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 Encyclopedia of Physical Science and Technology  EN014A-654  July 28, 2001  16:35






               34                                                                            Reactors in Process Engineering


               or                                                                 Y A0 ν  (0.5)(2)
                                                                            E A =     =         = 1.0.
                                     t

                                1   V dC A  C A dV  t                             |ν A |  |−1|

                        −r A =−  t        +        ,
                                V    dt       dt
                                                                   c. Summary of ideal batch reactor design
               or
                                                                 equations.
                                               t
                                   dC A   C A dV                   i. General case.
                          −r A =−      +         .
                                    dt    V t  dt
                                                                                  1 dN i             N i
               From thermodynamics, assuming ideal solutions, we can               t    = r i   C i ≡  t
                                                                                  V dt               V
               derive an expression relating the volume at any conversion
                                                                                      t
                                                                               C i d(ln V )
               with the original volume,                                 dC i  +        = r i
                                                                         dt       dt

                          t    t     N A0  ν i V i
                        V = V 1 +           t  X A ,                           N A0 − N A
                              0
                                       |ν A |V                               ∼
                                           0                              X A =           [for reactant A]
                                                                                  N A0
               where V i is the molar specific volume of componenti. This
                                                                                 t
               expression is usually simplified by defining an expansion          V 0  dX A
                                                                           C A0  t      =−r A .
               factor in terms of any reactant; for A,                          V   dt
                                                                   ii. Constant temperature and pressure ideal solution.
                                     N A0  ν i V i
                               E A ≡
                                      |ν A |V  t
                                          0                                                   C A0  ν i V i
                                                                                         E A ≡
               and                                                                               |ν A |
                                    t
                               t
                             V = V (1 + E A X A ).                             C A0      dC A
                                   0
                                                                                            =−r A
               This changes the ideal batch reactor equation to            C A0 + E A C A  dt
                                                                   iii. Ideal gas.
                                     C A0  dX A
                            −r A =             ,
                                  1 + E A X A dt                                               Y A0 ν
                                                                                          E A ≡
               where                                                                            |ν A |
                                    C A0  ν i V i
                               E A ≡                                             C A0   dX A
                                       |ν A |                                                =−r A
                                                                              1 + E A C A  dt
               and assumes constant temperature, pressure, and ideal
                                                                   iv. Constant volume.
               solutions.
                 For the special case of an ideal gas mixture,                       dC i
                                                                                         = r i
                                                                                      dt
                                       Y A0 P
                                 C A0 =
                                        RT                                          dX A
                                                                                 C A0    =−r A .
               and                                                                   dt
                                       RT
                                  V i =                            3. Single Ideal Flow Reactor
                                        P
               which leads to an easy formula to calculate the change in  For batch reactors, time is the key design variable. The
               volume factor.                                    batch reactor design equations answer the question: How
                                      Y A0 ν                     long does it take to obtain a specified conversion or
                                 E A =    ,
                                       |ν A |                    concentration?
                                                                   With flow reactors, volume is the key design variable.
               where Y A0 is the initial mole fraction of A, ν the sum of
                                                                 For a given feed rate, how big must the reactor be to get a
               the stoichiometric numbers, and |ν A | the stoichiometric
                                                                 specified conversion?
               number of component A.
                 iii. Example.A → 3R. Given that the feed is 50% A
                                                                   a. Ideal continuous-stirred tank reactor design
               and 50% inerts, calculate E A . By stoichiometry,
                                                                 equations. Very well-mixed unreacted material flows
                         |ν A |=|−1|= 1                          into a vessel, reacts, and exits the reactor along with
                                                                 converted product. Starting with the general reactor de-
                           ν =  ν i = 3 − 1 = 2
                                                                 sign equation, several assumptions are made to reduce the
                         Y A0 = Y 10 = 0.50                      equation to a usable form.
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