Jump to
S1C2
Energy calculated at B1B95/6-31G*
| | hartrees |
| Energy at 0K | -151.862157 |
| Energy at 298.15K | |
| HF Energy | -151.862157 |
| Nuclear repulsion energy | 52.438494 |
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 B1B95/6-31G*
| 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 |
3517 |
3339 |
108.96 |
47.54 |
0.23 |
0.38 |
| 2 |
Σ |
2145 |
2037 |
178.60 |
2.48 |
0.45 |
0.62 |
| 3 |
Σ |
1335 |
1267 |
24.70 |
30.86 |
0.25 |
0.40 |
| 4 |
Π |
566 |
538 |
0.30 |
1.86 |
0.75 |
0.86 |
| 4 |
Π |
518 |
492 |
12.77 |
1.39 |
0.75 |
0.86 |
| 5 |
Π |
447 |
424 |
22.94 |
0.00 |
0.75 |
0.86 |
| 5 |
Π |
347i |
330i |
139.92 |
3.75 |
0.75 |
0.86 |
Unscaled Zero Point Vibrational Energy (zpe) 4090.7 cm
-1
Scaled (by 0.9493) Zero Point Vibrational Energy (zpe) 3883.3 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 B1B95/6-31G*
Point Group is C∞v
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
0.000 |
0.000 |
0.018 |
| C2 |
0.000 |
0.000 |
-1.242 |
| O3 |
0.000 |
0.000 |
1.206 |
| H4 |
0.000 |
0.000 |
-2.305 |
Atom - Atom Distances (Å)
| |
C1 |
C2 |
O3 |
H4 |
| C1 | | 1.2592 | 1.1884 | 2.3228 |
C2 | 1.2592 | | 2.4476 | 1.0635 | O3 | 1.1884 | 2.4476 | | 3.5111 | H4 | 2.3228 | 1.0635 | 3.5111 | |
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 B1B95/6-31G*
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
0.307 |
|
|
|
| 2 |
C |
-0.166 |
|
|
|
| 3 |
O |
-0.384 |
|
|
|
| 4 |
H |
0.243 |
|
|
|
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 |
-2.178 |
2.178 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-15.733 |
0.000 |
0.000 |
| y |
0.000 |
-17.337 |
0.000 |
| z |
0.000 |
0.000 |
-14.285 |
|
| Traceless |
| | x | y | z |
| x |
0.077 |
0.000 |
0.000 |
| y |
0.000 |
-2.328 |
0.000 |
| z |
0.000 |
0.000 |
2.250 |
|
| Polar |
| 3z2-r2 | 4.500 |
| x2-y2 | 1.603 |
| 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 |
1.418 |
0.000 |
0.000 |
| y |
0.000 |
1.420 |
0.000 |
| z |
0.000 |
0.000 |
5.363 |
<r2> (average value of r
2) Å
2
| <r2> |
36.059 |
| (<r2>)1/2 |
6.005 |
Jump to
S1C1
Energy calculated at B1B95/6-31G*
| | hartrees |
| Energy at 0K | -151.864105 |
| Energy at 298.15K | |
| HF Energy | -151.864105 |
| Nuclear repulsion energy | 52.326442 |
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 B1B95/6-31G*
| 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' |
3404 |
3232 |
40.17 |
74.53 |
0.31 |
0.47 |
| 2 |
A' |
2130 |
2022 |
264.97 |
3.21 |
0.29 |
0.46 |
| 3 |
A' |
1292 |
1227 |
8.12 |
27.72 |
0.30 |
0.46 |
| 4 |
A' |
550 |
522 |
6.98 |
3.92 |
0.75 |
0.86 |
| 5 |
A' |
481 |
457 |
231.32 |
7.67 |
0.20 |
0.33 |
| 6 |
A" |
498 |
473 |
3.69 |
0.76 |
0.75 |
0.86 |
Unscaled Zero Point Vibrational Energy (zpe) 4178.1 cm
-1
Scaled (by 0.9493) Zero Point Vibrational Energy (zpe) 3966.2 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 B1B95/6-31G*
Point Group is Cs
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
0.000 |
0.049 |
0.000 |
| C2 |
1.104 |
-0.618 |
0.000 |
| O3 |
-1.097 |
0.478 |
0.000 |
| H4 |
2.156 |
-0.410 |
0.000 |
Atom - Atom Distances (Å)
| |
C1 |
C2 |
O3 |
H4 |
| C1 | | 1.2893 | 1.1780 | 2.2041 |
C2 | 1.2893 | | 2.4584 | 1.0724 | O3 | 1.1780 | 2.4584 | | 3.3720 | H4 | 2.2041 | 1.0724 | 3.3720 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| C1 |
C2 |
H4 |
137.711 |
|
C2 |
C1 |
O3 |
170.219 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at B1B95/6-31G*
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
0.405 |
|
|
|
| 2 |
C |
-0.275 |
|
|
|
| 3 |
O |
-0.356 |
|
|
|
| 4 |
H |
0.226 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
1.753 |
0.437 |
0.000 |
1.807 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-14.710 |
1.063 |
0.000 |
| y |
1.063 |
-18.438 |
0.000 |
| z |
0.000 |
0.000 |
-15.835 |
|
| Traceless |
| | x | y | z |
| x |
2.427 |
1.063 |
0.000 |
| y |
1.063 |
-3.165 |
0.000 |
| z |
0.000 |
0.000 |
0.738 |
|
| Polar |
| 3z2-r2 | 1.477 |
| x2-y2 | 3.728 |
| xy | 1.063 |
| xz | 0.000 |
| yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
4.703 |
-1.546 |
0.000 |
| y |
-1.546 |
2.505 |
0.000 |
| z |
0.000 |
0.000 |
1.867 |
<r2> (average value of r
2) Å
2
| <r2> |
36.081 |
| (<r2>)1/2 |
6.007 |