Jump to
S1C2
Energy calculated at PBEPBE/6-31G**
| hartrees |
Energy at 0K | -685.792846 |
Energy at 298.15K | -685.795103 |
HF Energy | -685.792846 |
Nuclear repulsion energy | 186.492543 |
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 PBEPBE/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' |
3592 |
3543 |
51.84 |
|
|
|
2 |
A' |
1104 |
1089 |
58.19 |
|
|
|
3 |
A' |
971 |
958 |
39.47 |
|
|
|
4 |
A' |
558 |
550 |
156.51 |
|
|
|
5 |
A' |
462 |
456 |
24.03 |
|
|
|
6 |
A' |
344 |
339 |
5.01 |
|
|
|
7 |
A" |
1114 |
1098 |
176.87 |
|
|
|
8 |
A" |
328 |
323 |
38.11 |
|
|
|
9 |
A" |
70 |
69 |
57.79 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 4271.4 cm
-1
Scaled (by 0.9863) Zero Point Vibrational Energy (zpe) 4212.8 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 PBEPBE/6-31G**
Point Group is Cs
Cartesians (Å)
Atom |
x (Å) |
y (Å) |
z (Å) |
Cl1 |
0.358 |
0.138 |
0.000 |
O2 |
-0.204 |
-1.573 |
0.000 |
H3 |
-1.186 |
-1.473 |
0.000 |
O4 |
-0.204 |
0.731 |
1.260 |
O5 |
-0.204 |
0.731 |
-1.260 |
Atom - Atom Distances (Å)
|
Cl1 |
O2 |
H3 |
O4 |
O5 |
Cl1 | | 1.8010 | 2.2317 | 1.5015 | 1.5015 |
O2 | 1.8010 | | 0.9869 | 2.6259 | 2.6259 | H3 | 2.2317 | 0.9869 | | 2.7222 | 2.7222 | O4 | 1.5015 | 2.6259 | 2.7222 | | 2.5195 | O5 | 1.5015 | 2.6259 | 2.7222 | 2.5195 | |
More geometry information
Calculated Bond Angles
atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
Cl1 |
O2 |
H5 |
33.530 |
|
O2 |
Cl1 |
O3 |
25.588 |
O2 |
Cl1 |
O4 |
104.972 |
|
O3 |
Cl1 |
O4 |
91.501 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at PBEPBE/6-31G**
Charges (e)
Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
1 |
Cl |
1.107 |
|
|
|
2 |
O |
-0.535 |
|
|
|
3 |
H |
0.330 |
|
|
|
4 |
O |
-0.451 |
|
|
|
5 |
O |
-0.451 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
|
x |
y |
z |
Total |
|
0.006 |
-0.726 |
0.000 |
0.726 |
CHELPG |
|
|
|
|
AIM |
|
|
|
|
ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
Primitive |
| x | y | z |
x |
-24.711 |
3.149 |
0.000 |
y |
3.149 |
-30.537 |
0.000 |
z |
0.000 |
0.000 |
-32.326 |
|
Traceless |
| x | y | z |
x |
6.720 |
3.149 |
0.000 |
y |
3.149 |
-2.018 |
0.000 |
z |
0.000 |
0.000 |
-4.702 |
|
Polar |
3z2-r2 | -9.404 |
x2-y2 | 5.826 |
xy | 3.149 |
xz | 0.000 |
yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
|
x |
y |
z |
x |
2.819 |
0.335 |
0.000 |
y |
0.335 |
4.814 |
0.000 |
z |
0.000 |
0.000 |
4.493 |
<r2> (average value of r
2) Å
2
<r2> |
79.047 |
(<r2>)1/2 |
8.891 |
Jump to
S1C1
Energy calculated at PBEPBE/6-31G**
| hartrees |
Energy at 0K | -685.792862 |
Energy at 298.15K | |
HF Energy | -685.792862 |
Nuclear repulsion energy | 186.506551 |
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 PBEPBE/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 |
3592 |
3543 |
51.83 |
|
|
|
2 |
A |
1114 |
1099 |
176.92 |
|
|
|
3 |
A |
1107 |
1091 |
58.01 |
|
|
|
4 |
A |
972 |
959 |
39.68 |
|
|
|
5 |
A |
558 |
550 |
156.58 |
|
|
|
6 |
A |
462 |
456 |
23.84 |
|
|
|
7 |
A |
345 |
340 |
5.05 |
|
|
|
8 |
A |
327 |
323 |
37.20 |
|
|
|
9 |
A |
56 |
55 |
58.71 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 4265.9 cm
-1
Scaled (by 0.9863) Zero Point Vibrational Energy (zpe) 4207.4 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 PBEPBE/6-31G**
Point Group is C1
Cartesians (Å)
Atom |
x (Å) |
y (Å) |
z (Å) |
Cl1 |
-0.175 |
0.000 |
-0.342 |
O2 |
1.585 |
-0.000 |
0.040 |
H3 |
1.588 |
0.000 |
1.027 |
O4 |
-0.706 |
1.260 |
0.279 |
O5 |
-0.706 |
-1.259 |
0.279 |
Atom - Atom Distances (Å)
|
Cl1 |
O2 |
H3 |
O4 |
O5 |
Cl1 | | 1.8012 | 2.2318 | 1.5012 | 1.5012 |
O2 | 1.8012 | | 0.9869 | 2.6256 | 2.6256 | H3 | 2.2318 | 0.9869 | | 2.7216 | 2.7220 | O4 | 1.5012 | 2.6256 | 2.7216 | | 2.5192 | O5 | 1.5012 | 2.6256 | 2.7220 | 2.5192 | |
More geometry information
Calculated Bond Angles
atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
Cl1 |
O2 |
H5 |
33.530 |
|
O2 |
Cl1 |
O3 |
25.590 |
O2 |
Cl1 |
O4 |
104.957 |
|
O3 |
Cl1 |
O4 |
91.475 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at PBEPBE/6-31G**
Charges (e)
Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
1 |
Cl |
1.107 |
|
|
|
2 |
O |
-0.535 |
|
|
|
3 |
H |
0.330 |
|
|
|
4 |
O |
-0.451 |
|
|
|
5 |
O |
-0.451 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
|
x |
y |
z |
Total |
|
0.718 |
0.000 |
-0.081 |
0.723 |
CHELPG |
|
|
|
|
AIM |
|
|
|
|
ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
Primitive |
| x | y | z |
x |
-29.825 |
0.001 |
3.682 |
y |
0.001 |
-32.325 |
0.001 |
z |
3.682 |
0.001 |
-25.424 |
|
Traceless |
| x | y | z |
x |
-0.951 |
0.001 |
3.682 |
y |
0.001 |
-4.700 |
0.001 |
z |
3.682 |
0.001 |
5.651 |
|
Polar |
3z2-r2 | 11.302 |
x2-y2 | 2.499 |
xy | 0.001 |
xz | 3.682 |
yz | 0.001 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
|
x |
y |
z |
x |
4.861 |
0.000 |
0.122 |
y |
0.000 |
4.492 |
0.000 |
z |
0.122 |
0.000 |
2.771 |
<r2> (average value of r
2) Å
2
<r2> |
79.038 |
(<r2>)1/2 |
8.890 |