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Sec. 4.2   Scale-up of Liquid-Phase Batch  Reactor Data to the Design of a CSTR   139






                                  If  instead  of  two GSTRs in  series we  had  n equal-sized CSTRs connected in
                                  series  (7,  = z2 =   = z,  = z)  operating  at  the  sane temperature  (k, == k,  =
                                  ... zz  k,  = k), the concentration leaving the last reactor would be

                                                                                              (4-10)


                                  The conversion for these n tank reactors in series would be
                     Conversion as a                      I
                      function of the                                                         (4-1 1)
                         number of
                      tanks in series

                                  A plot of the conversion as a function of the number of reactors in series for a
                                  first-order reaction is shown in Figure 4-4 for various values of the Damkohler











                     CSTRs in series






                                                  0  1  2  3  4  5  6  7  8  9  1  0  1  1  I  2  1  3
                                                               Number of tonks, n
                                       Figure 4-4  Conversion as a function of the number of tanks in series for different
                                       Damkohler numbers for a first-order reaction.


                                  number  zk. Observe from Figure 4-4 that when the product of  the space time
                                  and  the  specific reaction rate  is relatively large,  say, Da  2 1,  approximately
                                  90%  conversion is achieved in  two  or three reactors; thus the  cost of adding
                                  subsequent  reactors  might  not  be  justified.  When  the  product  zk  is  small,
                                  Da - (3.1, the conyersion continues to increase significantly with  each reactor
                                  added.
                                       The rate of disappearance of A in the nth reactor is

                                                        -rAn = kCAn = k -
                                                                         c.40
                                                                       (1 + zk)"
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