Page 710 - Bird R.B. Transport phenomena
P. 710

690  Chapter 22  Interphase Transport in Nonisothermal Mixtures

                               The  mean two phase mass transfer  coefficients  must be defined  carefully,  and we con-
                            sider  here only  the special  case where  bulk  concentrations in  the two  adjacent  phases  do
                            not  change significantly  over the total mass-transfer  surface  S. We may then define K°  by
                                                                                                  XIU
                                                     |
                                             (N )  = J  K° , (x  -  x )dS  = K'JXAC  ~         (22.4-11)
                                               A0 m       x loc  Ae  Ab
                            so that, when  Eq. 22.3-9 is  used,

                                                                             -dS               (22.4-12)
                            Frequently  area  mean  overall  mass  transfer  coefficients  are  calculated  from  area  mean
                            coefficients  for the two adjoining  phases:

                                                                                               (22.4-13)
                                                     х
                                                     дг,арргох  (I/O  +  а/т Щ,„)
                                                                          х
                            The  two  mean values  in  Eqs. 22.4-12  and  13 can be  significantly  different  (see  Example
                            22.4-3).

       EXAMPLE 22.4-1       Oxygen  is to be removed  from  water using  nitrogen gas  at atmospheric pressure and 20°C in
                            the  form  of bubbles  exhibiting  internal circulation, as shown  in Fig. 22.4-3. Estimate the rela-
      Determination  of  the  t i v e  importance of  the two  mass  transfer  coefficients  k°  and  ^  l o c .  Let Л stand  for  О„ В for
                                                                        xloc
      Controlling Resistance  H O, and С for N .
                                         2
                             2
      SOLUTION              We can do this by assuming that the penetration model (see §18.5) holds in each phase, so that
                                             t°  «  k  = r,  /  —•  к 0  «  к  —г  /  л с      СУ)  4-1 А.)

                            where  с, and  c  are the total molar concentrations in the liquid  and  gas  phases,  respectively.
                                       g
                            The  effective  exposure time, f , is the same for  each of the phases.
                                                   exp
















                                               Oxygen-
                                              , containing
                                                water







                                                         Fig.  22.4-3.  Schematic diagram  of an oxygen  stripper, in
                                 Nitrogen                which oxygen  from the water diffuses  into the nitrogen
                                   gas                   gas  bubbles.
   705   706   707   708   709   710   711   712   713   714   715