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46 CHAPTER 2


               Knowing the distribution functions, g(r), as a function  of r from experiment or
           calculation from a central particle, it is possible to calculate how the water molecules
           spread out from a central particle. With knowledge of this function, it is possible to
           calculate various properties of liquid water (e.g., its compressibility), and these can
           then be compared with experimental values as a test of the calculation.

           2.4.1. How Does the Presence of an Ion Affect the Structure of
                  Neighboring Water?

               The aim here is to take a microscopic view of an ion inside a solvent. The central
           consideration is that ions orient dipoles. The spherically symmetrical electric field of
           the ion may  tear water dipoles out of the water lattice and make them point (like
           compass needles oriented toward a magnetic pole) with the appropriate charged end
           toward the central ion. Hence,  viewing the ion as  a point charge and the  solvent
           molecules as electric dipoles, one obtains a picture of ion–dipole forces as the principal
           source of ion–solvent interactions.
               Owing to the operation of these ion–dipole forces, a number of water molecules
           in the immediate vicinity of the ion (the number will be discussed later) may be trapped
           and oriented in the ionic field. Such water molecules cease to associate with the water
           molecules that remain part of the network characteristic of water (Section 2.4.3). They
           are immobilized except  insofar as  the ion  moves, in  which  case the  sheath of
           immobilized water molecules moves with the ion. The ion and its water sheath then
           become a single kinetic entity (there is more discussion of this in Section 2.4.3). Thus,
           the picture (Fig. 2.11) of a hydrated ion is one of an ion enveloped by a solvent sheath
           of oriented, immobilized water molecules.
               How about the situation far away from the ion? At a sufficient distance from the
           ion, its  influence  must  become  negligible  because the  ionic fields have  become

















                                  Fig. 2.11.  An ion envel-
                                  oped by  a  sheath of  ori-
                                  ented solvent molecules.
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