Jump to
S1C2
Energy calculated at BLYP/6-311G*
| hartrees |
Energy at 0K | -686.256426 |
Energy at 298.15K | -686.258594 |
HF Energy | -686.256426 |
Nuclear repulsion energy | 182.337896 |
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 BLYP/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' |
3507 |
3498 |
27.85 |
|
|
|
2 |
A' |
1060 |
1057 |
59.43 |
|
|
|
3 |
A' |
872 |
870 |
47.81 |
|
|
|
4 |
A' |
500 |
499 |
126.13 |
|
|
|
5 |
A' |
436 |
434 |
28.99 |
|
|
|
6 |
A' |
308 |
308 |
5.22 |
|
|
|
7 |
A" |
992 |
990 |
176.45 |
|
|
|
8 |
A" |
298 |
297 |
48.76 |
|
|
|
9 |
A" |
124 |
124 |
59.64 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 4048.9 cm
-1
Scaled (by 0.9975) Zero Point Vibrational Energy (zpe) 4038.8 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 BLYP/6-311G*
Point Group is Cs
Cartesians (Å)
Atom |
x (Å) |
y (Å) |
z (Å) |
Cl1 |
0.361 |
0.152 |
0.000 |
O2 |
-0.206 |
-1.645 |
0.000 |
H3 |
-1.191 |
-1.576 |
0.000 |
O4 |
-0.206 |
0.759 |
1.271 |
O5 |
-0.206 |
0.759 |
-1.271 |
Atom - Atom Distances (Å)
|
Cl1 |
O2 |
H3 |
O4 |
O5 |
Cl1 | | 1.8849 | 2.3225 | 1.5186 | 1.5186 |
O2 | 1.8849 | | 0.9870 | 2.7200 | 2.7200 | H3 | 2.3225 | 0.9870 | | 2.8352 | 2.8352 | O4 | 1.5186 | 2.7200 | 2.8352 | | 2.5423 | O5 | 1.5186 | 2.7200 | 2.8352 | 2.5423 | |
More geometry information
Calculated Bond Angles
atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
Cl1 |
O2 |
H5 |
32.529 |
|
O2 |
Cl1 |
O3 |
24.413 |
O2 |
Cl1 |
O4 |
105.600 |
|
O3 |
Cl1 |
O4 |
92.749 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at BLYP/6-311G*
Charges (e)
Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
1 |
Cl |
0.934 |
|
|
|
2 |
O |
-0.576 |
|
|
|
3 |
H |
0.387 |
|
|
|
4 |
O |
-0.373 |
|
|
|
5 |
O |
-0.373 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
|
x |
y |
z |
Total |
|
0.062 |
-0.484 |
0.000 |
0.488 |
CHELPG |
|
|
|
|
AIM |
|
|
|
|
ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
Primitive |
| x | y | z |
x |
-24.974 |
3.499 |
0.000 |
y |
3.499 |
-31.915 |
0.000 |
z |
0.000 |
0.000 |
-33.508 |
|
Traceless |
| x | y | z |
x |
7.737 |
3.499 |
0.000 |
y |
3.499 |
-2.674 |
0.000 |
z |
0.000 |
0.000 |
-5.063 |
|
Polar |
3z2-r2 | -10.127 |
x2-y2 | 6.941 |
xy | 3.499 |
xz | 0.000 |
yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
|
x |
y |
z |
x |
2.825 |
0.446 |
0.000 |
y |
0.446 |
5.432 |
0.000 |
z |
0.000 |
0.000 |
4.697 |
<r2> (average value of r
2) Å
2
<r2> |
83.087 |
(<r2>)1/2 |
9.115 |
Jump to
S1C1
Energy calculated at BLYP/6-311G*
| hartrees |
Energy at 0K | -686.256418 |
Energy at 298.15K | |
HF Energy | -686.256418 |
Nuclear repulsion energy | 182.377681 |
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 BLYP/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 |
3507 |
3498 |
27.93 |
|
|
|
2 |
A |
1061 |
1058 |
59.24 |
|
|
|
3 |
A |
993 |
991 |
176.62 |
|
|
|
4 |
A |
873 |
871 |
47.76 |
|
|
|
5 |
A |
500 |
499 |
126.55 |
|
|
|
6 |
A |
436 |
434 |
28.87 |
|
|
|
7 |
A |
309 |
308 |
5.25 |
|
|
|
8 |
A |
297 |
296 |
47.40 |
|
|
|
9 |
A |
118 |
118 |
61.15 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 4046.6 cm
-1
Scaled (by 0.9975) Zero Point Vibrational Energy (zpe) 4036.4 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 BLYP/6-311G*
Point Group is C1
Cartesians (Å)
Atom |
x (Å) |
y (Å) |
z (Å) |
Cl1 |
-0.188 |
0.000 |
-0.344 |
O2 |
1.657 |
-0.003 |
0.037 |
H3 |
1.689 |
0.000 |
1.023 |
O4 |
-0.731 |
1.272 |
0.282 |
O5 |
-0.737 |
-1.270 |
0.283 |
Atom - Atom Distances (Å)
|
Cl1 |
O2 |
H3 |
O4 |
O5 |
Cl1 | | 1.8843 | 2.3226 | 1.5183 | 1.5183 |
O2 | 1.8843 | | 0.9870 | 2.7187 | 2.7195 | H3 | 2.3226 | 0.9870 | | 2.8333 | 2.8367 | O4 | 1.5183 | 2.7187 | 2.8333 | | 2.5418 | O5 | 1.5183 | 2.7195 | 2.8367 | 2.5418 | |
More geometry information
Calculated Bond Angles
atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
Cl1 |
O2 |
H5 |
32.528 |
|
O2 |
Cl1 |
O3 |
24.405 |
O2 |
Cl1 |
O4 |
105.568 |
|
O3 |
Cl1 |
O4 |
92.665 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at BLYP/6-311G*
Charges (e)
Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
1 |
Cl |
0.935 |
|
|
|
2 |
O |
-0.576 |
|
|
|
3 |
H |
0.387 |
|
|
|
4 |
O |
-0.373 |
|
|
|
5 |
O |
-0.373 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
|
x |
y |
z |
Total |
|
0.476 |
0.003 |
-0.111 |
0.489 |
CHELPG |
|
|
|
|
AIM |
|
|
|
|
ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
Primitive |
| x | y | z |
x |
-31.125 |
0.005 |
4.133 |
y |
0.005 |
-33.508 |
0.001 |
z |
4.133 |
0.001 |
-25.757 |
|
Traceless |
| x | y | z |
x |
-1.493 |
0.005 |
4.133 |
y |
0.005 |
-5.067 |
0.001 |
z |
4.133 |
0.001 |
6.560 |
|
Polar |
3z2-r2 | 13.119 |
x2-y2 | 2.383 |
xy | 0.005 |
xz | 4.133 |
yz | 0.001 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
|
x |
y |
z |
x |
5.491 |
0.001 |
0.173 |
y |
0.001 |
4.695 |
0.001 |
z |
0.173 |
0.001 |
2.761 |
<r2> (average value of r
2) Å
2
<r2> |
83.053 |
(<r2>)1/2 |
9.113 |