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ION–ION INTERACTIONS 295

           more than half of the water in the solution is associated with the ions, and a sharp
           increase of activity coefficient, somewhat of a doubling in fact, would be expected to
           express the increase in effective concentration of the ions. To what extent can this
          rough sketch be turned into a quantitative model?

           3.6.2. Quantitative Theory of the Activity of an Electrolyte as a
                 Function of the Hydration Number
              The basic thought here has to be similar to that which lay beneath the theory of
          electrostatic interactions: to calculate the work done in going from a state in which the
           ions are too far apart to feel any interionic attraction to the state at a finite concentration
           c at which part of the ions’ behavior is due to this. This work was then [Eq. (3.59)]
          placed equal to RT ln f, where f is the activity coefficient, which was thereby calculated.
              When one realizes that a reversal of the direction in which the activity coefficient
           varies with concentration has to be explained by taking into account the removal of
           some of the  solvent from effectively  partaking  in the ionic  solution’s activity, the
          philosophy behind the calculation of this effect on the activity coefficient becomes
          clear. One must calculate the work done in the changes caused by solvent removal and
           add this  to the work done in  building up the  ionic  atmosphere.  What, then,  is the
          contribution due to these water-removing processes? [Note that ions are hydrated at
          all times in which they are in the solution. One is not going to calculate the heat of
          hydration; that was done in Chapter 2. Here, the task is to calculate the work done as
          a consequence of the fact that when water molecules enter the solvation sheath, they
          are, so to speak, no longer operating as far as the solvent is concerned. It is to be an
                     type of calculation.]
              As a device for the calculation, let it be assumed that the interionic attraction is
          switched off. (Reasons for employing this artifice will be given.) Thus, there are two
          kinds of work that must be taken into account.

              1.  The         kind of work done when there is a change in concentration
                 of the free solvent water caused by introducing ions of a certain concentration
                 into the solution.
              2. The          kind of work done when there is a corresponding change in
                concentration of the ions due to the removal of the water to their sheaths.
              The work done for process 1 is easy to calculate. Before the ions have been added,
          the concentration of the water is unaffected by anything; it is the concentration of pure
          water and its activity, the activity of a pure substance, can be regarded as unity. After
          the ions are there, the activity of the water is, say,  Then, the work when the activity
          of the water goes from 1 to   is RT ln
              However, one wishes to know the change of activity caused in the electrolyte by
          this change of activity of the water. Furthermore, the calculation must be reduced to
          that for 1 mole of electrolyte. Let the sum of the moles of water in the primary sheath
          per liter of solution for both ions of the imagined 1:1  electrolyte be    (for  1-molar
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