Jump to
S1C2
Energy calculated at B97D3/3-21G
| hartrees |
Energy at 0K | -682.566904 |
Energy at 298.15K | |
HF Energy | -682.566904 |
Nuclear repulsion energy | 166.409382 |
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 B97D3/3-21G
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' |
3255 |
3200 |
11.63 |
|
|
|
2 |
A' |
955 |
939 |
64.29 |
|
|
|
3 |
A' |
712 |
700 |
9.95 |
|
|
|
4 |
A' |
428 |
420 |
43.24 |
|
|
|
5 |
A' |
335 |
329 |
14.36 |
|
|
|
6 |
A' |
237 |
233 |
17.07 |
|
|
|
7 |
A" |
802 |
788 |
37.87 |
|
|
|
8 |
A" |
247 |
243 |
48.60 |
|
|
|
9 |
A" |
104i |
102i |
55.87 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 3433.4 cm
-1
Scaled (by 0.983) Zero Point Vibrational Energy (zpe) 3375.0 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 B97D3/3-21G
Point Group is Cs
Cartesians (Å)
Atom |
x (Å) |
y (Å) |
z (Å) |
Cl1 |
0.400 |
0.146 |
0.000 |
O2 |
-0.231 |
-1.774 |
0.000 |
H3 |
-1.241 |
-1.645 |
0.000 |
O4 |
-0.231 |
0.835 |
1.406 |
O5 |
-0.231 |
0.835 |
-1.406 |
Atom - Atom Distances (Å)
|
Cl1 |
O2 |
H3 |
O4 |
O5 |
Cl1 | | 2.0218 | 2.4297 | 1.6882 | 1.6882 |
O2 | 2.0218 | | 1.0181 | 2.9639 | 2.9639 | H3 | 2.4297 | 1.0181 | | 3.0246 | 3.0246 | O4 | 1.6882 | 2.9639 | 3.0246 | | 2.8129 | O5 | 1.6882 | 2.9639 | 3.0246 | 2.8129 | |
More geometry information
Calculated Bond Angles
atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
Cl1 |
O2 |
H5 |
33.253 |
|
O2 |
Cl1 |
O3 |
24.295 |
O2 |
Cl1 |
O4 |
105.699 |
|
O3 |
Cl1 |
O4 |
92.759 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at B97D3/3-21G
Charges (e)
Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
1 |
Cl |
0.932 |
|
|
|
2 |
O |
-0.465 |
|
|
|
3 |
H |
0.340 |
|
|
|
4 |
O |
-0.404 |
|
|
|
5 |
O |
-0.404 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
|
x |
y |
z |
Total |
|
0.062 |
-0.625 |
0.000 |
0.628 |
CHELPG |
|
|
|
|
AIM |
|
|
|
|
ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
Primitive |
| x | y | z |
x |
-24.452 |
3.561 |
0.000 |
y |
3.561 |
-31.116 |
0.000 |
z |
0.000 |
0.000 |
-32.507 |
|
Traceless |
| x | y | z |
x |
7.359 |
3.561 |
0.000 |
y |
3.561 |
-2.637 |
0.000 |
z |
0.000 |
0.000 |
-4.722 |
|
Polar |
3z2-r2 | -9.444 |
x2-y2 | 6.664 |
xy | 3.561 |
xz | 0.000 |
yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
|
x |
y |
z |
x |
2.306 |
0.477 |
0.000 |
y |
0.477 |
5.573 |
0.000 |
z |
0.000 |
0.000 |
4.967 |
<r2> (average value of r
2) Å
2
<r2> |
94.930 |
(<r2>)1/2 |
9.743 |
Jump to
S1C1
Energy calculated at B97D3/3-21G
| hartrees |
Energy at 0K | -682.566885 |
Energy at 298.15K | |
HF Energy | -682.566885 |
Nuclear repulsion energy | 166.712301 |
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 B97D3/3-21G
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 |
3255 |
3199 |
11.65 |
|
|
|
2 |
A |
957 |
941 |
64.55 |
|
|
|
3 |
A |
802 |
788 |
37.89 |
|
|
|
4 |
A |
712 |
700 |
9.88 |
|
|
|
5 |
A |
429 |
422 |
43.73 |
|
|
|
6 |
A |
335 |
329 |
14.16 |
|
|
|
7 |
A |
249 |
244 |
50.40 |
|
|
|
8 |
A |
235 |
231 |
16.80 |
|
|
|
9 |
A |
95i |
94i |
54.05 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 3438.8 cm
-1
Scaled (by 0.983) Zero Point Vibrational Energy (zpe) 3380.3 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 B97D3/3-21G
Point Group is C1
Cartesians (Å)
Atom |
x (Å) |
y (Å) |
z (Å) |
Cl1 |
0.183 |
0.000 |
-0.384 |
O2 |
-1.788 |
-0.017 |
0.063 |
O3 |
0.795 |
1.414 |
0.307 |
O4 |
0.824 |
-1.399 |
0.310 |
H5 |
-1.756 |
0.006 |
1.081 |
Atom - Atom Distances (Å)
|
Cl1 |
O2 |
O3 |
O4 |
H5 |
Cl1 | | 2.0212 | 1.6882 | 1.6881 | 2.4300 |
O2 | 2.0212 | | 2.9625 | 2.9652 | 1.0181 | O3 | 1.6882 | 2.9625 | | 2.8128 | 3.0145 | O4 | 1.6881 | 2.9652 | 2.8128 | | 3.0369 | H5 | 2.4300 | 1.0181 | 3.0145 | 3.0369 | |
More geometry information
Calculated Bond Angles
atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
Cl1 |
O2 |
H5 |
100.974 |
|
O2 |
Cl1 |
O3 |
105.652 |
O2 |
Cl1 |
O4 |
105.797 |
|
O3 |
Cl1 |
O4 |
112.834 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at B97D3/3-21G
Charges (e)
Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
1 |
Cl |
0.932 |
|
|
|
2 |
O |
-0.465 |
|
|
|
3 |
O |
-0.404 |
|
|
|
4 |
O |
-0.403 |
|
|
|
5 |
H |
0.340 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
|
x |
y |
z |
Total |
|
-0.621 |
0.024 |
-0.119 |
0.632 |
CHELPG |
|
|
|
|
AIM |
|
|
|
|
ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
Primitive |
| x | y | z |
x |
-30.384 |
-0.048 |
-4.124 |
y |
-0.048 |
-32.507 |
0.017 |
z |
-4.124 |
0.017 |
-25.180 |
|
Traceless |
| x | y | z |
x |
-1.541 |
-0.048 |
-4.124 |
y |
-0.048 |
-4.725 |
0.017 |
z |
-4.124 |
0.017 |
6.266 |
|
Polar |
3z2-r2 | 12.531 |
x2-y2 | 2.123 |
xy | -0.048 |
xz | -4.124 |
yz | 0.017 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
|
x |
y |
z |
x |
5.634 |
-0.006 |
-0.163 |
y |
-0.006 |
4.967 |
0.010 |
z |
-0.163 |
0.010 |
2.244 |
<r2> (average value of r
2) Å
2
<r2> |
94.924 |
(<r2>)1/2 |
9.743 |