Jump to
S1C2
Energy calculated at HSEh1PBE/6-31G*
| hartrees |
Energy at 0K | -685.823496 |
Energy at 298.15K | -685.825960 |
HF Energy | -685.823496 |
Nuclear repulsion energy | 192.003989 |
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/6-31G*
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' |
3675 |
3495 |
80.37 |
|
|
|
2 |
A' |
1224 |
1164 |
63.51 |
|
|
|
3 |
A' |
1052 |
1001 |
55.44 |
|
|
|
4 |
A' |
644 |
613 |
199.69 |
|
|
|
5 |
A' |
515 |
489 |
26.79 |
|
|
|
6 |
A' |
401 |
381 |
9.96 |
|
|
|
7 |
A" |
1202 |
1143 |
224.47 |
|
|
|
8 |
A" |
394 |
375 |
50.11 |
|
|
|
9 |
A" |
48 |
46 |
67.93 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 4577.5 cm
-1
Scaled (by 0.951) Zero Point Vibrational Energy (zpe) 4353.2 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/6-31G*
Point Group is Cs
Cartesians (Å)
Atom |
x (Å) |
y (Å) |
z (Å) |
Cl1 |
0.357 |
0.125 |
0.000 |
O2 |
-0.204 |
-1.499 |
0.000 |
H3 |
-1.180 |
-1.414 |
0.000 |
O4 |
-0.204 |
0.705 |
1.230 |
O5 |
-0.204 |
0.705 |
-1.230 |
Atom - Atom Distances (Å)
|
Cl1 |
O2 |
H3 |
O4 |
O5 |
Cl1 | | 1.7187 | 2.1752 | 1.4708 | 1.4708 |
O2 | 1.7187 | | 0.9795 | 2.5241 | 2.5241 | H3 | 2.1752 | 0.9795 | | 2.6374 | 2.6374 | O4 | 1.4708 | 2.5241 | 2.6374 | | 2.4604 | O5 | 1.4708 | 2.5241 | 2.6374 | 2.4604 | |
More geometry information
Calculated Bond Angles
atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
Cl1 |
O2 |
H5 |
34.368 |
|
O2 |
Cl1 |
O3 |
25.902 |
O2 |
Cl1 |
O4 |
104.358 |
|
O3 |
Cl1 |
O4 |
90.547 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at HSEh1PBE/6-31G*
Charges (e)
Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
1 |
Cl |
1.236 |
|
|
|
2 |
O |
-0.651 |
|
|
|
3 |
H |
0.438 |
|
|
|
4 |
O |
-0.511 |
|
|
|
5 |
O |
-0.511 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
|
x |
y |
z |
Total |
|
0.039 |
-1.093 |
0.000 |
1.094 |
CHELPG |
|
|
|
|
AIM |
|
|
|
|
ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
Primitive |
| x | y | z |
x |
-24.487 |
3.338 |
0.000 |
y |
3.338 |
-30.389 |
0.000 |
z |
0.000 |
0.000 |
-32.817 |
|
Traceless |
| x | y | z |
x |
7.116 |
3.338 |
0.000 |
y |
3.338 |
-1.737 |
0.000 |
z |
0.000 |
0.000 |
-5.379 |
|
Polar |
3z2-r2 | -10.758 |
x2-y2 | 5.902 |
xy | 3.338 |
xz | 0.000 |
yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
|
x |
y |
z |
x |
2.685 |
0.273 |
0.000 |
y |
0.273 |
4.326 |
0.000 |
z |
0.000 |
0.000 |
4.136 |
<r2> (average value of r
2) Å
2
<r2> |
75.221 |
(<r2>)1/2 |
8.673 |
Jump to
S1C1
Energy calculated at HSEh1PBE/6-31G*
| hartrees |
Energy at 0K | -685.823507 |
Energy at 298.15K | |
HF Energy | -685.823507 |
Nuclear repulsion energy | 192.016204 |
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/6-31G*
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 |
3673 |
3493 |
80.23 |
|
|
|
2 |
A |
1225 |
1165 |
63.61 |
|
|
|
3 |
A |
1203 |
1144 |
224.30 |
|
|
|
4 |
A |
1054 |
1002 |
55.31 |
|
|
|
5 |
A |
644 |
612 |
200.01 |
|
|
|
6 |
A |
514 |
489 |
26.82 |
|
|
|
7 |
A |
401 |
381 |
9.69 |
|
|
|
8 |
A |
394 |
375 |
49.21 |
|
|
|
9 |
A |
18i |
18i |
68.92 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 4544.2 cm
-1
Scaled (by 0.951) Zero Point Vibrational Energy (zpe) 4321.5 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/6-31G*
Point Group is C1
Cartesians (Å)
Atom |
x (Å) |
y (Å) |
z (Å) |
Cl1 |
0.163 |
-0.000 |
0.341 |
O2 |
-1.513 |
0.001 |
-0.042 |
H3 |
-1.533 |
-0.000 |
-1.021 |
O4 |
0.680 |
1.229 |
-0.278 |
O5 |
0.678 |
-1.231 |
-0.278 |
Atom - Atom Distances (Å)
|
Cl1 |
O2 |
H3 |
O4 |
O5 |
Cl1 | | 1.7191 | 2.1755 | 1.4705 | 1.4705 |
O2 | 1.7191 | | 0.9795 | 2.5242 | 2.5241 | H3 | 2.1755 | 0.9795 | | 2.6381 | 2.6368 | O4 | 1.4705 | 2.5242 | 2.6381 | | 2.4598 | O5 | 1.4705 | 2.5241 | 2.6368 | 2.4598 | |
More geometry information
Calculated Bond Angles
atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
Cl1 |
O2 |
H5 |
34.362 |
|
O2 |
Cl1 |
O3 |
25.899 |
O2 |
Cl1 |
O4 |
104.362 |
|
O3 |
Cl1 |
O4 |
90.579 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at HSEh1PBE/6-31G*
Charges (e)
Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
1 |
Cl |
1.236 |
|
|
|
2 |
O |
-0.651 |
|
|
|
3 |
H |
0.438 |
|
|
|
4 |
O |
-0.511 |
|
|
|
5 |
O |
-0.511 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
|
x |
y |
z |
Total |
|
-1.079 |
-0.001 |
0.156 |
1.091 |
CHELPG |
|
|
|
|
AIM |
|
|
|
|
ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
Primitive |
| x | y | z |
x |
-29.612 |
0.001 |
3.891 |
y |
0.001 |
-32.814 |
0.000 |
z |
3.891 |
0.000 |
-25.265 |
|
Traceless |
| x | y | z |
x |
-0.572 |
0.001 |
3.891 |
y |
0.001 |
-5.376 |
0.000 |
z |
3.891 |
0.000 |
5.948 |
|
Polar |
3z2-r2 | 11.895 |
x2-y2 | 3.202 |
xy | 0.001 |
xz | 3.891 |
yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
|
x |
y |
z |
x |
4.365 |
0.000 |
0.092 |
y |
0.000 |
4.134 |
0.000 |
z |
0.092 |
0.000 |
2.645 |
<r2> (average value of r
2) Å
2
<r2> |
75.216 |
(<r2>)1/2 |
8.673 |