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              Adsorption (Chemical Engineering)                                                           255

                            q/q s = bp/(1 + bp)          (2)      When the equilibrium constant b is large (highly favor-
                                                                able adsorption) the Langmuir isotherm approaches irre-
              where q s is the saturation capacity and b an equilibrium
                                                                versible or rectangular form,
              constant that is directly related to the Henry constant           ∗                ∗

              (K = bq s ). To a first approximation q s is independent of  p = 0, q = 0;  p > 0, q = q s    (3)
              temperature, so the temperature dependence of b is the  where q represents the equilibrium constant ratio in the
                                                                      ∗
              same as that of the Henry constant [Eq. (1)]. The Langmuir  adsorbed phase. This provides the basis for a very use-
              model was originally derived for localized chemisorption  ful limiting case, which is widely used in the analysis of
              on an ideal surface with no interaction between adsorbed  adsorption column dynamics since the solutions for a rect-
              molecules, but with certain approximations the same form  angular isotherm are generally relatively simple and they
              of equation can be derived for mobile physical adsorption  provide a reasonably reliable prediction of the behaviour
              at moderate coverage. Although this model provides a  that can be expected for a real system when the isotherm
              quantitatively accurate description of the isotherms for  is highly favorable.
              only a few systems, the expression shows the correct  According to the Langmuir model the heat of adsorp-
              asymptotic behavior at both high and low concentrations  tion should be independent of adsorbed-phase concentra-
              and therefore provides a useful qualitative or semiquanti-  tion, but in practice the heat of adsorption generally varies
              tative representation for many systems. A variety of more  quite significantly. For nonpolar sorbates an increase in
              sophisticated model isotherms have been developed to  the heat of sorption with coverage is generally observed,
              take account of such factors as energetic heterogeneity  and this is commonly attributed to sorbate–sorbate inter-
              and sorbate–sorbate interactions, but none of these has  action. For polar sorbates on polar adsorbents, the heat of
              proved universally applicable. From the perspective  sorption generally decreases with coverage, reflecting the
              of the overall modeling and design of adsorption systems,  dominance of energetic heterogeneity and the decreasing
              the more sophisticated models offer little advantage over  contribution of electrostatic contributions to the energy of
              the simple Langmuir model since any increase in accuracy  adsorption at higher coverage (Fig. 2).
              is generally more than offset by the additional complexity  In homologous series such as the n-paraffins heats of
              of the model and the need for more empirical parameters.  adsorption increase regularly with carbon number (Fig. 3).





































                     FIGURE 2  Variation of isosteric heat of sorption − H 0 with coverage c showing the difference in trends between
                     polar and nonpolar sorbates. (Reprinted from Ruthven, D. M. (1976). Sep. Purif. Methods 5 (2), 184, copyright Marcel
                     Dekker, Inc., New York.)
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