Page 690 - Bird R.B. Transport phenomena
P. 690

670  Chapter 21  Concentration Distributions in Turbulent Flow

                           as shown  in Fig. 21В.З(я). A small  voltage  is applied  across  the plates to produce a deposition
                           of  Ag  on the cathode (lower  plate) and  to polarize the circuit completely  (that is, to maintain
                           the Ag +  concentration at the cathode very nearly  zero). Forced diffusion  may be ignored, and
                           the Ag +  may  be  considered  to be  moving  to the cathode by  ordinary  (that is, Fickian)  diffu-
                           sion  and eddy  diffusion  only. Furthermore, this solution  is  sufficiently  dilute that the  effects
                           of the other ionic species  on the diffusion  of Ag +  are  negligible.
                           (a)  Calculate the Ag +  concentration profile,  assuming  that  (i) the effective  binary  diffusivity
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                           of  Ag +  through water  is  1.06  X  10~  cm /s;  (ii) the truncated  Lin, Moulton, and  Putnam ex-
                           pression  of  Eq.  5.4-2  for  the turbulent  velocity  distribution  in  round  tubes  is  valid  for  "slit
                           flow"  as well,  if  four  times the hydraulic  radius  is  substituted  for  the tube diameter; (iii) the
                           plates are  1.27  cm apart, and W /p  is  11.4 cm/s.
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                           (b)  Estimate the rate of deposition of Ag  on the cathode, neglecting all other electrode reactions.
                           (c)  Does the method of calculation in part (a) predict a discontinuous slope  for  the concentra-
                           tion profile  at the center plane of the system?  Explain.
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                           Answers: (a) See Fig. 21B.3(W;  (b) 6.7  X 10~  equiv/cm  2  • s
                     21B.5.  Mixing-length expression for  the velocity profile.
                            (a)  Start with  Eq. 5.5-3, and show  that for  steadily  driven, fully  developed  turbulent flow  in
                           a tube




                            (b)  Next set  т, 2  = т^ 0  + r^, where  т^° is given  by  the cylindrical  coordinate analog  of  Eq. 5.2-9,
                           and  т*2 by  Eq. 5.5-5. Show that Eq. 21B.5-1  then becomes




                            (c)  Obtain Eq. 21.4-13  from  Eq. 21B.5-2 by introducing the dimensionless  symbols  used  in the
                            former equation.
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