Page 205 - Bird R.B. Transport phenomena
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§6.4  Friction Factors for  Packed Columns  189
                 banks, flow near baffles,  and near flow around rotating disks.  These and many more are
                 summarized  in various  reference  works. 1  One complex  system  of  considerable  interest
                 in chemical engineering  is the packed  column, widely used  for  catalytic reactors and  for
                 separation  processes.
                     There have  been two  main approaches  for  developing  friction  factor  expressions  for
                 packed  columns. In one method the packed  column is visualized  as  a bundle  of  tangled
                 tubes  of  weird  cross  section; the theory  is  then developed  by  applying  the previous  re-
                 sults  for single straight  tubes  to the collection  of crooked tubes. In the second method the
                 packed column is regarded  as a collection of submerged  objects, and the pressure drop is
                 obtained  by  summing  up  the  resistances  of  the submerged  particles.  2  The tube  bundle
                 theories have been somewhat  more successful,  and we  discuss  them here. Figure  6.4-1 (я)
                 depicts a packed column, and Fig. 6.4-1 (b) illustrates  the tube bundle model.
                     A  variety  of  materials  may  be  used  for  the packing  in  columns: spheres,  cylinders,
                 Berl saddles, and  so on. It is assumed  throughout the following  discussion  that the pack-
                 ing  is statistically  uniform, so that there is no "channeling"  (in actual practice, channeling
                 frequently  occurs, and  then the development  given here does  not apply).  It is  further  as-
                 sumed  that the diameter  of the packing particles  is small  in comparison to the diameter of
                 the column in which the packing  is contained, and that the column diameter is  uniform.
                     We  define  the friction  factor  for  the packed column analogously  to Eq. 6.1-4:

                                                4
                                                  U                                   (6.4-1)
                 in  which  L is  the length  of  the packed  column, D p  is  the effective  particle diameter (de-
                 fined  presently), and  v  is  the superficial velocity; this  is  the volume  flow  rate divided  by
                                    0
                 the empty column cross  section, v 0  = zv/pS.
                     The pressure  drop through  a representative  tube in the tube bundle model is  given
                 by  Eq. 6.2-17

                                                                                      (6.4-2)



                  i  *
                  I

                  ЦЦ
                  1









                                         Fig. 6.4-1.  (a) A cylindrical  tube packed with  spheres;
                                 (b)     (b) a "tube bundle" model for  the packed column in (a).



                      P. C. Carman, Flow of Gases through Porous Media, Butterworths, London (1956); ]. G. Richardson,
                     1
                 Section  16 in Handbook of Fluid Dynamics  (V.  L. Streeter, ed.), McGraw-Hill, New York  (1961); M.  Kaviany,
                 Chapter  21 in The Handbook of Fluid Dynamics  (R. W. Johnson, ed.), CRC Press, Boca Raton, Fla. (1998).
                      W.  E. Ranz, Chem.  Eng. Prog., 48, 274-253  (1952); H. C. Brinkman, Appl. Sci. Research., Al,  27-34,
                     2
                 81-86, 333-346  (1949). Henri Coenraad Brinkman (1908-1961)  did research on viscous  dissipation
                 heating, flow in porous media, and plasma  physics; he taught at the University  of Bandung, Indonesia,
                 from  1949 to  1954, where he wrote The Application of Spinor Invariants to Atomic Physics.
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