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48    FUNDAMENTALS OF THE ADSORPTION THEORY

           where e s is the (molar) adsorption potential of the solute, e l the adsorption
           potential of the solvent, e sl the adsorption potential of the solute from solu-
                         the respective molar volumes of the solute and solvent, C s the
           tion, V s  and  V l
           solute solubility in the solvent, and C e the solute concentration in the solvent
           at equilibrium. Equation (4.12) may be further converted to give

                           e sl V =  e s V - e l V = ( RT  s V ) ( C s C )  (4.13)
                                                       ln
                                             l
                                      s
                                                              e
                               s
                                                                   ) is simply the
           As seen, the net adsorption potential density of the solute (e sl /V s
                                                                   ) and solvent
           difference between the potential densities of pure solute (e s /V s
                ). Thus one may in principle predict the adsorption of a partially mis-
           (e l /V l
           cible solute from solution from established or estimated correlation curves
           of the pure solute and solvent. Equation (4.13) has been found most success-
           ful for partially miscible liquid solutes in solution, in which the effective
                                               ) is practically the same as the molar
           molar volume of the liquid adsorbate (V s
           volume of the pure liquid. For solid solutes, the effective adsorbate molar
           volume may well exceed that of the pure substance, because packing of the
           condensed solid crystallite into fine-pore adsorption spaces may be hindered
           significantly by crystalline structure; therefore, for solid solutes, adjustment of
           molar volumes for packing efficiency is often required. Manes (1998) extended
           the Polanyi theory to a wide range of vapor and solution systems, including
           single and multiple vapors and solutes that are either completely or partially
           miscible to each other.
              In adsorption from solution, the net heat of adsorption for a partially mis-
           cible solute (e sl ) is usually smaller than that of its single vapor-phase adsorp-
           tion (e s ) because of the energy required to displace the solvent, as depicted by
           Eq. (4.12). In such systems (i.e., where the solute separates out as a liquid
           or a solid phase in adsorption space), the total molar heat of adsorption is
                                    is the molar heat of solution of the solute. One
           -(e sl +DH sol ), where DH sol
                                                                for solid solutes
           may recall from the discussion in Chapter 3 that the DH sol
                                                   ).
           includes the associated heats of fusion (DH fus

           4.6 SURFACE AREAS OF SOLIDS

           The surface area of a solid (adsorbent) plays a fundamental role in the
           physical adsorption of vapors. The BET method with appropriate adsorbate
           gases has become a universal method for determining the solid surface area.
           Suitable vapor adsorbates must be chemically inert, not subject to molecular
           sieving by the solid pore, and confined only to the exterior of the solid (i.e.,
           no vapor penetration into the interior network). The use of an inert vapor as
           the adsorbate is to eliminate any specific interaction (or reaction) with either
           solid surface or its interior network. Prevention of molecular sieving is ac-
           complished by the use of small adsorbates. Measurement at low temperature
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