Jump to
S1C2
Energy calculated at mPW1PW91/6-31G*
| hartrees |
Energy at 0K | -686.126708 |
Energy at 298.15K | -686.129198 |
HF Energy | -686.126708 |
Nuclear repulsion energy | 191.997350 |
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 mPW1PW91/6-31G*
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' |
3687 |
3497 |
82.21 |
|
|
|
2 |
A' |
1226 |
1163 |
62.87 |
|
|
|
3 |
A' |
1050 |
996 |
56.07 |
|
|
|
4 |
A' |
646 |
612 |
199.60 |
|
|
|
5 |
A' |
515 |
488 |
27.01 |
|
|
|
6 |
A' |
401 |
380 |
10.05 |
|
|
|
7 |
A" |
1200 |
1138 |
224.39 |
|
|
|
8 |
A" |
394 |
374 |
50.70 |
|
|
|
9 |
A" |
61 |
58 |
68.45 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 4589.8 cm
-1
Scaled (by 0.9483) Zero Point Vibrational Energy (zpe) 4352.5 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 mPW1PW91/6-31G*
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 |
-1.179 |
-1.417 |
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 | | 1.7188 | 2.1761 | 1.4708 | 1.4708 |
O2 | 1.7188 | | 0.9785 | 2.5245 | 2.5245 | H3 | 2.1761 | 0.9785 | | 2.6393 | 2.6393 | O4 | 1.4708 | 2.5245 | 2.6393 | | 2.4603 | O5 | 1.4708 | 2.5245 | 2.6393 | 2.4603 | |
More geometry information
Calculated Bond Angles
atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
Cl1 |
O2 |
H5 |
34.358 |
|
O2 |
Cl1 |
O3 |
25.847 |
O2 |
Cl1 |
O4 |
104.380 |
|
O3 |
Cl1 |
O4 |
90.600 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at mPW1PW91/6-31G*
Charges (e)
Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
1 |
Cl |
1.246 |
|
|
|
2 |
O |
-0.655 |
|
|
|
3 |
H |
0.439 |
|
|
|
4 |
O |
-0.515 |
|
|
|
5 |
O |
-0.515 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
|
x |
y |
z |
Total |
|
0.048 |
-1.105 |
0.000 |
1.106 |
CHELPG |
|
|
|
|
AIM |
|
|
|
|
ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
Primitive |
| x | y | z |
x |
-24.432 |
3.356 |
0.000 |
y |
3.356 |
-30.357 |
0.000 |
z |
0.000 |
0.000 |
-32.808 |
|
Traceless |
| x | y | z |
x |
7.150 |
3.356 |
0.000 |
y |
3.356 |
-1.737 |
0.000 |
z |
0.000 |
0.000 |
-5.414 |
|
Polar |
3z2-r2 | -10.827 |
x2-y2 | 5.925 |
xy | 3.356 |
xz | 0.000 |
yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
|
x |
y |
z |
x |
2.669 |
0.269 |
0.000 |
y |
0.269 |
4.325 |
0.000 |
z |
0.000 |
0.000 |
4.133 |
<r2> (average value of r
2) Å
2
<r2> |
75.213 |
(<r2>)1/2 |
8.673 |
Jump to
S1C1
Energy calculated at mPW1PW91/6-31G*
| hartrees |
Energy at 0K | -686.126729 |
Energy at 298.15K | |
HF Energy | -686.126729 |
Nuclear repulsion energy | 191.997165 |
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 mPW1PW91/6-31G*
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 |
3688 |
3497 |
82.14 |
|
|
|
2 |
A |
1227 |
1164 |
62.93 |
|
|
|
3 |
A |
1201 |
1139 |
224.44 |
|
|
|
4 |
A |
1051 |
997 |
56.06 |
|
|
|
5 |
A |
645 |
612 |
199.57 |
|
|
|
6 |
A |
515 |
489 |
27.02 |
|
|
|
7 |
A |
402 |
381 |
10.00 |
|
|
|
8 |
A |
394 |
373 |
50.22 |
|
|
|
9 |
A |
53 |
50 |
68.88 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 4587.9 cm
-1
Scaled (by 0.9483) Zero Point Vibrational Energy (zpe) 4350.7 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 mPW1PW91/6-31G*
Point Group is C1
Cartesians (Å)
Atom |
x (Å) |
y (Å) |
z (Å) |
Cl1 |
-0.163 |
0.000 |
-0.341 |
O2 |
1.513 |
-0.005 |
0.042 |
H3 |
1.535 |
-0.001 |
1.020 |
O4 |
-0.675 |
1.232 |
0.278 |
O5 |
-0.684 |
-1.228 |
0.278 |
Atom - Atom Distances (Å)
|
Cl1 |
O2 |
H3 |
O4 |
O5 |
Cl1 | | 1.7193 | 2.1766 | 1.4706 | 1.4706 |
O2 | 1.7193 | | 0.9785 | 2.5245 | 2.5252 | H3 | 2.1766 | 0.9785 | | 2.6377 | 2.6416 | O4 | 1.4706 | 2.5245 | 2.6377 | | 2.4598 | O5 | 1.4706 | 2.5252 | 2.6416 | 2.4598 | |
More geometry information
Calculated Bond Angles
atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
Cl1 |
O2 |
H5 |
34.336 |
|
O2 |
Cl1 |
O3 |
25.841 |
O2 |
Cl1 |
O4 |
104.358 |
|
O3 |
Cl1 |
O4 |
90.510 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at mPW1PW91/6-31G*
Charges (e)
Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
1 |
Cl |
1.246 |
|
|
|
2 |
O |
-0.655 |
|
|
|
3 |
H |
0.439 |
|
|
|
4 |
O |
-0.515 |
|
|
|
5 |
O |
-0.515 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
|
x |
y |
z |
Total |
|
1.090 |
0.001 |
-0.166 |
1.102 |
CHELPG |
|
|
|
|
AIM |
|
|
|
|
ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
Primitive |
| x | y | z |
x |
-29.577 |
-0.001 |
3.910 |
y |
-0.001 |
-32.805 |
-0.003 |
z |
3.910 |
-0.003 |
-25.213 |
|
Traceless |
| x | y | z |
x |
-0.568 |
-0.001 |
3.910 |
y |
-0.001 |
-5.410 |
-0.003 |
z |
3.910 |
-0.003 |
5.978 |
|
Polar |
3z2-r2 | 11.955 |
x2-y2 | 3.228 |
xy | -0.001 |
xz | 3.910 |
yz | -0.003 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
|
x |
y |
z |
x |
4.366 |
0.001 |
0.087 |
y |
0.001 |
4.131 |
0.001 |
z |
0.087 |
0.001 |
2.630 |
<r2> (average value of r
2) Å
2
<r2> |
75.217 |
(<r2>)1/2 |
8.673 |