Page 245 - Adsorption Technology & Design, Elsevier (1998)
P. 245

222  Selected  adsorption  processes



               OL-~z2  --  U-~Z  +   u~dq" dZ  -  0                     (7.14)

            where e is the bed voidage, c and q are fluid and solid phase concentrations
            (each on the basis of moles per unit mass) at a point z in the column, u~ and u
            are  the  solid  and  interstitial  fluid  flow rates  and  DL is the  axial  dispersion
            coefficient.
              Assuming  the  rate  of adsorption  dq/dt  (equivalent  to -  u~ dq/dz)  can be
            represented by a linear driving force k (q* -q)  and that a linear equilibrium
            relationship q*  -  Kc  holds, the defining equation becomes

               DL-S-~_ 2  --  u--  --   k(Kc-q)  =  0                   (7.15)
                 dz     dz
            A steady state material balance between a plane z in the column and the inlet
            yields

               (1 -  e)  u~  (q  -  qo)  -  eu  (c  -  co)             (7.16)
            Substitution  of  this  mass  balance  into  the  differential  equation  for  the
            column  and  application  of the  usual  Dankwerts  boundary condition  at the
            column  fluid entrance  (z  -  0) and zero change  of concentration  flux at the
            column  exit  (z  =  L)  leads  to a formal  solution  for the concentration  ratio.
            When plug flow prevails and mass transfer resistance is small, CL/CO is given
            by
                        /
               C....~L
                 =  ~1  ~  (1-qo/Kco)ye St(l-r)  + yqo/Kco-1  I         (7.17)
               co   ?'- 1
                                                       J
            where  the  Stanton  number  St  -  kL/u  and  y  -  (1 -e)  Kudeu.  For  a  four-
            column countercurrent  adsorptive  fractionating  system there  are four such
            equations. In conjunction with four mass balances over each of the four beds
            and  two  additional  mass  balances  at  the  feed  point  and  over  the  fluid
            recirculating  stream,  ten  equations  define  the  total  system  enabling  ten
            unknown fluid and adsorbent  concentrations  to be found.  Given values for
            the Peclet  and Stanton  numbers  (Pe  and St),  the two equilibrium  constants
            KA and KB, the  bed voidage e and the dispersion  coefficient DL, any given
            adsorptive fractionation of a binary feed may be completely described.
              As an alternative to the continuous countercurrent model an equilibrium
            stage model of the adsorptive fractionation system exists (Ching et al.  1985).
            In effect the concentration  ratio CL/Co for each column is represented by the
            well-known equation (Kremser 1930, Souders and Brown 1932):
                           ~,n+l
                CO-  CL        -- ~'
                       =                                                (7.18)
               co-  cL/K   yn§  _  1
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