Abstract
The classic thermodynamic treatments considering self-associated liquids A as multicomponent systems are unable to explain the solubilities of substances B in these liquids by effects directly related to the presence of H-bond chains. This is not the case when the hypothesis of successive equilibria between the i-mers is abandoned and replaced by a single equilibrium between bonded and free hydroxylic protons. In the new treatment presented here two combinatorial entropies are considered : that resulting from the exchange possibilities between bonded and non-bonded protons and that originating from the exchange between A and B molecules. For large values of φ A , the volume fraction of the associated liquid, it is shown that the latter combinatorial entropy is practically equal to that calculated in absence of self-association. The fraction γ of the free hydroxylic protons depends on the molar enthalpy of the hydrogen bond ΔH h and on the entropy of chain-reintegration ΔS h . The latter depends on the formal concentration F A of the associated substance and a quantitative treatment shows that dΔS h /dlnF A = R (gas constant). This conclusion is experimentally confirmed by the variation of the vapor pressure with F A in the series of the primary alcohols. The introduction of an inert substance B causes F A to decrease and enhances the lowering of the entropy of the bonded molecules with respect to the non-bonded molecules. This creates a hydrophobic effect that is at the origin of the lowering of the solubility φ B of B in A. As a consequence, lnφ B at the equilibrium is diminished by an amount equal to b A φ A V B / V A , where V B and V A are the formal molar volumes of both substances. b A is a so called “structuration factor” of the solvent A that nearly equals −1 for strongly associated solvents with single H-bond chains, like alcohols, and −2 for solvents with double chains like water. Taking for the combinatorial entropy between A and B an expression intermediate between the classic one in mole fractions and that of Flory-Huggins in volume fractions, one derives equations that predict the solubility of alkanes in water and in alcohols. Although these equations do not contain any adjustable parameter and that the experimental solubilities φ B cover several orders or magnitude, the agreement between prediction and experiment is remarkable.
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