1.22.10: Volume: Aqueous Binary Liquid Mixtures

A Notebook for Topics in Thermodynamics of Solutions and Liquid Mixtures · LibreTexts

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    1.22.10: Volume: Aqueous Binary Liquid Mixtures

    For binary aqueous mixtures (at ambient pressure and fixed temperature) there are two interesting reference points.

    1. The molar volume of the pure liquid component 2, \(\mathrm{V}_{2}^{*}(\lambda)\).

    In the latter case we imagine that each molecule of liquid 2 is surrounded by an infinite expanse of water. With gradual increase in \(\mathrm{x}_{2}\), so (on average) the molecules of liquid 2 move closer together.

    Typically Aqueous Mixtures

    For these systems \(\left[\mathrm{V}_{2}^{\infty}(\operatorname{mix})-\mathrm{V}_{2}^{*}(\lambda)\right]\) is negative. But this pattern is not unique to aqueous systems. The unique feature is the decrease in \(\left[\mathrm{V}_{2}(\operatorname{mix})-\mathrm{V}_{2}^{*}(\lambda)\right]\) with increase in \(\mathrm{x}_{2}\) at low \(\mathrm{x}_{2}\) [1]. In fact with increase in hydrophobicity of chemical substance 2, the decrease is more striking and the minimum in \(\left[\mathrm{V}_{2}(\operatorname{mix})-\mathrm{V}_{2}^{*}(\lambda)\right]\) occurs at lower \(\mathrm{x}_{2}\). At mole fractions beyond \(\mathrm{x}_{2}\left[\mathrm{~V}_{2}(\mathrm{mix})-\mathrm{V}_{2}^{*}(\lambda)\right]\) increases with increase in \(\mathrm{x}_{2}\). Many explanations have been offered for this complicated pattern. The following is one explanation.

    The negative \(\left[\mathrm{V}_{2}^{\infty}(\operatorname{mix})-\mathrm{V}_{2}^{*}(\lambda)\right]\) is accounted for in terms of a liquid clathrate in which part of the hydrophobic group ‘occupies’ a guest site in the liquid water ‘lattice’. The decrease in \(\left[\mathrm{V}_{2}(\operatorname{mix})-\mathrm{V}_{2}^{*}(\lambda)\right]\) is accounted for in terms of an increasing tendency towards a liquid clathrate hydrate structure. With increase in \(\mathrm{x}_{2}\) there comes a point where there is insufficient water to construct the liquid clathrate host. Hence \(\left[\mathrm{V}_{2}(\operatorname{mix})-\mathrm{V}_{2}^{*}(\lambda)\right]\) increases [2,3].

    Typically Non-Aqueous Systems

    Although \(\left[\mathrm{V}_{2}^{\infty}(\operatorname{mix})-\mathrm{V}_{2}^{*}(\lambda)\right]\) is negative no minimum is observed in \(\left[\mathrm{V}_{2}(\operatorname{mix})-\mathrm{V}_{2}^{*}(\lambda)\right]\).

    Footnotes

    [1] See for example; fluoroalcohols(aq); C. H. Rochester and J. R. Symonds, J. Fluorine Chem.,1974,4,141.

    [2] F. Franks, Ann. N. Y. Acad. Sci.,1955,125,277.

    [3] For many binary aqueous mixtures the patterns in volume related properties often identify transition points at ‘structurally interesting compositions’; G. Roux, D. Roberts, G. Perron and J. E. Desnoyers, J. Solution Chem.,1980,9,629.


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