Page 74 - Adsorption Technology & Design, Elsevier (1998)
P. 74

Rates of adsorption of gases and vapours by porous media  71


            coefficient. The classical kinetic theory of gases (Present  1958) reveals that
            the diffusion of a gas is determined by the mean velocity of molecules and
            the  distance  they  travel  before  they  collide  either  with  another  molecule
            (molecular or Maxwellian diffusion)  or with the wall of a narrow capillary
            (Knudsen  diffusion).  When  the  mean  free  path  A,  is  smaller  than  the
            dimensions  of  a  containing  conduit,  unconstrained  molecular  transport
            occurs; if, on the other hand, the mean free path is greater than the radius of
            a narrow channel  (for example, pores within a porous solid) through which
            molecules are travelling, then Knudsen diffusion obtains.
              Pore  size  distribution  data  obtained  from  gas  desorption  (Barret  et al.
            1951)  and  mercury porisimetry experiments  together with  a  knowledge  of
            adsorbate molecular size thus enables the mode of diffusive transport to be
            ascertained.  It should be noted that both molecular and Knudsen diffusion
            may occur in the  same porous  medium when the porous  medium contains
            both  macropores  and  micropores  (revealed  from  an  analysis of a  bimodal
            pore  size  distribution  curve).  Unconstrained  molecular  diffusion,  DM, and
            Knudsen  diffusion,  DK,  coefficients  are  subsequently  calculated  from
            formulae  derived  from  transport  properties  of fluids  (gaseous  and  liquid)
            and  the  kinetic theory  of gases. The  molecular diffusivity for  a  binary gas
            mixture  of  A  and  B  is  evaluated  from  the  Chapman-Enskog  theory
            (Chapman and Cowling 1951) equation
                      (1.858 x  10-7)T 3/2 ((lIMA) + (lIMB)) t/2
               DM =                 pO.2AB I                             (4.9)

            in  which  DM  is  expressed  in  units  m 2 s -1,  MA  and  MB  are  the  molecular
            masses  of  the  species  A  and  B,  Crab is  a  constant  in  the  Lennard-Jones
            potential  function  and  I  is  the  collision  integral  (see  Section  3.1).  The
            Knudsen  diffusivity,  in  contrast  to  the  bulk  diffusion  coefficient,  is
            calculated from the kinetic theory formula
                     2      2  (8Re, T] '/2
               DK =  -~- re =  --3 r  trM  ]                            (4.10)

            where  r  is  the  pore  radius,  C" the  average  molecular  velocity  and  M  the
            molecular  mass. When  the  mean  free  path  and  pore  radius  are  of a  similar
            magnitude the resultant diffusivity is calculated in proportion to the individual
            bulk and Knudsen  diffusivities. According to Pollard and Present  (1948), for
            adsorption  and  desorption,  equimolar  counterdiffusion  occurs  and  so  the
            resultant resistance to diffusion is the sum of the resistances to bulk diffusion
            and Knudsen diffusion. Thus the net diffusion coefficient D is given by

               I/D = (I/DM) + (I/DK)                                    (4.11)
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