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230    CHAPTER 3


           3.3. THE DEBYE–HÜCKEL (OR ION-CLOUD) THEORY OF ION–ION
                INTERACTIONS

           3.3.1. A Strategy for a Quantitative Understanding of Ion–Ion
                  Interactions

               The first  task in  thinking in  detail about  ion–ion  interactions  is to  evolve a
                                             1
           quantitative measure of these interactions.   One approach is to follow a procedure
           similar to that used in the discussion of ion–solvent interactions (Section 2.4). Thus,
           one can consider an  initial state  in  which ion–ion  interactions do not  exist (are
           “switched off”) and a final state in which the interactions are in play (are “switched
           on”). Then, the free-energy change in going from the initial state to the final state can
           be considered the free energy   of ion–ion interactions (Fig.  3.3).
               The final  state is  obvious;  it is  ions  in solution. The  initial  state is  not so
           straightforward; one  cannot  take ions in  vacuum,  because  then there  will be
           ion–solvent interactions when these ions enter the solvent. The following approach is
           therefore adopted. One conceives of a hypothetical situation in which the ions are there
           in solution but  are  nevertheless not  interacting. Now, if  ion–ion  interactions are
           assumed to be electrostatic in origin, then the imaginary initial state of noninteracting
           ions implies an assembly of discharged ions.
               Thus, the process of going from an initial state of noninteracting ions to a final
           state of ion–ion interactions is equivalent to taking an assembly of discharged ions,
           charging them up, and setting the electrostatic charging work equal to the free energy
                 of ion–ion interactions (Fig. 3.4).
               One point about the  above procedure  should be  borne in  mind.  Since, in  the
           charging process, both the positively charged and negatively charged ionic species are
           charged up, one  obtains a  free-energy change  that  involves all the  ionic  species


           1
            The question of how one obtains an experimental measure of ion–ion interactions is discussed in Section
            3.4.









                            Fig. 3.3. The free energy   of ion–ion
                            interactions is  the  free-energy change in
                            going from a hypothetical electrolytic solu-
                            tion, in which  ion-ion  interactions do  not
                            operate, to a real solution, in which these
                            interactions do operate.
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