Jump to
S1C2
Energy calculated at PBE1PBE/cc-pVDZ
| hartrees |
Energy at 0K | -685.814414 |
Energy at 298.15K | -685.816892 |
HF Energy | -685.814414 |
Nuclear repulsion energy | 190.441003 |
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 PBE1PBE/cc-pVDZ
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' |
3693 |
3551 |
82.18 |
|
|
|
2 |
A' |
1164 |
1119 |
55.89 |
|
|
|
3 |
A' |
1025 |
986 |
53.32 |
|
|
|
4 |
A' |
625 |
601 |
184.28 |
|
|
|
5 |
A' |
501 |
482 |
26.95 |
|
|
|
6 |
A' |
387 |
373 |
10.46 |
|
|
|
7 |
A" |
1165 |
1120 |
216.80 |
|
|
|
8 |
A" |
384 |
369 |
45.48 |
|
|
|
9 |
A" |
74 |
72 |
56.08 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 4509.4 cm
-1
Scaled (by 0.9615) Zero Point Vibrational Energy (zpe) 4335.8 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 PBE1PBE/cc-pVDZ
Point Group is Cs
Cartesians (Å)
Atom |
x (Å) |
y (Å) |
z (Å) |
Cl1 |
0.362 |
0.125 |
0.000 |
O2 |
-0.207 |
-1.518 |
0.000 |
H3 |
-1.179 |
-1.396 |
0.000 |
O4 |
-0.207 |
0.714 |
1.236 |
O5 |
-0.207 |
0.714 |
-1.236 |
Atom - Atom Distances (Å)
|
Cl1 |
O2 |
H3 |
O4 |
O5 |
Cl1 | | 1.7381 | 2.1648 | 1.4826 | 1.4826 |
O2 | 1.7381 | | 0.9790 | 2.5508 | 2.5508 | H3 | 2.1648 | 0.9790 | | 2.6313 | 2.6313 | O4 | 1.4826 | 2.5508 | 2.6313 | | 2.4720 | O5 | 1.4826 | 2.5508 | 2.6313 | 2.4720 | |
More geometry information
Calculated Bond Angles
atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
Cl1 |
O2 |
H5 |
34.251 |
|
O2 |
Cl1 |
O3 |
26.257 |
O2 |
Cl1 |
O4 |
104.466 |
|
O3 |
Cl1 |
O4 |
90.350 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at PBE1PBE/cc-pVDZ
Charges (e)
Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
1 |
Cl |
0.979 |
|
|
|
2 |
O |
-0.341 |
|
|
|
3 |
H |
0.189 |
|
|
|
4 |
O |
-0.414 |
|
|
|
5 |
O |
-0.414 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
|
x |
y |
z |
Total |
|
0.223 |
-1.025 |
0.000 |
1.049 |
CHELPG |
|
|
|
|
AIM |
|
|
|
|
ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
Primitive |
| x | y | z |
x |
-24.443 |
3.049 |
0.000 |
y |
3.049 |
-30.531 |
0.000 |
z |
0.000 |
0.000 |
-32.824 |
|
Traceless |
| x | y | z |
x |
7.234 |
3.049 |
0.000 |
y |
3.049 |
-1.897 |
0.000 |
z |
0.000 |
0.000 |
-5.337 |
|
Polar |
3z2-r2 | -10.674 |
x2-y2 | 6.088 |
xy | 3.049 |
xz | 0.000 |
yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
|
x |
y |
z |
x |
2.503 |
0.312 |
0.000 |
y |
0.312 |
4.350 |
0.000 |
z |
0.000 |
0.000 |
4.066 |
<r2> (average value of r
2) Å
2
<r2> |
76.155 |
(<r2>)1/2 |
8.727 |
Jump to
S1C1
Energy calculated at PBE1PBE/cc-pVDZ
| hartrees |
Energy at 0K | -685.814434 |
Energy at 298.15K | |
HF Energy | -685.814434 |
Nuclear repulsion energy | 190.455138 |
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 PBE1PBE/cc-pVDZ
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 |
3693 |
3551 |
82.29 |
|
|
|
2 |
A |
1165 |
1120 |
216.23 |
|
|
|
3 |
A |
1165 |
1120 |
56.35 |
|
|
|
4 |
A |
1025 |
986 |
53.49 |
|
|
|
5 |
A |
626 |
602 |
184.35 |
|
|
|
6 |
A |
502 |
482 |
26.95 |
|
|
|
7 |
A |
388 |
373 |
10.52 |
|
|
|
8 |
A |
384 |
369 |
44.95 |
|
|
|
9 |
A |
65 |
62 |
56.65 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 4506.5 cm
-1
Scaled (by 0.9615) Zero Point Vibrational Energy (zpe) 4333.0 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 PBE1PBE/cc-pVDZ
Point Group is C1
Cartesians (Å)
Atom |
x (Å) |
y (Å) |
z (Å) |
Cl1 |
-0.162 |
0.000 |
-0.347 |
O2 |
1.531 |
-0.001 |
0.048 |
H3 |
1.511 |
0.000 |
1.027 |
O4 |
-0.688 |
1.236 |
0.280 |
O5 |
-0.688 |
-1.236 |
0.281 |
Atom - Atom Distances (Å)
|
Cl1 |
O2 |
H3 |
O4 |
O5 |
Cl1 | | 1.7375 | 2.1644 | 1.4827 | 1.4827 |
O2 | 1.7375 | | 0.9791 | 2.5503 | 2.5503 | H3 | 2.1644 | 0.9791 | | 2.6305 | 2.6312 | O4 | 1.4827 | 2.5503 | 2.6305 | | 2.4721 | O5 | 1.4827 | 2.5503 | 2.6312 | 2.4721 | |
More geometry information
Calculated Bond Angles
atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
Cl1 |
O2 |
H5 |
34.260 |
|
O2 |
Cl1 |
O3 |
26.262 |
O2 |
Cl1 |
O4 |
104.459 |
|
O3 |
Cl1 |
O4 |
90.325 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at PBE1PBE/cc-pVDZ
Charges (e)
Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
1 |
Cl |
0.979 |
|
|
|
2 |
O |
-0.341 |
|
|
|
3 |
H |
0.189 |
|
|
|
4 |
O |
-0.414 |
|
|
|
5 |
O |
-0.414 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
|
x |
y |
z |
Total |
|
0.999 |
0.001 |
-0.328 |
1.052 |
CHELPG |
|
|
|
|
AIM |
|
|
|
|
ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
Primitive |
| x | y | z |
x |
-29.829 |
0.001 |
3.614 |
y |
0.001 |
-32.826 |
0.001 |
z |
3.614 |
0.001 |
-25.142 |
|
Traceless |
| x | y | z |
x |
-0.845 |
0.001 |
3.614 |
y |
0.001 |
-5.340 |
0.001 |
z |
3.614 |
0.001 |
6.185 |
|
Polar |
3z2-r2 | 12.371 |
x2-y2 | 2.997 |
xy | 0.001 |
xz | 3.614 |
yz | 0.001 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
|
x |
y |
z |
x |
4.391 |
0.000 |
0.113 |
y |
0.000 |
4.066 |
0.000 |
z |
0.113 |
0.000 |
2.458 |
<r2> (average value of r
2) Å
2
<r2> |
76.141 |
(<r2>)1/2 |
8.726 |