Page 71 - Adsorption Technology & Design, Elsevier (1998)
P. 71

68  Rates of adsorption of gases and vapours by porous media


            4.2    TRANSPORT PROCESSES IN POROUS SOLIDS

            We  consider each of the possible resistances to rapid adsorption which are
            listed  above  and  examine  their  significance  and  magnitude.  Interparticle
            (external  to  particles)  transport  resistance  occurs  in  series  with  the
            intraparticle  (within particles) transport resistances, enumerated 2, 3 and 4,
            which, if each were present, would be in parallel.

                   Interparticle mass and heat transport
            4.2.1
            Rates  at which mass and heat are transported between  a flowing bulk fluid
            phase  and  the  exterior  surface  of the  adsorbent  particles  are  limited  by  a
            relatively  thin  layer  of comparatively  stagnant  fluid  immediately  adjacent
            to, and completely enveloping, each of the solid particles. Such layers can be
            thought  of  as  films  of stagnant  fluid  or,  as  described  by  a  more  elaborate
            theory, in terms of so-called mass and heat transfer boundary layers. For the
            purposes  of  application  to  adsorption  either  of  these  concepts  can  be
            accommodated  by  defining  the  mass  or  heat  flux from fluid  to  solid  as the
            product  of a lumped coefficient and  a linear driving force. These mass and
            heat transfer coefficients for the respective interparticle processes subsume
            the  thickness  of  the  film  or  boundary  layer  and  relevant  fluid  properties
            while  the  driving  force  is  simply  the  difference  in  concentration  (mass
            transport)  or temperature  (heat transport)  between bulk fluid and exterior
            surface  of the  particle.  The  rate  of mass  transport  of a  specific component
            from bulk fluid to the exterior surface of a particle, expressed as the number
            of moles  of the  component  transferred  per unit  adsorbent  bed volume  per
            unit time, is
               R  = kap (Cg- c)                                          (4.2)
            where k is the mass transfer coefficient and a is the exterior surface area of a
            solid particle  per  unit volume.  The  dimensions  of k  are  thus  LT -1 or, in SI
            units, m s -1. An analogous equation describes the rate of heat transfer
               Rh = hap ( T-  Tg)                                        (4.3)

            where  T is the  temperature  at the exterior surface of the solid,  Tg the bulk
            fluid temperature  and h is the heat transfer coefficient which will have units
            (SI system) W m -2 K -1 if the rate of heat transfer is based on unit volume of
            adsorbent  bed.  Whereas  equation  (4.2)  indicates  mass  transfer  during
            adsorption  from  bulk  fluid  to  surface  (Cg  >  c),  because  adsorption  is
            exothermic  (see  Section  3.1)  heat  is released  from within  the  pellet  and  is
            transferred from the particle exterior surface to the bulk fluid (T >  Tg).
              Boundary  layer  theory  predicts  different  values  of  coefficients  for  the
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