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252  CHAPTER 3

                                            5
            In this expression, is the concentration  of the solute in mole fraction units, and
            is its chemical  potential in the standard state, i.e., when   assumes a standard or
            normalized value of unity


                                            when

               Since the solute particles in a solution of a nonelectrolyte are uncharged, they do
            not engage in long-range Coulombic interactions. The short-range interactions arising
            from  dipole–dipole or  dispersion forces become  significant only  when the  mean
            distance between the solute particles is small, i.e., when the concentration of the solute
            is high.  Thus, one can to  a good  approximation say  that there are no interactions
            between solute particles in dilute nonelectrolyte solutions. Hence, if Eq. (3.52) for the
            chemical potential of a solute in a nonelectrolyte solution (with noninteracting parti-
            cles) is used for the chemical potential of an ionic species i in an electrolytic solution,
            then it is tantamount to ignoring the long-range Coulombic interactions between ions.
            In an actual electrolytic solution, however, ion–ion interactions operate whether one
            ignores them or not. It is obvious therefore that measurements of the chemical potential
              of an ionic species—or, rather, measurements of any property that depends on the
            chemical potential—would reveal the error in Eq. (3.52), which is blind to ion–ion
            interactions. In other words, experiments show that even in dilute solutions,





               In this context, a frankly empirical approach was adopted by earlier workers not
            yet blessed  by  Debye and  Hückel’s  light.  Solutions that obeyed Eq.  (3.52)  were
            characterized as ideal solutions since this equation applies to systems of noninteracting
            solute particles, i.e., ideal particles. Electrolytic solutions that do not obey the equation
            were said to be nonideal. In order to use an equation of the form of Eq. (3.52) to treat
            nonideal electrolytic solutions, an empirical correction factor   was introduced by
            Lewis as a modifier of the concentration term 6







            5
            The value of  in the case of an electrolyte derives from the number of moles of ions of species i actually
            present in solution. This number need not be equal to the number of moles of i expected of dissolved
            electrolyte; if, for instance, the electrolyte is a potential one, then only a fraction of the electrolyte may
            react with the solvent to form ions, i.e., the electrolyte may be incompletely dissociated.
            6
            The standard chemical potential   has the same significance here as in Eq. (3.52) for ideal solutions. Thus,
              can be defined either as the chemical potential of an ideal solution in its standard state of   or as
            the chemical potential of a solution in its state of   and   No real solution can have
                when    so  the  standard state pertains to the same hypothetical solution as the standard state of
            an ideal solution.
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