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Mixing                                                                                           247



                                                                    on infinitesimal particles, as described by the Navier–
                                                                    Stokes equation. The continuous advection of vortex
                                                                    tubes past any given point with changing orientation is
                                                                    a plausible explanation for the Eulerian (i.e., fixed
                                                                    coordinates) observation of turbulence as illustrated
                                                                    in Figure 10.5. Figure 10.6 illustrates the alternate
                                                                    ‘‘Lagrangian’’ view, i.e., a relative coordinate system
                                                                    in which the observer moves with the motion of a given
                                                                    parcel.

                                                               10.3.1.2.2  Turbulence Generation
                                                               As stated, turbulence is associated with velocity gradients
                                                               (i.e., fluid shear). To generate turbulence for mixing, bound-
            FIGURE 10.6  Space-fillingvortextubes.(AdaptedfromHanson,A.T.  ary discontinuities give the highest velocity gradients, i.e.,
            and Cleasby, J.L., J. Am. Water Works Assoc., 82(11), 56–73, 1990.)  high shear. Form separation and submerged jets are two
                                                               approaches for causing such high-shear zones (Rushton and
                                                               Oldshue, 1953b, p. 268) and are illustrated in Figure 10.7a
                 Meroney, 2001; Bienkiewicz, 2001). Figure 10.6 is a  and b, respectively. In each case, the discontinuity causes
                 depiction of such an array of vortex tubes having a  eddies; the shear (velocity gradient) between a given eddy
                 spectrum of diameters, lengths, orientations, and  and the surrounding fluid results in an ‘‘eddy cascade.’’
                 energy levels. The tubes also interfere with one  The turbulence generated by the separation seen in (a) is
                 another, causing a given tube to combine with another  termed ‘‘wake turbulence’’ and causes ‘‘wake mixing’’
                 and perhaps breaking (Bienkiewicz, 2001). In addition,  (Stenquist and Kaufman, 1972, p. 7). In (b) there is no formal
                 a given vortex tube sheds smaller daughter vortices,  designation but the term, ‘‘jet mixing,’’ is descriptive. These
                 losing some of its energy. Eventually, the vortices  two themes, i.e., wake mixing and jet mixing, permeate
                 become small enough that viscous forces predominate  virtually all mixing technologies.
                 and the kinetic energy of the vortex dissipates as heat
                 that occurs in the ‘‘viscous sub-range’’ of the ‘‘energy  . Wake turbulence: Wake turbulence is created by
                 spectrum’’ (Section 10.3.1.2.3). The vortex tangle is  devices such as a flat-blade radial-flow impeller,
                 thus a part of a dynamic system and has a deterministic  an orifice plate in a pipeline, a sudden pipe expan-
                 character in that it is due to the forces and acceleration  sion, etc. Figure 10.8 illustrates the process of eddy
















                                         (a)


                                       Core of jet



                                 Nozzle





                                (b)


            FIGURE 10.7  Types of boundary discontinuities. (a) Flat plate causing wake turbulence. (b) Submerged jet generating eddies.
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