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Handbook of Solvents - George Wypych - ChemTech - Ventech!

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528 Y. Y. Fialkov, V. L. Chumak<br />

ΔG = σ −σ −ΔG<br />

solv, E solv, F<br />

( v )<br />

[9.48]<br />

The variation <strong>of</strong> free energy due to any chemical process consists <strong>of</strong> both covalent and<br />

electrostatic components:<br />

ΔG ΔG ΔG<br />

el<br />

= −<br />

(cov) ( )<br />

[9.49]<br />

Substituting [9.49] in [9.48], we come to an equation that in general describes the<br />

mixed solvent effect on the equilibrium chemical process:<br />

(cov) (cov) ( ,<br />

, )<br />

( el )<br />

solv E solv F ( solv, E solv,<br />

F)<br />

ΔG ΔG<br />

v ( )<br />

( el )<br />

=− + σ − σ + σ −σ<br />

[9.50]<br />

(el) (cov)<br />

For universal (chemically indifferent) solvents where σ >> σ , it may by assumed<br />

that<br />

ΔG ΔG<br />

v ( ) ( el ) ( el )<br />

=− + σ −σ<br />

[9.51]<br />

solv, E<br />

solv, F<br />

Thus the mixed solvent effect on the equilibrium <strong>of</strong> the chemical process [9.45] is determined<br />

not only by the vacuum component but also by the solvation energy <strong>of</strong> each <strong>of</strong> the<br />

chemical forms <strong>of</strong> equilibrium members.<br />

From free energy to equilibrium constants, one can obtain the equation describing<br />

mixed solvent effect on the equilibrium constant <strong>of</strong> the [9.45] process:<br />

( ) (cov) (cov)<br />

( el ) ( el )<br />

[ Δ ( σ σ solv, F solv, E ) ( σ σ<br />

solv, F solv,<br />

E ) ]<br />

lnK<br />

G v<br />

= + − + −<br />

/ RT [9.52]<br />

In the special case <strong>of</strong> universal media, i.e., mixed solvent formed by both solvation-inert<br />

components, this equation can be presented as:<br />

( el ) ( el )<br />

[ solv, f solv, E ]<br />

( univ ) ( v )<br />

ln K = ΔG + σ −σ<br />

/ RT<br />

[9.53]<br />

Because the energy <strong>of</strong> all types <strong>of</strong> electrostatic interaction is inversely proportional to<br />

permittivity, these equations can be rewritten in the form:<br />

and<br />

( ) (cov) (cov)<br />

[ Δ ( σ σ solv, F solv, E ) ( βsolv, F βsolv,<br />

E)<br />

]<br />

lnK<br />

G v<br />

= + − + −<br />

[ ( solv, F solv, E ) ]<br />

/ ε / RT [9.52a]<br />

( univ ) ( v )<br />

ln K = ΔG + β −β<br />

/ ε / RT<br />

[9.53a]<br />

where:<br />

β the multipliers <strong>of</strong> the magnitudes <strong>of</strong> reciprocal permittivity in equations <strong>of</strong> energy <strong>of</strong> the<br />

main types <strong>of</strong> electrostatic interactions such as dipole-dipole, ion-dipole, and ion-ion<br />

interactions<br />

As follows from [9.52a], in binary mixed solvents formed from solvation-indifferent<br />

components (i.e., universal media), equilibrium constants <strong>of</strong> the [9.45] process are expo-

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