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32    INTERPHASE PARTITION EQUATIONS

           ties associated with the water phase. By Eq. 3.5 and omitting the subscript i,
           one finds that

                                                    V       V             (3.6)
                                        w
                           logK sw = logg* - logg* s + log * w - log * s
           If the solute has a low solubility in water, one obtains from Eqs. (2.2), (2.5),
           and (3.3) the molar solubility of the solute in water (S w) as
                               l ()
                              S w = 1 g  w V w  for liquid solutes        (3.7)

           and
                                s ()
                                    s
                              S w =  a g w V w  for solid solutes         (3.8)
                                                                          o
                                                                   s
                  s
                                                                        s
           where a is the activity of the pure solid substance at T (i.e., a = P /P ) as
           defined by Eq. (2.4). From Eqs. (3.7) and (3.8), the supercooled liquid solu-
                                                          (s)
                          (l)
           bility of a solid, S w , is related to the solid solubility S w as follows:
                                   l ( )
                                                s ()
                                                   o
                                                       s
                                           s
                                 S w =  S w s ()  a =  S w ( P P )        (3.9)
           Substituting Eq. (3.7) into (3.6), one obtains for liquid (or supercooled-liquid)
           solutes,
                                       *      *          *        *
                  logK sw =-  logS w - logV s -  logg  s -  log(g w g w +  V w  )  (3.10)
                                                           ) log(V w
           In Eq. (3.10), the S w value for a solid solute is that of the supercooled liquid,
           as determined according to Eq. (3.9). The melting-point effect that affects the
           solid solubility in a single phase (e.g., water) does not affect the partition
           coefficient (K sw) because the effect cancels out in solute partition between any
           two separable phases. The g w/g* w term corrects for the effect of the dissolved
           organic solvent in water on the solute water solubility. The value of g w/g* w is
           usually greater than 1 and is called the  solubility enhancement factor.In
           solvent–water systems, where the solvent has a limited solubility in water, the
           change in the molar volume of water due to solvent saturation is not substan-
           tial (i.e., V * w/V w   1). Under this condition, Eq. (3.10) is further reduced to
                                             *      *          *
                        logK sw =- logS w -  logV s -  logg s -  log(g w g  w )  (3.11)


           3.3 PARTITION BETWEEN A MACROMOLECULAR
           PHASE AND WATER

           The solute partition coefficient at dilution between an amorphous polymeric
           or macromolecular organic substance and water (K pw ) cannot be represented
           by Eq. (3.6) or (3.11). This is because the solubility of common organic solutes
           in a macromolecular phase, as expressed by Eqs. (2.13) and (2.15), is under-
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