Page 606 - Bird R.B. Transport phenomena
P. 606

586  Chapter  19  Equations  of Change for Multicomponent Systems


                                 Liquid              Fig. 19.1-1.  Simultaneous diffusion,  convection, and chemi-
                                 В with              cal reaction.
                                  small
                                amounts
                                  of Л
                                 and С
                                          by  first-
                                           order
                                          reaction

                                         - Porous plug
                                          of A (slightly
                                          soluble in B)



                                 Liquid
                                   В


                           This is to be solved  with the boundary  conditions that c A  = c A0  at z = 0 and c A  = 0 at z  = oo.
                           Equation  19.1-19  is  a standard  second-order  linear  differential  equation  (Eq. C.7) for  which
                           there is a well-known method  of solution.
                                                az
                               A trial function  c A  = e  leads to two values of a, one of which violates the boundary con-
                           dition at z =  oo. The final solution is then

                                              -£  = exp[-(vT                                   (19.1-20)

                           This example  illustrates  the use  of the equation  of continuity  of A  for  setting up  a  diffusion
                           problem with convection and chemical reaction.



      519.2  SUMMARY OF THE MULTICOMPONENT
             EQUATIONS OF CHANGE
                           In the three main parts  of this book we have by stages introduced  the conservation  laws
                           known  as the equations  of change. In Chapter  3 conservation  of mass and  conservation
                           of momentum  in pure  fluids  were presented.  In Chapter  11 we added  the  conservation
                           of energy in pure fluids.  In §19.1 we added  mass conservation  equations  for  the  various
                           species  present.  We now  want  to summarize  the conservation  equations  for  multicom-
                           ponent systems.
                               We start, in Table 19.2-1, by giving the equations  of change for a mixture  of N chemical
                           species in terms  of the combined  fluxes with respect to stationary axes. The equation  num-
                           bers indicate where each equation  first appeared.  By tabulating the equations  of change in
                           this  way,  we  can  gain  an  appreciation  for  the  unity  of  the  subject.  The  only  assumption
                           made here is that  all the species are acted  on by the same external  force per unit  mass, g;
                           note (b) of Table 19.2-1 explains the modifications needed when this is not the case.
                               The important  feature  of these equations is that they are all of the  form
                                             r
                                              rate of      (net rate  |  [rate of
                                             < increase of =  \ of addition > +  < production J  (19.2-1)
                                             I entity      I of entity  I  I of entity
                           in which  "entity" stands  for mass, momentum, or energy, respectively. In each  equation
                           the net rate of addition  of the entity per unit volume is the negative  of a divergence term.
                           The  "rates  of  production"  arise  from  chemical  reactions  in  the  first  equation  and  from
                           the  external  force  field  in  the  other  two.  Each  equation  is  a  statement  of  a conservation
                           law.  Usually  we  think  of  the  conservation  statements  as  laws  that  have  gradually
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