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56  Chapter 2  Shell Momentum  Balances and Velocity Distributions in Laminar Flow
                               (iv)  The force exerted by  the fluid  on  the solid surfaces is  obtained  by  summing  the
                                   forces acting on the inner and  outer cylinders, as  follows:
                                                R  =

                                                                                               (2.4-18)
                           The reader should explain the choice of signs in front  of the shear stresses above and  also
                           give an interpretation  of the final  result.
                               The equations derived  above are valid  only  for laminar  flow. The  laminar-turbulent
                           transition  occurs  in the neighborhood  of  Re  =  2000, with  the Reynolds number  defined
                           as  Re  =  2R(1  -  K)(V Z) P//X.

      §2.5  FLOW OF TWO ADJACENT          IMMISCIBLE FLUIDS     1
                           Thus  far we have considered  flow situations with  solid-fluid  and  liquid-gas  boundaries.
                           We now give one example of a flow problem with a liquid-liquid  interface  (see Fig. 2.5-1).
                               Two immiscible, incompressible liquids are flowing  in the z direction  in a horizontal
                           thin  slit  of  length  L and  width  W under  the  influence  of  a horizontal  pressure  gradient
                           (Po ~  Pi)/L.  The fluid  flow rates are adjusted  so that the slit is half  filled  with  fluid  I (the
                           more dense phase) and  half  filled  with fluid  II (the less dense phase). The fluids are  flow-
                           ing  sufficiently  slowly  that  no instabilities  occur—that  is, that  the  interface  remains  ex-
                           actly planar.  It is desired  to find  the momentum-flux  and  velocity distributions.
                               A differential  momentum balance leads to the following  differential  equation  for  the
                           momentum   flux:
                                                              _  po -
                                                           dr xz     p L
                                                                                                (2.5-1)
                                                           dx      L
                           This  equation  is obtained  for  both  phase  I and  phase  II. Integration  of  Eq.  2.5-1  for  the
                           two regions gives

                                                                                                (2.5-2)

                                                                                                (2.5-3)



                                   Velocity                                     =  (Pn-Pi)b [M
                                  distribution -
                                                 Less dense,  t
                                                 less viscous I
                                                   fluid  b  Plane of zero shear stress
                                                Interface -

                                            i /  More dense,                      x  _ 1
                                               more viscous                       b  "  2
                                                  fluid

                                                                     v  Shear stress
                                                                      or momentum-
                                               2L
                                                                     flux  distribution
                            Fig. 2.5-1  Flow of two immiscible fluids between a pair  of horizontal plates under
                            the influence  of a pressure gradient.

                               1
                                 The adjacent  flow  of gases and liquids in conduits has been reviewed by A. E. Dukler and M.
                            Wicks, III, in Chapter 8 of Modern Chemical Engineering, Vol. 1, "Physical Operations/' A. Acrivos (ed.),
                            Reinhold, New York (1963).
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