Jump to
S1C2
Energy calculated at LSDA/6-311G**
| hartrees |
Energy at 0K | -684.070525 |
Energy at 298.15K | |
HF Energy | -684.070525 |
Nuclear repulsion energy | 189.915725 |
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 LSDA/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' |
3602 |
3558 |
78.66 |
|
|
|
2 |
A' |
1070 |
1056 |
76.10 |
|
|
|
3 |
A' |
983 |
970 |
33.74 |
|
|
|
4 |
A' |
580 |
573 |
194.17 |
|
|
|
5 |
A' |
481 |
475 |
28.67 |
|
|
|
6 |
A' |
356 |
351 |
9.20 |
|
|
|
7 |
A" |
1127 |
1113 |
224.71 |
|
|
|
8 |
A" |
355 |
351 |
45.82 |
|
|
|
9 |
A" |
14i |
14i |
61.51 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 4269.5 cm
-1
Scaled (by 0.9877) Zero Point Vibrational Energy (zpe) 4217.0 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 LSDA/6-311G**
Point Group is Cs
Cartesians (Å)
Atom |
x (Å) |
y (Å) |
z (Å) |
Cl1 |
0.361 |
0.132 |
0.000 |
O2 |
-0.206 |
-1.537 |
0.000 |
H3 |
-1.185 |
-1.430 |
0.000 |
O4 |
-0.206 |
0.717 |
1.232 |
O5 |
-0.206 |
0.717 |
-1.232 |
Atom - Atom Distances (Å)
|
Cl1 |
O2 |
H3 |
O4 |
O5 |
Cl1 | | 1.7635 | 2.1981 | 1.4774 | 1.4774 |
O2 | 1.7635 | | 0.9843 | 2.5693 | 2.5693 | H3 | 2.1981 | 0.9843 | | 2.6622 | 2.6622 | O4 | 1.4774 | 2.5693 | 2.6622 | | 2.4644 | O5 | 1.4774 | 2.5693 | 2.6622 | 2.4644 | |
More geometry information
Calculated Bond Angles
atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
Cl1 |
O2 |
H5 |
33.819 |
|
O2 |
Cl1 |
O3 |
25.922 |
O2 |
Cl1 |
O4 |
104.547 |
|
O3 |
Cl1 |
O4 |
90.641 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at LSDA/6-311G**
Charges (e)
Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
1 |
Cl |
0.923 |
|
|
|
2 |
O |
-0.445 |
|
|
|
3 |
H |
0.285 |
|
|
|
4 |
O |
-0.382 |
|
|
|
5 |
O |
-0.382 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
|
x |
y |
z |
Total |
|
0.058 |
-0.774 |
0.000 |
0.776 |
CHELPG |
|
|
|
|
AIM |
|
|
|
|
ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
Primitive |
| x | y | z |
x |
-24.917 |
3.266 |
0.000 |
y |
3.266 |
-31.498 |
0.000 |
z |
0.000 |
0.000 |
-33.566 |
|
Traceless |
| x | y | z |
x |
7.616 |
3.266 |
0.000 |
y |
3.266 |
-2.257 |
0.000 |
z |
0.000 |
0.000 |
-5.359 |
|
Polar |
3z2-r2 | -10.717 |
x2-y2 | 6.582 |
xy | 3.266 |
xz | 0.000 |
yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
|
x |
y |
z |
x |
2.827 |
0.352 |
0.000 |
y |
0.352 |
4.659 |
0.000 |
z |
0.000 |
0.000 |
4.379 |
<r2> (average value of r
2) Å
2
<r2> |
77.153 |
(<r2>)1/2 |
8.784 |
Jump to
S1C1
Energy calculated at LSDA/6-311G**
| hartrees |
Energy at 0K | -684.070541 |
Energy at 298.15K | -684.072794 |
HF Energy | -684.070541 |
Nuclear repulsion energy | 189.931910 |
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 LSDA/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 |
3602 |
3558 |
78.72 |
|
|
|
2 |
A |
1129 |
1115 |
223.69 |
|
|
|
3 |
A |
1071 |
1057 |
77.08 |
|
|
|
4 |
A |
984 |
972 |
34.01 |
|
|
|
5 |
A |
581 |
574 |
193.95 |
|
|
|
6 |
A |
481 |
475 |
28.80 |
|
|
|
7 |
A |
361 |
357 |
25.87 |
|
|
|
8 |
A |
350 |
346 |
28.36 |
|
|
|
9 |
A |
24 |
23 |
62.12 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 4290.7 cm
-1
Scaled (by 0.9877) Zero Point Vibrational Energy (zpe) 4237.9 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 LSDA/6-311G**
Point Group is C1
Cartesians (Å)
Atom |
x (Å) |
y (Å) |
z (Å) |
Cl1 |
0.170 |
0.003 |
-0.345 |
O2 |
-1.548 |
-0.091 |
0.043 |
O3 |
0.610 |
1.271 |
0.273 |
O4 |
0.769 |
-1.188 |
0.289 |
H5 |
-1.549 |
0.017 |
1.021 |
Atom - Atom Distances (Å)
|
Cl1 |
O2 |
O3 |
O4 |
H5 |
Cl1 | | 1.7640 | 1.4781 | 1.4762 | 2.1966 |
O2 | 1.7640 | | 2.5622 | 2.5755 | 0.9844 | O3 | 1.4781 | 2.5622 | | 2.4647 | 2.6070 | O4 | 1.4762 | 2.5755 | 2.4647 | | 2.7138 | H5 | 2.1966 | 0.9844 | 2.6070 | 2.7138 | |
More geometry information
Calculated Bond Angles
atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
Cl1 |
O2 |
H5 |
102.382 |
|
O2 |
Cl1 |
O3 |
104.083 |
O2 |
Cl1 |
O4 |
104.938 |
|
O3 |
Cl1 |
O4 |
113.083 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at LSDA/6-311G**
Charges (e)
Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
1 |
Cl |
0.924 |
|
|
|
2 |
O |
-0.445 |
|
|
|
3 |
O |
-0.386 |
|
|
|
4 |
O |
-0.377 |
|
|
|
5 |
H |
0.285 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
|
x |
y |
z |
Total |
|
-0.761 |
0.085 |
-0.150 |
0.781 |
CHELPG |
|
|
|
|
AIM |
|
|
|
|
ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
Primitive |
| x | y | z |
x |
-30.716 |
-0.143 |
-3.873 |
y |
-0.143 |
-33.563 |
0.068 |
z |
-3.873 |
0.068 |
-25.707 |
|
Traceless |
| x | y | z |
x |
-1.081 |
-0.143 |
-3.873 |
y |
-0.143 |
-5.352 |
0.068 |
z |
-3.873 |
0.068 |
6.433 |
|
Polar |
3z2-r2 | 12.866 |
x2-y2 | 2.847 |
xy | -0.143 |
xz | -3.873 |
yz | 0.068 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
|
x |
y |
z |
x |
4.715 |
-0.024 |
-0.152 |
y |
-0.024 |
4.379 |
0.025 |
z |
-0.152 |
0.025 |
2.768 |
<r2> (average value of r
2) Å
2
<r2> |
77.143 |
(<r2>)1/2 |
8.783 |