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                  3.5 Agitated Slurry Reactors                     137


                    For single-impeller systems, the correlation of Calderbank can be used (Bouaif i   et al  .,
                  onen  2001; Laakk  et al  ., 2005):

                                                    
 35   h  0.5
                                        d  bub     4.15  L  G  0.0009
                                                       P   g   25                 (3.263)
                                                    35
                                                   L   V   L   

                  These correlations have been derived for Ruhston turbines, but they can be applied for flat-
                  blade impellers as well (Laakkonen   et al  ., 2005). SI units should be used in these correlations.

                  Double-impeller combinations  Bouaifi   et al  v wing correlations . (2001) deried the follo
                  for stirred gas–liquid reactors with various combinations of double impellers.  The
                  impellers used were the lightning axial flow impeller (A-310), the four 45° pitched blade
                  turbine pumping down (PBTD) and the Rushton disk turbine (RDT). Furthermore, the tank
                    fles,
                  was a dish-bottom cylindrical tank equipped with four baf while the gas was intro-
                  duced by a ring sprager. The gas-flow rate ranged from 0.54 to 2.62 L/s, whereas the rota-
                  tional speed was from 1.66 to 11.67 s  –1  . The gas holdup is
                                                     P   g   0.24
                                             h  G  C      V   L    u  sG  0.65  (3.264)


                  where   h  G  is in %,  P / V  L  in W/m  3  , u  sG    0.018 m/s, and   C  is between 22.4 and 24.8.
                                   g
                  The gas holdup was found to be lower than 10% as in the case of simple impeller conf ig-
                  urations (Panja and Phaneswara Rao, 1993). This correlation holds for operating condi-
                  tions beyond the complete dispersion point, corresponding to the situation of
                  homogeneous gas dispersion in which bubbles reach the bottom of the tank. It should be
                  noted that in the case of agitated v it is dificult to propose a general correlation to f
                   essels,
                  predict gas holdup, because it is dependent on the stirrer configuration and sparger type
                  (Bouaifi   et al  ., 2001). Furthermore, gas holdup is expected to be influenced by the solids
                  in three-phase systems. The Sauter mean diameter is affected by the specific power con-
                  sumption, but not by the gas flow rate (Bouaif i   et al  ., 2001). For double-impeller combi-
                  nations (Bouaif i   et al  ., 2001),

                                                          P   g   0.20
                                          d     10.1 10    3                        (3.265)
                                           bub            V   L  

                  where   d  bub  is in m. SI units are used with this correlation.

                  The effect of solids
                    In general, the addition of solids influences the b ubble diameter due to the greater num-
                  ber of bubble collisions resulting in increased coalescence, and thus, in an increase in b ub-
                  ble size (Panja and Phaneswara Rao, 1993).
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