Jump to
S1C2
Energy calculated at M06-2X/6-311G**
| hartrees |
Energy at 0K | -686.137553 |
Energy at 298.15K | -686.140306 |
HF Energy | -686.137553 |
Nuclear repulsion energy | 193.864546 |
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 M06-2X/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' |
3748 |
3748 |
108.61 |
|
|
|
2 |
A' |
1201 |
1201 |
57.11 |
|
|
|
3 |
A' |
1023 |
1023 |
71.54 |
|
|
|
4 |
A' |
658 |
658 |
224.87 |
|
|
|
5 |
A' |
528 |
528 |
36.01 |
|
|
|
6 |
A' |
422 |
422 |
12.49 |
|
|
|
7 |
A" |
1161 |
1161 |
266.44 |
|
|
|
8 |
A" |
441 |
441 |
69.57 |
|
|
|
9 |
A" |
160 |
160 |
55.37 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 4671.4 cm
-1
Scaled (by 1) Zero Point Vibrational Energy (zpe) 4671.4 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 M06-2X/6-311G**
Point Group is Cs
Cartesians (Å)
Atom |
x (Å) |
y (Å) |
z (Å) |
Cl1 |
0.363 |
0.121 |
0.000 |
O2 |
-0.208 |
-1.476 |
0.000 |
H3 |
-1.177 |
-1.379 |
0.000 |
O4 |
-0.208 |
0.695 |
1.217 |
O5 |
-0.208 |
0.695 |
-1.217 |
Atom - Atom Distances (Å)
|
Cl1 |
O2 |
H3 |
O4 |
O5 |
Cl1 | | 1.6960 | 2.1498 | 1.4614 | 1.4614 |
O2 | 1.6960 | | 0.9733 | 2.4884 | 2.4884 | H3 | 2.1498 | 0.9733 | | 2.5922 | 2.5922 | O4 | 1.4614 | 2.4884 | 2.5922 | | 2.4332 | O5 | 1.4614 | 2.4884 | 2.5922 | 2.4332 | |
More geometry information
Calculated Bond Angles
atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
Cl1 |
O2 |
H5 |
34.780 |
|
O2 |
Cl1 |
O3 |
26.061 |
O2 |
Cl1 |
O4 |
103.768 |
|
O3 |
Cl1 |
O4 |
89.654 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at M06-2X/6-311G**
Charges (e)
Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
1 |
Cl |
1.075 |
|
|
|
2 |
O |
-0.456 |
|
|
|
3 |
H |
0.300 |
|
|
|
4 |
O |
-0.459 |
|
|
|
5 |
O |
-0.459 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
|
x |
y |
z |
Total |
|
0.307 |
-1.267 |
0.000 |
1.304 |
CHELPG |
|
|
|
|
AIM |
|
|
|
|
ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
Primitive |
| x | y | z |
x |
-24.682 |
3.361 |
0.000 |
y |
3.361 |
-31.286 |
0.000 |
z |
0.000 |
0.000 |
-34.181 |
|
Traceless |
| x | y | z |
x |
8.051 |
3.361 |
0.000 |
y |
3.361 |
-1.854 |
0.000 |
z |
0.000 |
0.000 |
-6.197 |
|
Polar |
3z2-r2 | -12.394 |
x2-y2 | 6.604 |
xy | 3.361 |
xz | 0.000 |
yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
|
x |
y |
z |
x |
2.668 |
0.299 |
0.000 |
y |
0.299 |
4.254 |
0.000 |
z |
0.000 |
0.000 |
4.036 |
<r2> (average value of r
2) Å
2
<r2> |
74.417 |
(<r2>)1/2 |
8.627 |
Jump to
S1C1
Energy calculated at M06-2X/6-311G**
| hartrees |
Energy at 0K | -686.137625 |
Energy at 298.15K | |
HF Energy | -686.137625 |
Nuclear repulsion energy | 193.817266 |
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 M06-2X/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 |
3751 |
3751 |
108.12 |
|
|
|
2 |
A |
1197 |
1197 |
59.38 |
|
|
|
3 |
A |
1166 |
1166 |
265.57 |
|
|
|
4 |
A |
1023 |
1023 |
69.91 |
|
|
|
5 |
A |
659 |
659 |
221.31 |
|
|
|
6 |
A |
527 |
527 |
36.23 |
|
|
|
7 |
A |
435 |
435 |
67.28 |
|
|
|
8 |
A |
420 |
420 |
14.50 |
|
|
|
9 |
A |
140 |
140 |
57.30 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 4658.4 cm
-1
Scaled (by 1) Zero Point Vibrational Energy (zpe) 4658.4 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 M06-2X/6-311G**
Point Group is C1
Cartesians (Å)
Atom |
x (Å) |
y (Å) |
z (Å) |
Cl1 |
-0.160 |
-0.000 |
-0.348 |
O2 |
1.491 |
0.000 |
0.046 |
H3 |
1.501 |
0.000 |
1.019 |
O4 |
-0.669 |
1.216 |
0.283 |
O5 |
-0.669 |
-1.216 |
0.283 |
Atom - Atom Distances (Å)
|
Cl1 |
O2 |
H3 |
O4 |
O5 |
Cl1 | | 1.6973 | 2.1514 | 1.4613 | 1.4613 |
O2 | 1.6973 | | 0.9734 | 2.4902 | 2.4902 | H3 | 2.1514 | 0.9734 | | 2.5946 | 2.5946 | O4 | 1.4613 | 2.4902 | 2.5946 | | 2.4323 | O5 | 1.4613 | 2.4902 | 2.5946 | 2.4323 | |
More geometry information
Calculated Bond Angles
atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
Cl1 |
O2 |
H5 |
34.740 |
|
O2 |
Cl1 |
O3 |
26.039 |
O2 |
Cl1 |
O4 |
103.816 |
|
O3 |
Cl1 |
O4 |
89.709 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at M06-2X/6-311G**
Charges (e)
Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
1 |
Cl |
1.075 |
|
|
|
2 |
O |
-0.457 |
|
|
|
3 |
H |
0.300 |
|
|
|
4 |
O |
-0.459 |
|
|
|
5 |
O |
-0.459 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
|
x |
y |
z |
Total |
|
1.226 |
0.000 |
-0.442 |
1.303 |
CHELPG |
|
|
|
|
AIM |
|
|
|
|
ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
Primitive |
| x | y | z |
x |
-30.484 |
0.000 |
4.003 |
y |
0.000 |
-34.174 |
0.000 |
z |
4.003 |
0.000 |
-25.488 |
|
Traceless |
| x | y | z |
x |
-0.653 |
0.000 |
4.003 |
y |
0.000 |
-6.188 |
0.000 |
z |
4.003 |
0.000 |
6.841 |
|
Polar |
3z2-r2 | 13.682 |
x2-y2 | 3.690 |
xy | 0.000 |
xz | 4.003 |
yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
|
x |
y |
z |
x |
4.304 |
0.000 |
0.123 |
y |
0.000 |
4.026 |
0.000 |
z |
0.123 |
0.000 |
2.613 |
<r2> (average value of r
2) Å
2
<r2> |
74.458 |
(<r2>)1/2 |
8.629 |