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262 CHAPTER 3





           where   is  the  mole fraction of the solvent. One allows for the nonideal behavior of
           the solvent in respect to its vapor pressure by writing




           As              Thus, the “standard state” is the pure solvent.
               At this point, one calls into play the Gibbs–Duhem equation of thermodynamics,
           according to which 10





           Or, for a two-component system (solvent and electrolyte)




           where the subscript  1  represents the solvent and the subscript  2  represents the
           electrolyte solute.
               It follows  from       ln  ,  that






           or







               Thus, if one measures a number of values of the vapor pressure of the solvent
             at a corresponding number of solute concentrations,   (to which there are matching
           solvent concentrations   one can plot the ln   values against the    ratios. Then
           the area of that plot will give ln    the   being the solute activity corresponding to
           the limit of the integral at   (this  being  the measured solvent activity for a solution
           containing a solute, the activity of which is
               The left-hand side of Eq. (3.98) came from


           10
            Any initial impression that there is something unreasonable about the Gibbs–Duhem equation should be
            instantly quelled. It merely tells one that (for a two-component system) when an increase in    occurs,
            it causes a decrease in   of equal magnitude, a typically powerful and general result of thermody-
            namic reasoning.
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