy at 0K | -151.824694 |
| Energy at 298.15K | |
| HF Energy | -151.680004 |
| Nuclear repulsion energy | 52.496461 |
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 B2PLYP/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 |
3492 |
3492 |
115.30 |
38.70 |
0.28 |
0.44 |
| 2 |
Σ |
2145 |
2145 |
275.53 |
1.18 |
0.09 |
0.17 |
| 3 |
Σ |
1302 |
1302 |
24.54 |
26.11 |
0.23 |
0.37 |
| 4 |
Π |
578 |
578 |
0.01 |
1.33 |
0.75 |
0.86 |
| 4 |
Π |
538 |
538 |
9.66 |
1.81 |
0.75 |
0.86 |
| 5 |
Π |
413 |
413 |
28.99 |
0.48 |
0.75 |
0.86 |
| 5 |
Π |
425i |
425i |
149.08 |
7.79 |
0.75 |
0.86 |
Unscaled Zero Point Vibrational Energy (zpe) 4020.9 cm
-1
Scaled (by 1) Zero Point Vibrational Energy (zpe) 4020.9 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 B2PLYP/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 |
-1.242 |
| O3 |
0.000 |
0.000 |
1.204 |
| H4 |
0.000 |
0.000 |
-2.303 |
Atom - Atom Distances (Å)
| |
C1 |
C2 |
O3 |
H4 |
| C1 | | 1.2622 | 1.1839 | 2.3236 |
C2 | 1.2622 | | 2.4461 | 1.0615 | O3 | 1.1839 | 2.4461 | | 3.5076 | H4 | 2.3236 | 1.0615 | 3.5076 | |
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 B2PLYP/6-311G*
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
0.190 |
|
|
|
| 2 |
C |
-0.250 |
|
|
|
| 3 |
O |
-0.221 |
|
|
|
| 4 |
H |
0.282 |
|
|
|
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 |
-2.096 |
2.096 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-17.914 |
0.000 |
0.000 |
| y |
0.000 |
-16.174 |
0.000 |
| z |
0.000 |
0.000 |
-14.750 |
|
| Traceless |
| | x | y | z |
| x |
-2.452 |
0.000 |
0.000 |
| y |
0.000 |
0.158 |
0.000 |
| z |
0.000 |
0.000 |
2.295 |
|
| Polar |
| 3z2-r2 | 4.589 |
| x2-y2 | -1.740 |
| 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 |
1.694 |
0.000 |
0.000 |
| y |
0.000 |
1.591 |
0.000 |
| z |
0.000 |
0.000 |
5.466 |
<r2> (average value of r
2) Å
2
| <r2> |
36.326 |
| (<r2>)1/2 |
6.027 |
Jump to
S1C1
Energy calculated at B2PLYP/6-311G*
| | hartrees |
| Energy at 0K | -151.827802 |
| Energy at 298.15K | |
| HF Energy | -151.680930 |
| Nuclear repulsion energy | 52.296943 |
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 B2PLYP/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' |
3356 |
3356 |
31.46 |
76.26 |
0.36 |
0.53 |
| 2 |
A' |
2117 |
2117 |
342.37 |
0.38 |
0.21 |
0.35 |
| 3 |
A' |
1241 |
1241 |
6.73 |
27.38 |
0.30 |
0.46 |
| 4 |
A' |
571 |
571 |
65.65 |
8.04 |
0.44 |
0.61 |
| 5 |
A' |
535 |
535 |
193.07 |
5.68 |
0.04 |
0.07 |
| 6 |
A" |
510 |
510 |
3.42 |
0.55 |
0.75 |
0.86 |
Unscaled Zero Point Vibrational Energy (zpe) 4164.1 cm
-1
Scaled (by 1) Zero Point Vibrational Energy (zpe) 4164.1 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 B2PLYP/6-311G*
Point Group is Cs
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
0.000 |
0.050 |
0.000 |
| C2 |
1.073 |
-0.682 |
0.000 |
| O3 |
-1.070 |
0.533 |
0.000 |
| H4 |
2.124 |
-0.471 |
0.000 |
Atom - Atom Distances (Å)
| |
C1 |
C2 |
O3 |
H4 |
| C1 | | 1.2989 | 1.1736 | 2.1875 |
C2 | 1.2989 | | 2.4630 | 1.0730 | O3 | 1.1736 | 2.4630 | | 3.3484 | H4 | 2.1875 | 1.0730 | 3.3484 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| C1 |
C2 |
H4 |
134.301 |
|
C2 |
C1 |
O3 |
169.924 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at B2PLYP/6-311G*
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
0.241 |
|
|
|
| 2 |
C |
-0.315 |
|
|
|
| 3 |
O |
-0.197 |
|
|
|
| 4 |
H |
0.270 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
1.596 |
0.542 |
0.000 |
1.686 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-15.144 |
1.116 |
-0.004 |
| y |
1.116 |
-19.278 |
0.009 |
| z |
-0.004 |
0.009 |
-16.305 |
|
| Traceless |
| | x | y | z |
| x |
2.648 |
1.116 |
-0.004 |
| y |
1.116 |
-3.554 |
0.009 |
| z |
-0.004 |
0.009 |
0.906 |
|
| Polar |
| 3z2-r2 | 1.812 |
| x2-y2 | 4.134 |
| xy | 1.116 |
| xz | -0.004 |
| yz | 0.009 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
4.697 |
-1.662 |
0.001 |
| y |
-1.662 |
3.015 |
0.000 |
| z |
0.001 |
0.000 |
2.015 |
<r2> (average value of r
2) Å
2
| <r2> |
36.435 |
| (<r2>)1/2 |
6.036 |