Jump to
S1C2
Energy calculated at B1B95/cc-pVTZ
| hartrees |
Energy at 0K | -686.323446 |
Energy at 298.15K | |
HF Energy | -686.323446 |
Nuclear repulsion energy | 195.258902 |
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 B1B95/cc-pVTZ
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' |
3734 |
3574 |
91.53 |
|
|
|
2 |
A' |
1201 |
1150 |
69.64 |
|
|
|
3 |
A' |
1071 |
1025 |
48.17 |
|
|
|
4 |
A' |
649 |
621 |
215.25 |
|
|
|
5 |
A' |
541 |
518 |
25.14 |
|
|
|
6 |
A' |
424 |
406 |
7.04 |
|
|
|
7 |
A" |
1225 |
1172 |
247.40 |
|
|
|
8 |
A" |
411 |
393 |
33.12 |
|
|
|
9 |
A" |
79i |
75i |
63.91 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 4588.6 cm
-1
Scaled (by 0.9571) Zero Point Vibrational Energy (zpe) 4391.8 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 B1B95/cc-pVTZ
Point Group is Cs
Cartesians (Å)
Atom |
x (Å) |
y (Å) |
z (Å) |
Cl1 |
0.357 |
0.119 |
0.000 |
O2 |
-0.204 |
-1.474 |
0.000 |
H3 |
-1.170 |
-1.380 |
0.000 |
O4 |
-0.204 |
0.696 |
1.203 |
O5 |
-0.204 |
0.696 |
-1.203 |
Atom - Atom Distances (Å)
|
Cl1 |
O2 |
H3 |
O4 |
O5 |
Cl1 | | 1.6886 | 2.1399 | 1.4476 | 1.4476 |
O2 | 1.6886 | | 0.9704 | 2.4814 | 2.4814 | H3 | 2.1399 | 0.9704 | | 2.5875 | 2.5875 | O4 | 1.4476 | 2.4814 | 2.5875 | | 2.4067 | O5 | 1.4476 | 2.4814 | 2.5875 | 2.4067 | |
More geometry information
Calculated Bond Angles
atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
Cl1 |
O2 |
H5 |
34.416 |
|
O2 |
Cl1 |
O3 |
26.121 |
O2 |
Cl1 |
O4 |
104.339 |
|
O3 |
Cl1 |
O4 |
90.188 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at B1B95/cc-pVTZ
Charges (e)
Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
1 |
Cl |
0.887 |
|
|
|
2 |
O |
-0.323 |
|
|
|
3 |
H |
0.222 |
|
|
|
4 |
O |
-0.393 |
|
|
|
5 |
O |
-0.393 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
|
x |
y |
z |
Total |
|
0.075 |
-1.160 |
0.000 |
1.162 |
CHELPG |
|
|
|
|
AIM |
|
|
|
|
ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
Primitive |
| x | y | z |
x |
-24.610 |
3.084 |
0.000 |
y |
3.084 |
-30.030 |
0.000 |
z |
0.000 |
0.000 |
-32.579 |
|
Traceless |
| x | y | z |
x |
6.695 |
3.084 |
0.000 |
y |
3.084 |
-1.435 |
0.000 |
z |
0.000 |
0.000 |
-5.259 |
|
Polar |
3z2-r2 | -10.519 |
x2-y2 | 5.420 |
xy | 3.084 |
xz | 0.000 |
yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
|
x |
y |
z |
x |
3.064 |
0.266 |
0.000 |
y |
0.266 |
4.615 |
0.000 |
z |
0.000 |
0.000 |
4.377 |
<r2> (average value of r
2) Å
2
<r2> |
73.138 |
(<r2>)1/2 |
8.552 |
Jump to
S1C1
Energy calculated at B1B95/cc-pVTZ
| hartrees |
Energy at 0K | -686.323508 |
Energy at 298.15K | |
HF Energy | -686.323508 |
Nuclear repulsion energy | 195.320843 |
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 B1B95/cc-pVTZ
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 |
3737 |
3577 |
97.79 |
|
|
|
2 |
A |
1236 |
1183 |
208.02 |
|
|
|
3 |
A |
1193 |
1142 |
104.93 |
|
|
|
4 |
A |
1066 |
1020 |
50.61 |
|
|
|
5 |
A |
655 |
627 |
211.14 |
|
|
|
6 |
A |
543 |
520 |
28.17 |
|
|
|
7 |
A |
428 |
410 |
8.18 |
|
|
|
8 |
A |
385 |
368 |
18.52 |
|
|
|
9 |
A |
129 |
124 |
77.42 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 4685.8 cm
-1
Scaled (by 0.9571) Zero Point Vibrational Energy (zpe) 4484.8 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 B1B95/cc-pVTZ
Point Group is C1
Cartesians (Å)
Atom |
x (Å) |
y (Å) |
z (Å) |
Cl1 |
-0.161 |
0.014 |
-0.342 |
O2 |
1.434 |
-0.379 |
0.059 |
H3 |
1.570 |
0.085 |
0.899 |
O4 |
-0.321 |
1.331 |
0.247 |
O5 |
-0.967 |
-0.991 |
0.308 |
Atom - Atom Distances (Å)
|
Cl1 |
O2 |
H3 |
O4 |
O5 |
Cl1 | | 1.6906 | 2.1307 | 1.4519 | 1.4429 |
O2 | 1.6906 | | 0.9701 | 2.4576 | 2.4903 | H3 | 2.1307 | 0.9701 | | 2.3562 | 2.8182 | O4 | 1.4519 | 2.4576 | 2.3562 | | 2.4118 | O5 | 1.4429 | 2.4903 | 2.8182 | 2.4118 | |
More geometry information
Calculated Bond Angles
atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
Cl1 |
O2 |
H5 |
34.037 |
|
O2 |
Cl1 |
O3 |
26.330 |
O2 |
Cl1 |
O4 |
102.634 |
|
O3 |
Cl1 |
O4 |
79.795 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at B1B95/cc-pVTZ
Charges (e)
Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
1 |
Cl |
0.888 |
|
|
|
2 |
O |
-0.325 |
|
|
|
3 |
H |
0.223 |
|
|
|
4 |
O |
-0.408 |
|
|
|
5 |
O |
-0.377 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
|
x |
y |
z |
Total |
|
1.222 |
0.277 |
-0.403 |
1.316 |
CHELPG |
|
|
|
|
AIM |
|
|
|
|
ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
Primitive |
| x | y | z |
x |
-28.804 |
0.479 |
3.404 |
y |
0.479 |
-32.494 |
0.286 |
z |
3.404 |
0.286 |
-25.889 |
|
Traceless |
| x | y | z |
x |
0.388 |
0.479 |
3.404 |
y |
0.479 |
-5.148 |
0.286 |
z |
3.404 |
0.286 |
4.760 |
|
Polar |
3z2-r2 | 9.520 |
x2-y2 | 3.691 |
xy | 0.479 |
xz | 3.404 |
yz | 0.286 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
|
x |
y |
z |
x |
4.701 |
0.071 |
0.107 |
y |
0.071 |
4.403 |
0.082 |
z |
0.107 |
0.082 |
2.936 |
<r2> (average value of r
2) Å
2
<r2> |
73.080 |
(<r2>)1/2 |
8.549 |