Jump to
S1C2
Energy calculated at mPW1PW91/3-21G*
| hartrees |
Energy at 0K | -682.794704 |
Energy at 298.15K | |
HF Energy | -682.794704 |
Nuclear repulsion energy | 190.417645 |
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 mPW1PW91/3-21G*
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' |
3425 |
3252 |
33.59 |
|
|
|
2 |
A' |
1168 |
1109 |
51.90 |
|
|
|
3 |
A' |
1002 |
951 |
45.15 |
|
|
|
4 |
A' |
624 |
592 |
172.71 |
|
|
|
5 |
A' |
503 |
478 |
25.02 |
|
|
|
6 |
A' |
391 |
371 |
18.24 |
|
|
|
7 |
A" |
1176 |
1117 |
159.63 |
|
|
|
8 |
A" |
395 |
375 |
69.48 |
|
|
|
9 |
A" |
12i |
11i |
73.44 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 4335.5 cm
-1
Scaled (by 0.9496) Zero Point Vibrational Energy (zpe) 4117.0 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 mPW1PW91/3-21G*
Point Group is Cs
Cartesians (Å)
Atom |
x (Å) |
y (Å) |
z (Å) |
Cl1 |
0.357 |
0.129 |
0.000 |
O2 |
-0.202 |
-1.511 |
0.000 |
H3 |
-1.207 |
-1.472 |
0.000 |
O4 |
-0.202 |
0.710 |
1.241 |
O5 |
-0.202 |
0.710 |
-1.241 |
Atom - Atom Distances (Å)
|
Cl1 |
O2 |
H3 |
O4 |
O5 |
Cl1 | | 1.7326 | 2.2380 | 1.4801 | 1.4801 |
O2 | 1.7326 | | 1.0051 | 2.5442 | 2.5442 | H3 | 2.2380 | 1.0051 | | 2.7039 | 2.7039 | O4 | 1.4801 | 2.5442 | 2.7039 | | 2.4820 | O5 | 1.4801 | 2.5442 | 2.7039 | 2.4820 | |
More geometry information
Calculated Bond Angles
atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
Cl1 |
O2 |
H5 |
34.286 |
|
O2 |
Cl1 |
O3 |
25.489 |
O2 |
Cl1 |
O4 |
104.456 |
|
O3 |
Cl1 |
O4 |
90.968 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at mPW1PW91/3-21G*
Charges (e)
Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
1 |
Cl |
1.122 |
|
|
|
2 |
O |
-0.569 |
|
|
|
3 |
H |
0.376 |
|
|
|
4 |
O |
-0.464 |
|
|
|
5 |
O |
-0.464 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
|
x |
y |
z |
Total |
|
-0.079 |
-1.054 |
0.000 |
1.056 |
CHELPG |
|
|
|
|
AIM |
|
|
|
|
ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
Primitive |
| x | y | z |
x |
-23.949 |
3.635 |
0.000 |
y |
3.635 |
-30.283 |
0.000 |
z |
0.000 |
0.000 |
-32.791 |
|
Traceless |
| x | y | z |
x |
7.588 |
3.635 |
0.000 |
y |
3.635 |
-1.913 |
0.000 |
z |
0.000 |
0.000 |
-5.675 |
|
Polar |
3z2-r2 | -11.349 |
x2-y2 | 6.334 |
xy | 3.635 |
xz | 0.000 |
yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
|
x |
y |
z |
x |
2.247 |
0.375 |
0.000 |
y |
0.375 |
3.794 |
0.000 |
z |
0.000 |
0.000 |
3.547 |
<r2> (average value of r
2) Å
2
<r2> |
76.144 |
(<r2>)1/2 |
8.726 |
Jump to
S1C1
Energy calculated at mPW1PW91/3-21G*
| hartrees |
Energy at 0K | -682.794707 |
Energy at 298.15K | |
HF Energy | -682.794707 |
Nuclear repulsion energy | 190.421957 |
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 mPW1PW91/3-21G*
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 |
3425 |
3252 |
33.55 |
|
|
|
2 |
A |
1177 |
1118 |
157.44 |
|
|
|
3 |
A |
1167 |
1108 |
54.27 |
|
|
|
4 |
A |
1002 |
952 |
44.85 |
|
|
|
5 |
A |
623 |
591 |
172.51 |
|
|
|
6 |
A |
503 |
478 |
25.13 |
|
|
|
7 |
A |
396 |
376 |
59.35 |
|
|
|
8 |
A |
390 |
370 |
28.02 |
|
|
|
9 |
A |
29i |
27i |
74.07 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 4327.1 cm
-1
Scaled (by 0.9496) Zero Point Vibrational Energy (zpe) 4109.0 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 mPW1PW91/3-21G*
Point Group is C1
Cartesians (Å)
Atom |
x (Å) |
y (Å) |
z (Å) |
Cl1 |
-0.168 |
0.002 |
-0.340 |
O2 |
1.523 |
-0.046 |
0.035 |
H3 |
1.596 |
-0.005 |
1.037 |
O4 |
-0.643 |
1.261 |
0.276 |
O5 |
-0.724 |
-1.219 |
0.283 |
Atom - Atom Distances (Å)
|
Cl1 |
O2 |
H3 |
O4 |
O5 |
Cl1 | | 1.7331 | 2.2381 | 1.4803 | 1.4795 |
O2 | 1.7331 | | 1.0050 | 2.5415 | 2.5472 | H3 | 2.2381 | 1.0050 | | 2.6825 | 2.7252 | O4 | 1.4803 | 2.5415 | 2.6825 | | 2.4816 | O5 | 1.4795 | 2.5472 | 2.7252 | 2.4816 | |
More geometry information
Calculated Bond Angles
atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
Cl1 |
O2 |
H5 |
34.193 |
|
O2 |
Cl1 |
O3 |
25.487 |
O2 |
Cl1 |
O4 |
104.270 |
|
O3 |
Cl1 |
O4 |
89.964 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at mPW1PW91/3-21G*
Charges (e)
Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
1 |
Cl |
1.122 |
|
|
|
2 |
O |
-0.569 |
|
|
|
3 |
H |
0.376 |
|
|
|
4 |
O |
-0.466 |
|
|
|
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 |
|
1.054 |
0.028 |
-0.040 |
1.055 |
CHELPG |
|
|
|
|
AIM |
|
|
|
|
ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
Primitive |
| x | y | z |
x |
-29.409 |
0.035 |
4.237 |
y |
0.035 |
-32.789 |
-0.015 |
z |
4.237 |
-0.015 |
-24.823 |
|
Traceless |
| x | y | z |
x |
-0.603 |
0.035 |
4.237 |
y |
0.035 |
-5.673 |
-0.015 |
z |
4.237 |
-0.015 |
6.276 |
|
Polar |
3z2-r2 | 12.551 |
x2-y2 | 3.380 |
xy | 0.035 |
xz | 4.237 |
yz | -0.015 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
|
x |
y |
z |
x |
3.860 |
0.009 |
0.198 |
y |
0.009 |
3.546 |
0.013 |
z |
0.198 |
0.013 |
2.182 |
<r2> (average value of r
2) Å
2
<r2> |
76.145 |
(<r2>)1/2 |
8.726 |