Page 193 - Adsorption Technology & Design, Elsevier (1998)
P. 193

Design procedures  179


            and  0.5,  respectively.  Equation  (6.71)  can  be  written  in  non-dimensional
            form as follows:
               1     DL    ?'IDM        ?'le
                                                                        (6.72)
                  "-   :  =      +~2   =   ~  +  ~  '  2
              Pe'   udp     ud v       ReSc
            The coefficient ?'1 is dependent on bed voidage as follows:

              y~ = 0.45 + 0.55e                                        (6.73)
            The coefficient )'2 is dependent upon flow characteristics as follows:
                             1
              ~'2  -"   ............
                                p ,t'm /                                (6.74)
                     ee'|   1+        ]

            At high Reynolds numbers the asymptotic value of the Peclet number takes
            the  value  of  2  for  relatively  large  particles,  i.e.  d o >  0.3 cm.  For  smaller
            particles,  i.e.  dp  <  0.3 cm,  experimental  data  show  much  smaller  limiting
            Peclet numbers, given approximately as follows:
              Pe'oo =  1.68do                                          (6.75)
            This  behaviour  is believed  to  be  due  to  the  tendency  of small particles  to
            form clusters which act effectively as single particles. Thus the advantage of
            reducing pore  diffusional  resistances  by using small particles could well be
            offset to some extent by an increase in axial dispersion.
              The variations of Peclet number with Reynolds number for gas and liquid
            phase systems are compared in Figure 6.12. At high Re, the asymptotic value
            of Pe'  = 2 is reached for liquids, but at lower values of Re, the axial dispersion
            is  greater  than  that  for  gases.  The  increased  dispersion  with  liquids  is
            believed  to  be  due  to  the  effect  of  greater  liquid  hold-up  in  the  laminar
            boundary  layer surrounding  particles,  together with small random fluctua-
            tions in the flow (Ruthven 1984).
              If adsorption  is fast  and  strong  then  the  concentration  profile  through  a
           particle  may become  asymmetric. This  can  lead  to  a significant  additional
           contribution to axial dispersion for gases at low Re. The effect is likely to be
           most  significant  when  most  of the  adsorption  occurs  at  the  outside  of the
           particle, as would occur in the initial stages of uptake in a mass transfer zone.
           Equation  (6.76)  has  been  suggested  for  a  rectangular  isotherm  as  an
           alternative to equation  (6.72). In this case ?'1 is typically 50, compared with
           the value of 0.7 for non-porous particles:
               1     20     1
                  =      +  -                                          (6.76)
              Pe'   ReSc    2
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