Page 162 - Adsorption Technology & Design, Elsevier (1998)
P. 162

150  Design procedures


            complex model should be sufficiently general to provide a good description
            in most systems.


            Isothermal, equilibrium controlled systems
            The  simplest  packed  bed  design  arises  with  a  single  dilute  adsorbate  in  a
            carrier fluid when it can be assumed that the process is isothermal, that there
            is  plug  flow,  and  that  there  are  no  mass  transfer  resistances.  In  such  a
            situation,  instantaneous  equilibrium  exists  at  all  points  in  the  system.
            Without the axial dispersion term and taking the velocity outside the partial
            differential term for the convective flow, equation (6.19) is simplified to:

                 ac    Of      (~)Oq
                                         -  0                          (6.22)
              U  ~   +    +  pp
                 Oz    Ot             Ot
            The  full  derivation  of this  equation  is provided  elsewhere  (Ruthven  1984,
            Coulson  et al.  1991).  In  general  terms  the  equilibrium  isotherm  may  be
            described as follows:
              q* =f(c)                                                 (6.23)

            As  shown by  Coulson et al. (1991) the velocity with which a point of given
            fluid concentration propagates through the bed is given as follows:



                                                                        (6.24)
               (O )c         u
                            (1_~) dq*
                      1 + pp      dc

            For a given point on the isotherm the speed of that point in the MTZ is seen
            to  be  constant  and  to  be  dependent  on  the  bulk  fluid  velocity,  the  bed
            voidage and the slope of the isotherm at the concentration in question. With
            an  unfavourable  isotherm  the  gradient  dq*/dc increases  as  the  fluid
            concentration c increases. Hence, using equation (6.24) it can be seen that a
            point  of high  concentration  in  the  MTZ  will move  at  a  slower  rate  than  a
            point of low concentration.  Thus the MTZ will broaden out as it progresses
            through  the  bed.  On  the  other  hand,  for  a  favourable  isotherm  (such  as  a
            Type I isotherm described in Section 3.2), a point of high concentration, i.e.
            one near the trailing edge of the MTZ, will travel faster through the column
            and  catch up with points  of lower concentration  at the  leading edge of the
            MTZ.  In  theory  it  would  seem  from  equation  (6.24)  that  points  of  high
            concentration  could  overtake  points  of low  concentration  in  the  MTZ.  In
            practice  however,  the  effects  of  axial  dispersion  (omitted  from  equation
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