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 Encyclopedia of Physical Science and Technology  EN006C-252  June 27, 2001  14:15








              Fluid Mixing                                                                                 87





























                                 FIGURE 14  The velocity spectra in the axial direction for an axial impeller A200.


              today is specifying mixers for industrial processes based  where ν is the dynamic viscosity and e is the power per
              on meeting criteria of this type. This is largely because  unit volume.
              processes are so complex that it is not possible to define
              the process requirements in terms of these fluid mechanics  II.  SCALEUP RELATIONSHIPS
              parameters. If the process results could be defined in terms
              of these parameters, sufficient information probably exists
                                                                Scaleup involves determining the controlling factors in a
              to permit the calculation of an approximate mixer design.
                                                                process, the role that mixing plays, and the application of
              It is important to continue studying fluid mechanics pa-
                                                                a suitable scaleup technique. In this section, the general
              rameters in both mixing and pipeline reactors to establish
                                                                scaleup relationships will be presented, and the particular
              what  is  required  by  different  processes  in  fundamental
                                                                types of processes involved will be covered. Section X
              terms.
                                                                will cover pilot planting, how runs are made to determine
                Recently, one of the most practical results of these stud-
                                                                the controlling factor, and how to choose a suitable design
              ies has been the ability to design pilot plant experiments
                                                                relationship for that situation.
              (and, in many cases, plant-scale experiments) that can es-
                                                                  Table III is a key for understanding scaleup relation-
              tablish  the  sensitivity  of  process  to  macroscale  mixing
                                                                ships. In the first column are listed many design vari-
              variables (as a function of power, pumping capacity, im-
                                                                ables involved in mixing processes. These include power,
              peller diameter, impeller tip speeds, and macroscale shear
                                                                power per unit volume, speed, impeller diameter, impeller
              rates) in contrast to microscale mixing variables (which
              are relative to power per unit volume, rms velocity fluctu-
              ations, and some estimation of the size of the microscale  TABLE III Properties of a Fluid Mixer on Scaleup
              eddies).                                                  Pilot scale
                Another useful and interesting concept is the size of the  Property  (80 Liters)  Plant scale (17.280 liters)
              eddies, L, at which the power of an impeller is eventually
              dissipated. This concept utilizes the principles of isotropic  P  1.0  216  7776   36      0.16
                                                                P/Vol      1.0     1.0     36     0.16    .0007
              turbulence developed by Komolgoroff [1]. The calcula-
                                                                N          1.0     0.3     1.0    0.16    .03
              tions assume some reasonable approach to the degree of
                                                                D          1.0     6.0     6.0    6.0    6.0
              isotropic turbulence, and the estimates do give some idea
                                                                Q          1.0     65     216    36      6.0
              as to how far down in the microscale size the power per
                                                                Q/Vol      1.0     0.3     1.0    0.16    .03
              unit volume can effectively reach
                                                                ND         1.0     1.8     6.0    1.0    0.16
                                                                  2
                                                                ND ρ       1.0     10.8    36     5.8    1.0
                                     3
                               L = (ν /e) 1/4                     µ
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