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                  3.8 T Fluid–Solid Fluidized Bed Reactors o-Phase, w  201


                    The use of internals can improe the smoothness of fluidization, when this is desirable. v
                  The use of vertical cylindrical tubes immersed in the bed is a representatie e v xample.
                  f
                  These tubes are suficiently long to extend from the distributor to the top of the bed. F or
                  this type of beds and for perforated plate distributors, the following correlation can be used
                  for the estimation of fluidized-bed porosity in gas–solid fluidization (Hilal, 2000):

                                             u    fm         f       w            (3.479)
                                               u
                                              s
                                                            fm
                                            u   u        1      
                                             ter  fm       fm
                  where:
                                             w  1.28 0.00033     P  3               (3.480)

                  where   u  ter  is the terminal velocity of the particles and   P is the hole pitch of the perforated
                  plate. A square pitch of 7–12 mm is typical.

                  e Criteria for distinguishing fluidization r gimes

                     ,
                  The minimum bubbling velocity for Group A particles (or more generally for TA ype
                  fluidization) and gas–solid systems is (Abrahamsen and Geldart, 1980;  e  Y  et al  ., 2005)
                                              2.07  0.06 G  d exp(0.716    p )  X  4 5
                                        u                                           (3.481)
                                         bm            0.347
                                                      
 G
                  where   X  45  is the fraction of particles with size smaller than 45   µm and   d  p  the siee diam- v
                  eter. In this equation, SI units should be used. In the region of Group B particles (for ambi-
                  ent conditions and air as gas phase) or in the  Type B fluidization regime (for other
                  conditions), where   u  bm  = u  fm  , the aboe equation results in  v  u  bm  <  u  fm  , which is not accept-
                  xample,
                  able. For e for ambient conditions and air as gas, if   d  p  = 0.24 mm and     = 1500
                                                                                   h
                  kg/m  3  , we are in the re (Figure 3.52) and the result is  gion of Group B particles  u  bm  = 0.022
                  m/s, while   u  fm  = 0.028 m/s.
                    Using the Bayens equation (3.460) and eq. (3.481), the ratio of minimum b ubbling
                  velocity to minimum fluidization velocity is
                                       u    2300    0.126  exp(0.716
 0.523  )  X
                                        bm       G   G            45                (3.482)
                                       u  fm   d  0.8 p  (   p     G  )  0.934  0.  g  9 934
                                               u  b m                          u  b m
                  For type B fluidization, we obtain (     =  1), while for type A fluidization (       1). In
                                               u                               u
                                                fm                              fm
                  the second case, the fluidization regime is
                  •  particulate, if   u  fm    u  s    u  bm
                  •  type A bubbling, if   u  s    u  bm

                    In Figure 3.54, the ratio of the minimum b elocity to the minimum fluidization ubbling v
                  velocity is plotted for air at 20 °C, and     is 1000–3000 kg/m  3  . From Figure 3.52 and the
                                                   p
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