Page 658 - Bird R.B. Transport phenomena
P. 658

638  Chapter 20  Concentration Distributions with  More Than One Independent Variable


                               (ii)  that the tangential  fluid  velocity  relative  to the interface  is negligible within  the
                                   concentration  boundary  layer.  (This  approximation  is  satisfactory  for
                                   fluid-fluid  systems  free  of  surfactants,  when  the  interfacial  drag  is  not  too
                                   large.)
                               (iii)  that the concentration boundary  layer  along  each interface  is thin relative  to the
                                   local radii  of  interfacial  curvature.
                               (iv)  that the concentration boundary  layers  on nonadjacent  interfacial  elements  do
                                   not  overlap.

                            Each  of  these  approximations  is  asymptotically  valid  for  small  ЯЬ  in  nonrecirculating
                                                                                    АВ
                            flows  with  nonrigid  interfaces  and nonzero Da) /Dt—that  is, with  time-dependent con-
                                                                    A
                            centration  as  viewed  by  an  observer  moving  with  the  fluid.  The systems  considered  in
                            part  (a) of  §20.3 are thus included, because they are time-dependent for  such an  observer
                            (though steady  for  a stationary one).
                               Interfacially  embedded  coordinates  are  used  in  this  discussion,  with  a  piecewise
                            smooth  interfacial  grid  as  in Fig. 20.4-1. Each interfacial  element in the system  is perma-
                                                                                         r
                            nently  labeled  with  surface  coordinates  (u, w), and  its  position  vector  is (u,  w,  t). Each
                                                                                          s
                            point in a boundary  layer  is identified  by  its distance у  from  the nearest interfacial  point,
                            together  with  the  surface  coordinates  {u, w)  of  that  point.  The  instantaneous  position
                            vector  of  each point (u, w, y) at time t is then
                                                  r(w, w,  y,  t)  = {u,  w,  t)  + yn(w, w,  t)  (20.4-2)
                                                             r
                                                              s
                            relative  to  a  stationary  origin,  as  illustrated  in  Fig.  20.4-2.  The function (w, w,  t) gives
                                                                                         r
                                                                                          s
                            the  trajectory  of  each  interfacial  point  (u, w,  0), and  the associated  function  п(м, w,  t) =
                            (d/dy)r  gives the instantaneous normal vector  from  each surface  element toward  its posi-
                            tive  side.  These  functions  are  computable  from  fluid  mechanics  for  simple  flows,  and
                            provide  a framework  for  analyzing  experiments  in complex  flows.


                                      Dropl
                                                                     Composite
                                                                       drop














                                                                                  14
                                                                                15







                            Fig.  20.4-1.  Schematic illustration  of embedded  coordinates in a simple coa-
                            lescence process. W.E. Stewart, J.B. Angelo, and E.N. Lightfoot,  AIChE Jour-
                            nal, 14,458^67 (1968).
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