Page 593 - Bird R.B. Transport phenomena
P. 593

Problems  573

                   Natural gas                    Fig. 18B.8.  Diffusion  of helium through pyrex  tubing.
                   containing           Pyrex  tube  The  length  of the tubing is L.
                     helium











                   (c)  Integrate this equation between  the limits r  and r  to get
                                                        1
                                                             2
                                                  _  сЯЬ АВ  (r 2 \  x B2
                                                                                      (18B.7-2)
                   What  is the limit  of this expression  when r  —»  °°?
                                                    2
            18B.8.  Method for  separating helium from  natural gas  (Fig. 18B.8).  Pyrex glass is almost imperme-
                   able  to  all  gases but  helium.  For example,  the  diffusivity  of  He through  pyrex  is  about  25
                   times the diffusivity  of H  through pyrex, hydrogen being the closest  "competitor" in the  dif-
                                       2
                   fusion  process. This fact suggests that a method for separating  helium from natural gas  could
                   be based  on the relative  diffusion  rates through  pyrex. 7
                      Suppose a natural gas mixture is contained in a pyrex  tube with dimensions shown in the
                   figure.  Obtain an expression  for  the rate at which helium will "leak"  out of  the tube, in terms
                   the  diffusivity  of  helium  through  pyrex,  the  interfacial  concentrations  of  the  helium  in the
                   pyrex, and the dimensions  of the tube.
                                  ^               )
                   Answer:

            18B.9.  Rate of  leachng (Fig. 18B.9).  In studying  the rate of  leaching  of a substance A  from  solid  par-
                   ticles by  a solvent  B, we  may postulate that the rate-controlling step is the diffusion  of A  from
                   the  particle  surface  through a stagnant  liquid  film  thickness  8 out into the main stream. The
                   molar solubility  of A  in В is c , and the concentration in the main stream is  c .
                                          A0
                                                                                A8
                   (a)  Obtain a differential  equation for c  as a function  of z by making a mass balance on A  over
                                                 A
                   a  thin slab  of  thickness  Az. Assume  that ЯЬ АВ  is constant and that A  is  only  slightly  soluble  in
                   B. Neglect the curvature  of the particle.









                     Solid
                    particle   Liquid   Main
                   containing   film    liquid
                      A                 stream
                                         of
                                       Л and В
                                                Fig. 18B.9.  Leaching  of A  by  diffusion  into a stagnant
                           2 = 0                liquid  film  of B.


                      7  Scientific American,  199, 52 (1958) describes  briefly the method developed  by К. В. McAfee  of Bell
                   Telephone  Laboratories.
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