Jump to
S1C2
Energy calculated at B3PW91/6-311+G(3df,2p)
| hartrees |
Energy at 0K | -686.223004 |
Energy at 298.15K | |
HF Energy | -686.223004 |
Nuclear repulsion energy | 195.917811 |
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 B3PW91/6-311+G(3df,2p)
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' |
3722 |
3563 |
91.00 |
|
|
|
2 |
A' |
1192 |
1141 |
78.16 |
|
|
|
3 |
A' |
1072 |
1026 |
42.56 |
|
|
|
4 |
A' |
630 |
604 |
207.67 |
|
|
|
5 |
A' |
542 |
519 |
32.31 |
|
|
|
6 |
A' |
426 |
408 |
3.17 |
|
|
|
7 |
A" |
1230 |
1177 |
255.29 |
|
|
|
8 |
A" |
405 |
388 |
25.17 |
|
|
|
9 |
A" |
99i |
95i |
68.24 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 4560.3 cm
-1
Scaled (by 0.9573) Zero Point Vibrational Energy (zpe) 4365.5 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 B3PW91/6-311+G(3df,2p)
Point Group is Cs
Cartesians (Å)
Atom |
x (Å) |
y (Å) |
z (Å) |
Cl1 |
0.352 |
0.122 |
0.000 |
O2 |
-0.201 |
-1.474 |
0.000 |
H3 |
-1.170 |
-1.402 |
0.000 |
O4 |
-0.201 |
0.695 |
1.198 |
O5 |
-0.201 |
0.695 |
-1.198 |
Atom - Atom Distances (Å)
|
Cl1 |
O2 |
H3 |
O4 |
O5 |
Cl1 | | 1.6896 | 2.1547 | 1.4383 | 1.4383 |
O2 | 1.6896 | | 0.9724 | 2.4780 | 2.4780 | H3 | 2.1547 | 0.9724 | | 2.6028 | 2.6028 | O4 | 1.4383 | 2.4780 | 2.6028 | | 2.3962 | O5 | 1.4383 | 2.4780 | 2.6028 | 2.3962 | |
More geometry information
Calculated Bond Angles
atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
Cl1 |
O2 |
H5 |
34.189 |
|
O2 |
Cl1 |
O3 |
25.861 |
O2 |
Cl1 |
O4 |
104.504 |
|
O3 |
Cl1 |
O4 |
90.583 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at B3PW91/6-311+G(3df,2p)
Charges (e)
Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
1 |
Cl |
0.973 |
|
|
|
2 |
O |
-0.448 |
|
|
|
3 |
H |
0.279 |
|
|
|
4 |
O |
-0.402 |
|
|
|
5 |
O |
-0.402 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
|
x |
y |
z |
Total |
|
-0.062 |
-1.108 |
0.000 |
1.110 |
CHELPG |
|
|
|
|
AIM |
|
|
|
|
ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
Primitive |
| x | y | z |
x |
-25.158 |
3.199 |
0.000 |
y |
3.199 |
-30.154 |
0.000 |
z |
0.000 |
0.000 |
-32.647 |
|
Traceless |
| x | y | z |
x |
6.243 |
3.199 |
0.000 |
y |
3.199 |
-1.252 |
0.000 |
z |
0.000 |
0.000 |
-4.991 |
|
Polar |
3z2-r2 | -9.982 |
x2-y2 | 4.997 |
xy | 3.199 |
xz | 0.000 |
yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
|
x |
y |
z |
x |
3.728 |
0.220 |
0.000 |
y |
0.220 |
5.314 |
0.000 |
z |
0.000 |
0.000 |
5.104 |
<r2> (average value of r
2) Å
2
<r2> |
73.058 |
(<r2>)1/2 |
8.547 |
Jump to
S1C1
Energy calculated at B3PW91/6-311+G(3df,2p)
| hartrees |
Energy at 0K | -686.223321 |
Energy at 298.15K | |
HF Energy | -686.223321 |
Nuclear repulsion energy | 195.853139 |
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 B3PW91/6-311+G(3df,2p)
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 |
3771 |
3610 |
110.11 |
|
|
|
2 |
A |
1269 |
1215 |
222.19 |
|
|
|
3 |
A |
1155 |
1106 |
115.39 |
|
|
|
4 |
A |
1086 |
1040 |
50.40 |
|
|
|
5 |
A |
645 |
618 |
158.84 |
|
|
|
6 |
A |
550 |
526 |
42.36 |
|
|
|
7 |
A |
424 |
406 |
1.49 |
|
|
|
8 |
A |
386 |
370 |
14.64 |
|
|
|
9 |
A |
61 |
59 |
96.20 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 4674.3 cm
-1
Scaled (by 0.9573) Zero Point Vibrational Energy (zpe) 4474.7 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 B3PW91/6-311+G(3df,2p)
Point Group is C1
Cartesians (Å)
Atom |
x (Å) |
y (Å) |
z (Å) |
Cl1 |
-0.175 |
0.029 |
-0.333 |
O2 |
1.391 |
-0.480 |
0.114 |
H3 |
1.858 |
0.343 |
0.325 |
O4 |
-0.264 |
1.341 |
0.258 |
O5 |
-0.986 |
-0.966 |
0.294 |
Atom - Atom Distances (Å)
|
Cl1 |
O2 |
H3 |
O4 |
O5 |
Cl1 | | 1.7066 | 2.1597 | 1.4410 | 1.4287 |
O2 | 1.7066 | | 0.9692 | 2.4642 | 2.4328 | H3 | 2.1597 | 0.9692 | | 2.3452 | 3.1307 | O4 | 1.4410 | 2.4642 | 2.3452 | | 2.4171 | O5 | 1.4287 | 2.4328 | 3.1307 | 2.4171 | |
More geometry information
Calculated Bond Angles
atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
Cl1 |
O2 |
H5 |
35.145 |
|
O2 |
Cl1 |
O3 |
25.786 |
O2 |
Cl1 |
O4 |
102.723 |
|
O3 |
Cl1 |
O4 |
78.500 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at B3PW91/6-311+G(3df,2p)
Charges (e)
Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
1 |
Cl |
0.960 |
|
|
|
2 |
O |
-0.457 |
|
|
|
3 |
H |
0.288 |
|
|
|
4 |
O |
-0.419 |
|
|
|
5 |
O |
-0.372 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
|
x |
y |
z |
Total |
|
1.522 |
0.883 |
-1.215 |
2.138 |
CHELPG |
|
|
|
|
AIM |
|
|
|
|
ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
Primitive |
| x | y | z |
x |
-26.866 |
1.874 |
1.688 |
y |
1.874 |
-32.089 |
0.245 |
z |
1.688 |
0.245 |
-28.374 |
|
Traceless |
| x | y | z |
x |
3.365 |
1.874 |
1.688 |
y |
1.874 |
-4.468 |
0.245 |
z |
1.688 |
0.245 |
1.103 |
|
Polar |
3z2-r2 | 2.206 |
x2-y2 | 5.223 |
xy | 1.874 |
xz | 1.688 |
yz | 0.245 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
|
x |
y |
z |
x |
5.493 |
0.090 |
-0.001 |
y |
0.090 |
5.177 |
0.015 |
z |
-0.001 |
0.015 |
3.546 |
<r2> (average value of r
2) Å
2
<r2> |
73.102 |
(<r2>)1/2 |
8.550 |