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                    310                                          4. Adsorption and Ion Exchange


                      Linear diffusion equations  : This is the simplest case and is used eely in the xtensi v
                                                                    y
                    related literature (Perry and Green, 1999; Hashimoto   et al  ., 1977; Coone 1990, 1993).
                                                                    ,
                    The equations are the follo wing:
                                                            q
                                        solid diffusion c : ontrol  (  )      Kq s  i  q    (4.130)
                                                            t

                                                              q
                                     fluid -film diffusion c : ontrol  (  )      KC f  C    i  (4.131)
                                                              t

                    where   K  s  and   K  f  are constants related to the local mass transfer coef The subscript icients.  f
                    “i” corresponds to the concentrations in the solid–fluid interf ace.
                                                  v
                      Differential diffusion equations  : In this case, we hae differential equations, one for
                    each diffusion step (Perry and Green, 1999; Hall   et al  ., 1966):

                                                  q
                                                      KC (  C   ) e                   (4.132)
                                                       f
                                                  t
                                                q         q 2  2   q 
                                                    K  s   +                        (4.133)
                                                t        r  2  r   r 

                                                 q    1       C 
                                                    K       R  2                    (4.134)
                                                 t  p  r  2   r    r 

                    where   K , K , and   K  f  are constants related to the local mass   transfer   coefficients.   Eq. (4.132)
                             p
                           s
                    is for the case of fluid-film diffusion control, eq. (4.133) for solid diffusion control, and
                    eq. (4.134) for pore diffusion control.  Pore diffusion is similar to solid dif ho fusion; it,  w-
                    ever, represents the fluid diffusion in pores and is considered to be an intermediate dif fu-
                    sion step, between fluid-film and solid diffusion. For the case of fluid-film dif the fusion,
                     we
                     ,
                    equation is the same as the LDF equation. Ho here, the equilibrium concentration
                     er
                     v
                    ( C ) is used in place of the interface concentration (  C ) to illustrate one significant point. i
                      e
                    These concentrations are equal only in the case of solid dif fusion as the controlling mech-
                    anism; otherwise they are different. For the case of differential diffusion equations, only
                    arithmetic solutions are possible and will not be presented in this book.
                    Equilibrium  The physical process (reaction) of adsorption or ion exchange is considered
                    to be so fast relative to diffusion steps that in and near the solid particles, a local equilibrium
                    exists. Then, the so-called adsorption isotherm of the form   q = f  ( C ) relates the stationary e
                    and mobile-phase concentrations at equilibrium.  The surface equilibrium relationship
                    between the solute in solution and on the solid surface can be described by simple analytical
                    equations (see Section 4.1.4). The material balance, rate, and equilibrium equations should
                    be solved simultaneously using the appropriate initial and boundary conditions. This system
                    consists of four equations and four unknown parameters (  C , q , q , and   C ). e
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