Jump to
S1C2
Energy calculated at wB97X-D/cc-pVQZ
| hartrees |
Energy at 0K | -686.292278 |
Energy at 298.15K | |
HF Energy | -686.292278 |
Nuclear repulsion energy | |
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 wB97X-D/cc-pVQZ
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' |
3763 |
3763 |
93.73 |
|
|
|
2 |
A' |
1220 |
1220 |
76.35 |
|
|
|
3 |
A' |
1087 |
1087 |
48.08 |
|
|
|
4 |
A' |
656 |
656 |
222.39 |
|
|
|
5 |
A' |
555 |
555 |
28.53 |
|
|
|
6 |
A' |
440 |
440 |
5.04 |
|
|
|
7 |
A" |
1241 |
1241 |
264.06 |
|
|
|
8 |
A" |
422 |
422 |
29.39 |
|
|
|
9 |
A" |
59i |
59i |
68.74 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 4662.7 cm
-1
Scaled (by 1) Zero Point Vibrational Energy (zpe) 4662.7 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 wB97X-D/cc-pVQZ
Point Group is Cs
Cartesians (Å)
Atom |
x (Å) |
y (Å) |
z (Å) |
Cl1 |
0.354 |
0.118 |
0.000 |
O2 |
-0.202 |
-1.464 |
0.000 |
H3 |
-1.168 |
-1.392 |
0.000 |
O4 |
-0.202 |
0.693 |
1.197 |
O5 |
-0.202 |
0.693 |
-1.197 |
Atom - Atom Distances (Å)
|
Cl1 |
O2 |
H3 |
O4 |
O5 |
Cl1 | | 1.6768 | 2.1438 | 1.4396 | 1.4396 |
O2 | 1.6768 | | 0.9686 | 2.4667 | 2.4667 | H3 | 2.1438 | 0.9686 | | 2.5907 | 2.5907 | O4 | 1.4396 | 2.4667 | 2.5907 | | 2.3941 | O5 | 1.4396 | 2.4667 | 2.5907 | 2.3941 | |
More geometry information
Calculated Bond Angles
atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
Cl1 |
O2 |
H5 |
34.422 |
|
O2 |
Cl1 |
O3 |
25.863 |
O2 |
Cl1 |
O4 |
104.396 |
|
O3 |
Cl1 |
O4 |
90.403 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at wB97X-D/cc-pVQZ
Charges (e)
Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
1 |
Cl |
1.059 |
|
|
|
2 |
O |
-0.385 |
|
|
|
3 |
H |
0.253 |
|
|
|
4 |
O |
-0.463 |
|
|
|
5 |
O |
-0.463 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
|
x |
y |
z |
Total |
|
-0.002 |
-1.240 |
0.000 |
1.240 |
CHELPG |
|
|
|
|
AIM |
|
|
|
|
ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
Primitive |
| x | y | z |
x |
-24.815 |
3.199 |
0.000 |
y |
3.199 |
-29.954 |
0.000 |
z |
0.000 |
0.000 |
-32.641 |
|
Traceless |
| x | y | z |
x |
6.483 |
3.199 |
0.000 |
y |
3.199 |
-1.226 |
0.000 |
z |
0.000 |
0.000 |
-5.256 |
|
Polar |
3z2-r2 | -10.513 |
x2-y2 | 5.139 |
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 |
3.405 |
0.225 |
0.000 |
y |
0.225 |
4.916 |
0.000 |
z |
0.000 |
0.000 |
4.702 |
<r2> (average value of r
2) Å
2
<r2> |
72.597 |
(<r2>)1/2 |
8.520 |
Jump to
S1C1
Energy calculated at wB97X-D/cc-pVQZ
| hartrees |
Energy at 0K | -686.292341 |
Energy at 298.15K | |
HF Energy | -686.292341 |
Nuclear repulsion energy | 196.393197 |
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 wB97X-D/cc-pVQZ
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 |
100.41 |
|
|
|
2 |
A |
1252 |
1252 |
228.51 |
|
|
|
3 |
A |
1209 |
1209 |
108.46 |
|
|
|
4 |
A |
1083 |
1083 |
49.01 |
|
|
|
5 |
A |
664 |
664 |
219.16 |
|
|
|
6 |
A |
560 |
560 |
29.61 |
|
|
|
7 |
A |
443 |
443 |
6.25 |
|
|
|
8 |
A |
399 |
399 |
15.19 |
|
|
|
9 |
A |
90 |
90 |
81.78 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 4732.7 cm
-1
Scaled (by 1) Zero Point Vibrational Energy (zpe) 4732.7 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 wB97X-D/cc-pVQZ
Point Group is C1
Cartesians (Å)
Atom |
x (Å) |
y (Å) |
z (Å) |
Cl1 |
-0.160 |
0.012 |
-0.339 |
O2 |
1.431 |
-0.351 |
0.056 |
H3 |
1.577 |
0.100 |
0.900 |
O4 |
-0.348 |
1.318 |
0.246 |
O5 |
-0.940 |
-1.006 |
0.305 |
Atom - Atom Distances (Å)
|
Cl1 |
O2 |
H3 |
O4 |
O5 |
Cl1 | | 1.6789 | 2.1356 | 1.4436 | 1.4352 |
O2 | 1.6789 | | 0.9684 | 2.4470 | 2.4726 | H3 | 2.1356 | 0.9684 | | 2.3703 | 2.8133 | O4 | 1.4436 | 2.4470 | 2.3703 | | 2.3991 | O5 | 1.4352 | 2.4726 | 2.8133 | 2.3991 | |
More geometry information
Calculated Bond Angles
atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
Cl1 |
O2 |
H5 |
34.130 |
|
O2 |
Cl1 |
O3 |
26.063 |
O2 |
Cl1 |
O4 |
102.939 |
|
O3 |
Cl1 |
O4 |
80.420 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at wB97X-D/cc-pVQZ
Charges (e)
Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
1 |
Cl |
1.060 |
|
|
|
2 |
O |
-0.390 |
|
|
|
3 |
H |
0.256 |
|
|
|
4 |
O |
-0.481 |
|
|
|
5 |
O |
-0.446 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
|
x |
y |
z |
Total |
|
1.307 |
0.287 |
-0.327 |
1.377 |
CHELPG |
|
|
|
|
AIM |
|
|
|
|
ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
Primitive |
| x | y | z |
x |
-28.723 |
0.519 |
3.480 |
y |
0.519 |
-32.547 |
0.317 |
z |
3.480 |
0.317 |
-26.109 |
|
Traceless |
| x | y | z |
x |
0.605 |
0.519 |
3.480 |
y |
0.519 |
-5.131 |
0.317 |
z |
3.480 |
0.317 |
4.526 |
|
Polar |
3z2-r2 | 9.052 |
x2-y2 | 3.824 |
xy | 0.519 |
xz | 3.480 |
yz | 0.317 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
|
x |
y |
z |
x |
4.985 |
0.057 |
0.066 |
y |
0.057 |
4.729 |
0.063 |
z |
0.066 |
0.063 |
3.307 |
<r2> (average value of r
2) Å
2
<r2> |
72.551 |
(<r2>)1/2 |
8.518 |