Page 361 - APPLIED PROCESS DESIGN FOR CHEMICAL AND PETROCHEMICAL PLANTS, Volume 1, 3rd Edition
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Mixing of Liquids                                       329












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                                     H











                            JACKETED VESSEL HITH ANCHOR-!MPELLER   JACKETED VESSEL HITH HELICAL  IMPELLER
           Figure 5-39.  Close-clearance anchor and helical  impellers.  By permission, Oldshue, J. Y., Fluid Mixing Technology,  1983,  Chemical Engineer-
           ing  McGraw-Hil!  Publications Co.,  Inc.  [29].


             The vertical  tubes  serve  as  baffles  lo  a  certain  extent,   3.  Anchor,  no baffles
           but not enough  to  prevent some  vortex formation.  The   (a)  R,,  =  300 to 4,000, coefficient is 0.38 and µ.jµ is
           helical coil instaliations may have sidewall baffles  (usually   raised to  -0.18 power.
           four Yio  or Yi, dia.), or baffles assembled with the coil itself.   (b)  R,  =  30 to 300,  coefficient is 1.00 and  (µ,Jµ)-o.1s
           (See  Figures 5-23H,  5-231,  5-38 and 5-39.)                and Reynolds number term is raised to 0.50 power.
             Figure  5-40  gives  the  heat  transfer relations  for  a  flat
           paddle  turbine  and  for anchors  in  a jacketed vessel  and   The correlations of  Cummings and West [5, 29]  for tur-
           also  in  coil-lank  arrangements.  The  data  of Cummings   bine mixers  in vessels wi.thjackets and coils are:
           and  West  [5]  are  based  on  large  equipment  and  give
           results  16%  higher for  the  coil  and  11 %  higher for  the   l. Vertical Helical Coils,  Multiple Coils  [29]
          jacket than the results of Chilton,  et al.  [3].
             Heat  transfer data  appear  Lo  be  no  better than  ±20%
           when trying to compare several investigators and the basic
           fundamentals of their systems.
             The  exponents  applying  to  each  system  are  given  on
           the figure.
             The work  of Uhl  [22]  gave  particular emphasis  to vis-
           cous  materials  in jacketed  vessels,  and  the  correlating   m  =  can vary from 0.1  to  1.0
           equations are:                                            m  = 0.1  (µ 8.621  X  10- 5)-021

             1. Paddles, with or without baffles;  R,  =  20 to 4,000   The tube diameter,  d., and tube spacing influence
                                                                     the  film  coefficient,  h.,  The work  of Oldshue  [29]
                                      Jo
                          2
             hT  _    _  D Np  J 0.57   (  cµ  .  3·3  (   µw   J-o  2-1   covers  a  practical  range  about as  large  and as small
             - -0.4b   ( --        -      -            (5- 73)       as  is  industrially  used.  The  tube  spacing  of 2  to  4
              k.           µ        k      µ
                                                                     tube diameters produced consistent results.
             2. Turbine,  no baffles;  Re  =  20  to 200             where  D  =  impeller diameter,  ft
                                                                           T =  tank diameter,  ft
             Relation  same as  for paddle,  coefficient changes  from      µ =  bulk viscosity
           0.415 to 0.535 when the turbine is about two-thirds of the      �' =  wall viscosity at bulk process fluid tempera-
           distance down from top to bottom of the vessel. When the            ture,  d,
           turbine is very near the bottom the coefficient is 0.44.        d, =  tube diameter,  ft,  0.0.
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