Jump to
S1C2
Energy calculated at B3LYP/6-311G*
| hartrees |
Energy at 0K | -686.263034 |
Energy at 298.15K | -686.265453 |
HF Energy | -686.263034 |
Nuclear repulsion energy | 188.787983 |
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 B3LYP/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' |
3655 |
3532 |
48.74 |
|
|
|
2 |
A' |
1166 |
1127 |
59.21 |
|
|
|
3 |
A' |
962 |
930 |
62.89 |
|
|
|
4 |
A' |
566 |
547 |
182.51 |
|
|
|
5 |
A' |
486 |
470 |
33.78 |
|
|
|
6 |
A' |
363 |
351 |
5.38 |
|
|
|
7 |
A" |
1094 |
1057 |
227.73 |
|
|
|
8 |
A" |
362 |
350 |
56.85 |
|
|
|
9 |
A" |
111 |
107 |
68.76 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 4382.7 cm
-1
Scaled (by 0.9663) Zero Point Vibrational Energy (zpe) 4235.0 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 B3LYP/6-311G*
Point Group is Cs
Cartesians (Å)
Atom |
x (Å) |
y (Å) |
z (Å) |
Cl1 |
0.361 |
0.137 |
0.000 |
O2 |
-0.206 |
-1.553 |
0.000 |
H3 |
-1.180 |
-1.492 |
0.000 |
O4 |
-0.206 |
0.724 |
1.237 |
O5 |
-0.206 |
0.724 |
-1.237 |
Atom - Atom Distances (Å)
|
Cl1 |
O2 |
H3 |
O4 |
O5 |
Cl1 | | 1.7818 | 2.2418 | 1.4823 | 1.4823 |
O2 | 1.7818 | | 0.9759 | 2.5913 | 2.5913 | H3 | 2.2418 | 0.9759 | | 2.7186 | 2.7186 | O4 | 1.4823 | 2.5913 | 2.7186 | | 2.4742 | O5 | 1.4823 | 2.5913 | 2.7186 | 2.4742 | |
More geometry information
Calculated Bond Angles
atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
Cl1 |
O2 |
H5 |
33.588 |
|
O2 |
Cl1 |
O3 |
24.868 |
O2 |
Cl1 |
O4 |
104.731 |
|
O3 |
Cl1 |
O4 |
91.445 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at B3LYP/6-311G*
Charges (e)
Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
1 |
Cl |
1.024 |
|
|
|
2 |
O |
-0.598 |
|
|
|
3 |
H |
0.411 |
|
|
|
4 |
O |
-0.419 |
|
|
|
5 |
O |
-0.419 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
|
x |
y |
z |
Total |
|
0.113 |
-0.860 |
0.000 |
0.867 |
CHELPG |
|
|
|
|
AIM |
|
|
|
|
ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
Primitive |
| x | y | z |
x |
-24.730 |
3.570 |
0.000 |
y |
3.570 |
-31.581 |
0.000 |
z |
0.000 |
0.000 |
-33.818 |
|
Traceless |
| x | y | z |
x |
7.970 |
3.570 |
0.000 |
y |
3.570 |
-2.307 |
0.000 |
z |
0.000 |
0.000 |
-5.663 |
|
Polar |
3z2-r2 | -11.326 |
x2-y2 | 6.851 |
xy | 3.570 |
xz | 0.000 |
yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
|
x |
y |
z |
x |
2.703 |
0.385 |
0.000 |
y |
0.385 |
4.791 |
0.000 |
z |
0.000 |
0.000 |
4.279 |
<r2> (average value of r
2) Å
2
<r2> |
78.098 |
(<r2>)1/2 |
8.837 |
Jump to
S1C1
Energy calculated at B3LYP/6-311G*
| hartrees |
Energy at 0K | -686.263045 |
Energy at 298.15K | |
HF Energy | -686.263045 |
Nuclear repulsion energy | 188.790323 |
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 B3LYP/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 |
3654 |
3531 |
48.66 |
|
|
|
2 |
A |
1166 |
1127 |
59.16 |
|
|
|
3 |
A |
1095 |
1058 |
227.71 |
|
|
|
4 |
A |
963 |
930 |
62.93 |
|
|
|
5 |
A |
566 |
547 |
182.51 |
|
|
|
6 |
A |
487 |
470 |
33.63 |
|
|
|
7 |
A |
364 |
352 |
5.42 |
|
|
|
8 |
A |
362 |
350 |
56.18 |
|
|
|
9 |
A |
105 |
102 |
69.42 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 4381.0 cm
-1
Scaled (by 0.9663) Zero Point Vibrational Energy (zpe) 4233.4 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 B3LYP/6-311G*
Point Group is C1
Cartesians (Å)
Atom |
x (Å) |
y (Å) |
z (Å) |
Cl1 |
-0.174 |
0.000 |
-0.344 |
O2 |
1.566 |
-0.001 |
0.040 |
H3 |
1.609 |
-0.001 |
1.015 |
O4 |
-0.697 |
1.237 |
0.282 |
O5 |
-0.699 |
-1.237 |
0.282 |
Atom - Atom Distances (Å)
|
Cl1 |
O2 |
H3 |
O4 |
O5 |
Cl1 | | 1.7822 | 2.2419 | 1.4821 | 1.4822 |
O2 | 1.7822 | | 0.9759 | 2.5912 | 2.5915 | H3 | 2.2419 | 0.9759 | | 2.7178 | 2.7183 | O4 | 1.4821 | 2.5912 | 2.7178 | | 2.4739 | O5 | 1.4822 | 2.5915 | 2.7183 | 2.4739 | |
More geometry information
Calculated Bond Angles
atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
Cl1 |
O2 |
H5 |
33.584 |
|
O2 |
Cl1 |
O3 |
24.872 |
O2 |
Cl1 |
O4 |
104.708 |
|
O3 |
Cl1 |
O4 |
91.413 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at B3LYP/6-311G*
Charges (e)
Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
1 |
Cl |
1.024 |
|
|
|
2 |
O |
-0.598 |
|
|
|
3 |
H |
0.411 |
|
|
|
4 |
O |
-0.419 |
|
|
|
5 |
O |
-0.419 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
|
x |
y |
z |
Total |
|
0.838 |
0.000 |
-0.205 |
0.862 |
CHELPG |
|
|
|
|
AIM |
|
|
|
|
ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
Primitive |
| x | y | z |
x |
-30.752 |
-0.001 |
4.213 |
y |
-0.001 |
-33.816 |
-0.002 |
z |
4.213 |
-0.002 |
-25.562 |
|
Traceless |
| x | y | z |
x |
-1.063 |
-0.001 |
4.213 |
y |
-0.001 |
-5.659 |
-0.002 |
z |
4.213 |
-0.002 |
6.722 |
|
Polar |
3z2-r2 | 13.445 |
x2-y2 | 3.064 |
xy | -0.001 |
xz | 4.213 |
yz | -0.002 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
|
x |
y |
z |
x |
4.850 |
0.000 |
0.156 |
y |
0.000 |
4.278 |
0.000 |
z |
0.156 |
0.000 |
2.646 |
<r2> (average value of r
2) Å
2
<r2> |
78.097 |
(<r2>)1/2 |
8.837 |