Page 54 - The engineering of chemical reactions
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38   Reaction Rates, the Batch Reactor, and the Real World

                             We will write all reactor mass and heat balances as

                                  accumulation =  flow  in  -  flow out + generation by reaction


                        an expression we will see many times in mass and energy balances throughout this book.
                             We remark before proceeding that equations such as
                                                      dC.4  = -kCA
                                                      -
                                                    .  dt
                        and its integrated form

                                                      CA  =  cAoeekt
                        arise from a very special situation requiring both a single$rst-order  irreversible reaction
                        and a constant-volume isothermal batch reactor. This example is almost trivial,  although
                        we will use it frequently as a comparison with more interesting and accurate examples. The
                        assumption of first-order kinetics is a simple first guess for kinetics and a good starting
                        point before more elaborate calculations.
                             We note before proceeding that we must formulate and solve many mass-balance
                        equations. We strongly encourage the student not to memorize anything except the basic
                        defining relations. We stress that you should be able to derive every equation from these
                        definitions as needed. This is because (1) only by being able to do this will you understand
                        the principles of the subject: and (2) we need to make many different approximations, and
                        remembering the wrong equation is disastrous.

        THE BATCH REACTOR

                        A batch reactor is defined as a closed spatially uniform system which has concentration
                        parameters that are specified at time zero. It might look as illustrated in Figure 2-4. This
                        requires that the system either be stirred rapidly (the propeller in Fig. 24) or started out
                        spatially uniform so that stirring is not necessary. Composition and temperature are therefore
                        independent of position in the reactor, so that the number of moles of species j  in the system
                        Nj  is a function of time alone, Since the system is closed (no flow in or out), we can write
                        simply that the change in the total number of moles of species j  in the reactor is equal to the
                        stoichiometric coefficient  vi  multiplied by the rate multiplied by the volume of the reactor,


                                                 Figure 2-4.  Sketch of a uniform closed container for running chemical
                                                 reactions, which we call a batch reactor.


                                           cj(t)
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