Page 580 - Bird R.B. Transport phenomena
P. 580

560  Chapter 18  Concentration Distributions in Solids and in Laminar Flow

                           An  exactly  analogous  problem  occurred  in  Example  4.1-1,  which  was  solved  by  the
                           method  of  combination  of  variables.  It is  therefore  possible  to take  over  the solution  to
                           that problem just  by  changing the notation. The solution  is  3

                                                r,       9  f  x/V4Z AB z/v m ^
                                                                                              (18.5-15)

                           or
                                                                 =  = erfc -                  (18.5-16)
                                            440

                           In  these  expressions  "erf  x"  and  "erfc  x"  are the "error  function"  and  the "complemen-
                           tary  error function"  of  x, respectively.  They  are discussed  in §C6  and tabulated  in stan-
                           dard  reference  works. 4
                               Once the concentration profiles  are known, the local  mass  flux  at the gas-liquid  in-
                           terface may be found  as  follows:

                                                                                              (18.5-17)
                                                              dx  x=0
                           Then the total molar flow  of A  across  the surface  at x  = 0 (i.e., being  absorbed  by  a liquid
                           film  of length L and width  W) is










                                                                  TIL                         (18.5-18)
                           The  same result  is obtained by  integrating  the product v c  over  the flow cross  section
                                                                          max A
                           at z  = L (see Problem 18C.3).
                               Equation  18.5-18 shows  that  the  mass  transfer  rate  is  directly  proportional  to  the
                           square  root  of  the diffusivity  and inversely  proportional to the square  root  of  the  "expo-
                           sure time," t exp  = L/v .  This approach for  studying  gas  absorption was  apparently  first
                                             max
                           proposed by  Higbie. 5
                               The  problem  discussed  in  this  section  illustrates  the  "penetration model"  of  mass
                           transfer.  This model is discussed  further  in Chapters 20 and 22.


       EXAMPLE   18o5-l    Estimate the rate at which gas  bubbles  of A are absorbed  by  liquid  В as the gas bubbles  rise at
                                             v
                           their terminal velocity  through a clean quiescent  liquid.
      Gas  Absorption  from                   t
      Rising  Bubbles


                               3
                                The solution is worked  out in detail by the method of combination of variables  in Example 4.1-1.
                               4
                                M. Abramowitz  and I. A. Stegun, Handbook of Mathematical Functions, Dover, New York, 9th printing
                           (1973),pp.310etseq.
                               5
                                R. Higbie, Trans. AIChE, 31, 365-389 (1935). Ralph Wilmarth  Higbie (1908-1941), a graduate of the
                           University  of Michigan, provided  the basis for the "penetration model" of mass  transfer.  He worked at
                           E. I. du Pont de Nemours & Co., Inc., and also at Eagle-Picher Lead Co.; then he taught at the University
                           of Arkansas  and the University  of North Dakota.
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