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Handbook of Solvents - George Wypych - ChemTech - Ventech!

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772 Roland Schmid<br />

simulations. 188-191 It should be emphasized, however, that the present discussion might be<br />

confined to water as the solvent. Recent theoretical treatments advise the cavity radius not<br />

to be considered as an intrinsic property <strong>of</strong> the solute, but instead to vary with solvent polarity,<br />

with orientational saturation prevailing at low polarity and electrostriction at high polarity.<br />

191,192 It would appear that the whole area <strong>of</strong> nonaqueous ion solvation deserves more<br />

methodical attention. It should in addition be emphasized that the cavity radius is sensitive<br />

to temperature. Combining eq. [13.1.29] with<br />

o ⎛∂ΔG<br />

* ⎞<br />

ΔH = ΔG<br />

* + T⎜<br />

⎟<br />

⎝ ∂T<br />

⎠<br />

one obtains 177<br />

⎡<br />

o<br />

ΔH = ΔG<br />

* ⎢1+<br />

⎣⎢<br />

T ⎛ ⎞ T r<br />

⎜ ⎟ −<br />

⎝ T ⎠ r T<br />

⎛ ∂ε ∂ ⎞<br />

⎜ ⎟<br />

ε ε ∂ ⎝∂⎠<br />

( −1)<br />

P P<br />

⎤<br />

⎥<br />

⎦⎥<br />

[13.1.33]<br />

[13.1.34]<br />

The derivation <strong>of</strong> (∂r/∂T) P from reliable values <strong>of</strong> ΔH° and ΔG* is interesting, in that<br />

nominally the dielectric effect (-0.018 for water) is smaller than the size effect (-0.069 for<br />

chloride), a result that has not given previously the attention due to it. Consequently, as<br />

Roux et al. 177 stated, unless a precise procedure for evaluating the dependence <strong>of</strong> the radius<br />

on the temperature is available, the Born model should be restricted to the free energy <strong>of</strong> solvation.<br />

Notwithstanding this, beginning with Voet, 172 the Born model has usually been<br />

tested by considering the enthalpies <strong>of</strong> hydration. 193 The reason for the relative success lies<br />

in the fact that ion hydration is strongly enthalpy controlled, i.e., ΔH° ~ ΔG*.<br />

The discussion <strong>of</strong> radii given here should have implications to all calculations involving<br />

aqueous ionic radii, for instance the solvent reorganization energy in connection with<br />

eq. [13.1.26]. Thus, treatments using the crystal radii as an input parameter 194-197 may be revisited.<br />

13.1.8 THE FUTURE OF THE PHENOMENOLOGICAL APPROACH<br />

Originally, the empirical solvent parameters have been introduced to provide guidelines for<br />

the comparison <strong>of</strong> different solvent qualities and for an orientation in the search for an understanding<br />

<strong>of</strong> the complex phenomena in solution chemistry. Indeed, the choice <strong>of</strong> the right<br />

solvent for a particular application is an everyday decision for the chemist: which solvent<br />

should be the best to dissolve certain products, and what solvent should lead to increased reaction<br />

yields and/or rates <strong>of</strong> a reaction?<br />

In the course <strong>of</strong> time, however, a rather sophisticated scheme has developed <strong>of</strong> quantitative<br />

treatments <strong>of</strong> solute-solvent interactions in the framework <strong>of</strong> LSERs. 198 The individual<br />

parameters employed were imagined to correspond to a particular solute-solvent<br />

interaction mechanism. Unfortunately, as it turned out, the various empirical polarity scales<br />

feature just different blends <strong>of</strong> fundamental intermolecular forces. As a consequence, we<br />

note at the door to the twenty-first century, alas with melancholy, that the era <strong>of</strong> combining<br />

empirical solvent parameters in multiparameter equations, in a scientific context, is beginning<br />

to fade away. As a matter <strong>of</strong> fact, solution chemistry research is increasingly being occupied<br />

by theoretical physics in terms <strong>of</strong> molecular dynamics (MD) and Monte Carlo (MC)<br />

simulations, the integral equation approach, etc.

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