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Handbook of Solvents - George Wypych - ChemTech - Ventech!

Handbook of Solvents - George Wypych - ChemTech - Ventech!

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11.1 Theoretical treatment <strong>of</strong> solvent effects 653<br />

where Q is the numerical value <strong>of</strong> the ionic charge. The next term (l = 0) corresponds to the<br />

total dipole interaction with the corresponding reaction field (Onsager dipolar term)<br />

E Onsager<br />

a<br />

=<br />

2<br />

( 1−ε)<br />

μ<br />

3 ( 2ε+ 1)<br />

�<br />

[11.1.32]<br />

0<br />

where � μ is the dipole moment <strong>of</strong> the solute. In most applications, only these two terms that<br />

are the largest by size are considered in the calculation <strong>of</strong> the electrostatic interaction energy.<br />

However, depending on system studied, the interaction <strong>of</strong> higher electrical moments<br />

with the corresponding reaction field may become also significant and the terms corresponding<br />

to higher moments <strong>of</strong> order 2 l (quadruple, octuple, hexadecuple, etc.) should be<br />

taken into account.<br />

In many cases, the shape <strong>of</strong> the solute molecule may be very different from the sphere<br />

and therefore, it is necessary to develop the methods <strong>of</strong> calculation <strong>of</strong> the electrostatic solvation<br />

energy for more complex cavities. In the case <strong>of</strong> the ellipsoidal cavity with main<br />

semiaxes a, b, and c, the analytical formulas are still available for the calculation <strong>of</strong> the<br />

charge and dipolar terms <strong>of</strong> the electrostatic interaction with the reaction field. The charge<br />

term is simply<br />

2<br />

ell ( 1−ε)<br />

Q<br />

E Born =<br />

2ε<br />

abc<br />

whereas in the respective dipolar term 19<br />

ell<br />

E Onsager<br />

[11.1.33]<br />

= R � μ [11.1.34]<br />

the reaction field R is presented using a special tensor as follows<br />

⎛3Aa(<br />

1− Aa)(<br />

1−<br />

εμ )<br />

⎞<br />

a<br />

⎜<br />

0 0 ⎟<br />

⎜ abc[<br />

ε+ ( 1−<br />

ε)<br />

Aa]<br />

⎟<br />

⎜<br />

3Ab( 1− Ab)(<br />

1−<br />

εμ )<br />

⎟<br />

b<br />

�<br />

R = ⎜ 0<br />

0 ⎟μ<br />

⎜<br />

abc[<br />

ε+ ( 1−<br />

ε)<br />

Ab]<br />

⎟<br />

⎜<br />

3Ac( 1− Ac)(<br />

1−<br />

εμ ) ⎟<br />

c<br />

⎜<br />

0 0<br />

⎟<br />

⎝<br />

abc[<br />

ε+ ( 1−<br />

ε)<br />

Ac]<br />

⎟<br />

⎠<br />

[11.1.35]<br />

where A a,A band A c are the standard ellipsoidal shape factor integrals, and μ a, μ b and μ c are<br />

the dipole moment components along the main semiaxes <strong>of</strong> the ellipsoid. Several methods<br />

have been developed to define the semiaxes <strong>of</strong> the ellipsoidal cavity. For instance, these<br />

have been taken collinear with the axes <strong>of</strong> the solute dipole polarizability tensor, and their<br />

lengths proportional to the respective eigenvalues. 20 Another definition proceeds from the<br />

inertia tensor <strong>of</strong> the van-der-Waals solid, i.e., a solid or uniform density composed <strong>of</strong> interlocking<br />

van-der-Waals spheres. 21 Also, the ellipsoidal surface has been defined in terms <strong>of</strong><br />

the best fitting <strong>of</strong> a given molecular electrostatic isopotential surface. 22<br />

The above-discussed theoretical formulation <strong>of</strong> the electrostatic solute-solvent interaction<br />

is applicable for the fixed charge distribution inside the solute molecule. However,<br />

the solvent reaction field may cause a redistribution <strong>of</strong> the charge inside the solute. The

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