Page 129 - Modelling in Transport Phenomena A Conceptual Approach
P. 129

4.5.  FLOW ZN CIRCULAR PIPES                                         109


          Analysis
          System: Air in the naphthalene tube

          If naphthalene is designated as species A, then the rate equation for the conservation
           of  species A becomes

                         Rate of  moles of  A in = Rate of  moles of  A out    (1)
           The tern in Eq.  (1) are expressed by

                     Rate of  moles  of  A in = TDL(~,)(AcA)LM                 (2)
                    Rate of  moles of  A out = e(CAb)out = (7rD2/4)(v)(C~b)out   (3)
          Since the  concentration  at  the wall is constant,  the expression for (ACA)LM,
                                                                               Eq.
           (4.5-35), becomes
                                                (CA, )out
                                (ACA)LM                                        (4)
                                        =


          Substitution  of  Eqs.  (i!)-(4) into Eq.  (1) gives
                                                 CAW  ]
                                   1 (4
                            L     4 (kc)  [    (cA, )mt
                                        In  l--
                            D
                              -
                              __-- (')  In (1 - 0.25) = 0.072
                                  4  (kc)
          Note that Eq.  (5) can also be  expressed in the form




          The value of L  depends on the correlations as follows:

          Chilton-Colburn analogy

          Substitution  of  Eq.  (3.5-13) into Eq.  (6) gives
                                      L         2
                                      - = 0.072 - Sc2I3
                                      D         f
          The Reynolds number is




                       - (2-5 10-2)(9) = 13,274  =+        Turbulent flow
                       -
                           16.95 x
   124   125   126   127   128   129   130   131   132   133   134