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142 CHAPTER 2






















               The solvation numbers would be expected to be zero for sufficiently large ions.
           For these ions, the ion’s field is too weak to hold the dipoles and rises toward (but
            never equals) the coordination number as the ion’s size falls; therefore its Coulombic
           attraction upon the water molecule increases (Fig. 2.23).

           2.16.3.  A Reconsideration of the Methods for Determining the Primary
                   Hydration Numbers Presented in Section 2.15
                   34
               Most  of the methods employed to yield primary hydration numbers have already
           been presented (Section 2.15). Thus, one of the simplest methods,  which has been
           applied to organic molecules as well as ions in solution, is that originated by Passynski.
           As with most methods, it purports to give the total solvation number for the salt, but
           this should not be counted as a difficulty. More to the point is Onori’s criticism that
           the primary hydration  shell is not incompressible.  Onori has  measured  this while
           dropping Passynski’s assumption, but the solvation numbers he gets seem unreason-
           ably large and may be invalidated by his counter assumption, i.e., that solvation is
           temperature independent.
               The mobility method (Section 2.10.1) has the advantage of yielding individual
           solvation numbers directly (as long as the transport numbers are known). However,
           this positive point is offset by the fact that the viscosity term used should be the local
           viscosity near the ion, which will be less than the viscosity of the solvent, which is

           34
            Thus the entropy of solvation (Section 2.15.12) can be used to obtain hydration numbers. Knowing the
             value of   (Section 2.5.3), it is necessary only to know the entropy change of one water molecule as it
             transfers from a position in a somewhat broken-up water lattice, where it has librative (and some limited
             translatory) entropy but ends up, after having been trapped by the ion, with only vibrational entropy. The
             value assigned to this change is generally 25   of water, so that
              As a rough-and-ready estimate, this will do. However, the method is open to further development,
             particularly as to the broken-down character of water in the neighborhood of the ion and how this affects
             the value of 25   per  water  molecule.
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