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Handbook of Solvents - George Wypych - ChemTech - Ventech!

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294 Kenneth A. Connors<br />

the three quantities on the right-hand side <strong>of</strong> eq. [5.5.42]. Thus the problem is solved in<br />

principle. 18<br />

In practice, <strong>of</strong> course, there are difficulties. Each <strong>of</strong> the δ MΔG soln terms contains three<br />

adjustable parameters, for nine in all, far too many for eq. [5.5.42] to be practicable in that<br />

form. We therefore introduce simplifications in terms <strong>of</strong> some special cases. The first thing<br />

to do is to adopt a 1-step model by setting K 2 = 0. This leaves a six-parameter equation,<br />

which, though an approximation, will <strong>of</strong>ten be acceptable, especially when the experimental<br />

study does not cover a wide range in solvent composition (as is usually the case). This<br />

simplification gives eq. [5.5.43].<br />

δ<br />

C C C<br />

S<br />

gA γ kT K K x gA γ kT<br />

Δ G<br />

C<br />

x K x<br />

* S S<br />

( ′ − ln ) ( ′ 1 1 2 − lnK<br />

) K x<br />

=<br />

−<br />

S<br />

+<br />

x + K x<br />

M comp<br />

1 1 2<br />

L L L<br />

( gA ′ −kT<br />

ln K ) K x<br />

−<br />

L<br />

x + K x<br />

γ 1 1 2<br />

1 1 2<br />

1 1 2<br />

1 1 2<br />

[5.5.43]<br />

Next, in what is labeled the full cancellation approximation, we assume K 1 C =K1 S =K1 L =<br />

K 1and we write ΔgA=gA C -gA S -gA L . The result is<br />

δ<br />

ΔG<br />

*<br />

M comp<br />

( ln + Δ γ′<br />

)<br />

kT K gA K x<br />

=<br />

x + K x<br />

1 1 2<br />

1 1 2<br />

[5.5.44]<br />

and we now have a 2-parameter model. The assumption <strong>of</strong> identical solvation constants is<br />

actually quite reasonable; recall from the solubility studies that K 1 is not markedly sensitive<br />

to the solute identity.<br />

The particular example <strong>of</strong> cyclodextrin complexes led to the identification <strong>of</strong> another<br />

special case as the partial cancellation approximation; in this case we assume K 1 C =K1 S <<br />

K 1 L , and the result is, approximately. 19<br />

δ<br />

M comp<br />

( − γ′<br />

)<br />

kT K gA K x<br />

Δ G<br />

x K x<br />

* ln<br />

=<br />

+<br />

1 1 2<br />

1 1 2<br />

[5.5.45]<br />

Functionally eqs. [5.5.44] and [5.5.45] are identical; the distinction is made on the basis<br />

<strong>of</strong> the magnitudes <strong>of</strong> the parameters found. Note that gA in eq. [5.5.45] is a positive<br />

quantity whereas ΔgA in eq. [5.5.44] is a negative quantity. In eq. [5.5.45] it is understood<br />

that gA and K 1 refer to L. Eqs. [5.5.44] and [5.5.45] both have the form<br />

δ<br />

M comp<br />

( + γ′<br />

)<br />

kT K G K x<br />

Δ G<br />

x K x<br />

* ln<br />

=<br />

+<br />

1 1 2<br />

1 1 2<br />

[5.5.46]<br />

where G = ΔgA in eq. [5.5.44] and G = -gA in eq. [5.5.45]. Table 5.5.5 shows G and K 1 values<br />

obtained in studies <strong>of</strong> α-cyclodextrin complexes. 19,20 The assignments are made on the<br />

basis <strong>of</strong> the magnitude <strong>of</strong> K 1; those values substantially higher than typical solubility K 1 values<br />

suggest that the full cancellation condition is not satisfied. After the assignments are<br />

made, G can be interpreted as either ΔgA (full cancellation) or -gA (partial cancellation).

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