Jump to
S1C2
Energy calculated at HSEh1PBE/6-311+G(3df,2p)
| hartrees |
Energy at 0K | -686.004115 |
Energy at 298.15K | |
HF Energy | -686.004115 |
Nuclear repulsion energy | 196.968234 |
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 HSEh1PBE/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' |
3736 |
3736 |
95.39 |
|
|
|
2 |
A' |
1209 |
1209 |
82.22 |
|
|
|
3 |
A' |
1090 |
1090 |
42.21 |
|
|
|
4 |
A' |
651 |
651 |
217.20 |
|
|
|
5 |
A' |
553 |
553 |
27.56 |
|
|
|
6 |
A' |
439 |
439 |
4.82 |
|
|
|
7 |
A" |
1249 |
1249 |
264.11 |
|
|
|
8 |
A" |
419 |
419 |
27.10 |
|
|
|
9 |
A" |
95i |
95i |
68.29 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 4624.5 cm
-1
Scaled (by 1) Zero Point Vibrational Energy (zpe) 4624.5 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 HSEh1PBE/6-311+G(3df,2p)
Point Group is Cs
Cartesians (Å)
Atom |
x (Å) |
y (Å) |
z (Å) |
Cl1 |
0.352 |
0.119 |
0.000 |
O2 |
-0.200 |
-1.460 |
0.000 |
H3 |
-1.169 |
-1.388 |
0.000 |
O4 |
-0.200 |
0.690 |
1.194 |
O5 |
-0.200 |
0.690 |
-1.194 |
Atom - Atom Distances (Å)
|
Cl1 |
O2 |
H3 |
O4 |
O5 |
Cl1 | | 1.6728 | 2.1414 | 1.4339 | 1.4339 |
O2 | 1.6728 | | 0.9715 | 2.4593 | 2.4593 | H3 | 2.1414 | 0.9715 | | 2.5852 | 2.5852 | O4 | 1.4339 | 2.4593 | 2.5852 | | 2.3872 | O5 | 1.4339 | 2.4593 | 2.5852 | 2.3872 | |
More geometry information
Calculated Bond Angles
atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
Cl1 |
O2 |
H5 |
34.381 |
|
O2 |
Cl1 |
O3 |
25.985 |
O2 |
Cl1 |
O4 |
104.410 |
|
O3 |
Cl1 |
O4 |
90.389 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at HSEh1PBE/6-311+G(3df,2p)
Charges (e)
Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
1 |
Cl |
0.979 |
|
|
|
2 |
O |
-0.437 |
|
|
|
3 |
H |
0.280 |
|
|
|
4 |
O |
-0.411 |
|
|
|
5 |
O |
-0.411 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
|
x |
y |
z |
Total |
|
-0.071 |
-1.183 |
0.000 |
1.185 |
CHELPG |
|
|
|
|
AIM |
|
|
|
|
ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
Primitive |
| x | y | z |
x |
-25.230 |
3.203 |
0.000 |
y |
3.203 |
-30.128 |
0.000 |
z |
0.000 |
0.000 |
-32.729 |
|
Traceless |
| x | y | z |
x |
6.199 |
3.203 |
0.000 |
y |
3.203 |
-1.148 |
0.000 |
z |
0.000 |
0.000 |
-5.050 |
|
Polar |
3z2-r2 | -10.101 |
x2-y2 | 4.898 |
xy | 3.203 |
xz | 0.000 |
yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
|
x |
y |
z |
x |
3.727 |
0.210 |
0.000 |
y |
0.210 |
5.216 |
0.000 |
z |
0.000 |
0.000 |
5.047 |
<r2> (average value of r
2) Å
2
<r2> |
72.413 |
(<r2>)1/2 |
8.510 |
Jump to
S1C1
Energy calculated at HSEh1PBE/6-311+G(3df,2p)
| hartrees |
Energy at 0K | -686.004357 |
Energy at 298.15K | |
HF Energy | -686.004357 |
Nuclear repulsion energy | 196.922609 |
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 HSEh1PBE/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 |
3766 |
3766 |
114.25 |
|
|
|
2 |
A |
1276 |
1276 |
227.39 |
|
|
|
3 |
A |
1191 |
1191 |
113.34 |
|
|
|
4 |
A |
1087 |
1087 |
47.50 |
|
|
|
5 |
A |
663 |
663 |
197.94 |
|
|
|
6 |
A |
561 |
561 |
34.45 |
|
|
|
7 |
A |
438 |
438 |
2.17 |
|
|
|
8 |
A |
382 |
382 |
6.15 |
|
|
|
9 |
A |
77 |
77 |
95.92 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 4720.3 cm
-1
Scaled (by 1) Zero Point Vibrational Energy (zpe) 4720.3 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 HSEh1PBE/6-311+G(3df,2p)
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