Page 109 - Fundamentals of Water Treatment Unit Processes : Physical, Chemical, and Biological
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64                             Fundamentals of Water Treatment Unit Processes: Physical, Chemical, and Biological



            4.3.3.3.2  General Applicability of Equation 4.9   clearly that the solute concentration within the reactor varies
            First, consider that we may wish to let either Q or C 0 , or both  with Z. Therefore, the reactor is not homogeneous. Conse-
            at once, vary with time, which is the operating condition for  quently, the materials balance equation cannot be applied to
            most treatment plants. Such a condition can be imposed  the reactor as a whole, that is, over the column length. The
            merely by writing Equation 4.9 in finite difference form and  condition of homogeneity may be true, however, if the vol-
            solving numerically.                               ume element is infinitesimal. Figure 4.6 shows such a volume
              In addition, we can impose any special conditions (as noted  element for a column slice of thickness DZ.As DZ approaches
            in Section 4.3.3.1) that we wish, such as for a ‘‘batch’’ reactor,  zero, then the solute approaches homogeneity within the
            that is, Q C in ¼ 0 and Q C ¼ 0. Or we can impose the ‘‘steady  element. Thus, the materials balance equation may be applied
            state’’ condition, in which the observed mass rate of change in  to the infinitesimal slice.
            the reactor, the term on the left side of Equation 4.9, is zero.
                                                               4.3.3.3.5  Application of Materials Balance Equation
            Finally, we can let the rate of reaction equal zero and solve for
            the effluent concentration, C, leaving the reactor, such as for a  Figure 4.7 shows a materials balance for an infinitesimal
            salt solution displacing some other solution from the reactor.  column slice of thickness, DZ and area, A. The corresponding
                                                               mathematical statement is given by Equation 4.10. The mass
            4.3.3.3.3  Packed-Bed Reactor (Column)             transport terms are advection and dispersion, both illustrated
            Packed-bed reactors include: activated carbon, ion exchange,  in Figure 4.7.
            trickling filters, various biofilm reactors (e.g., slow sand), and

            rapid rate filters. All packed-bed reactors have concentration  q(C   DZ   A)  ¼   v   A   C in     v   A   C out þ j A   j A
            changes from the entrance of the reactor to its exit, as Figure  qt  0                  in   out
            4.6 illustrates. In Figure 4.6, the concentration of the solute       q(C   DZ   A)
            entering the reactor is designated, C 0 . The concentration               qt     r             (4:10)
            declines as a continuous function with distance, Z, along the
            column, that is, C(Z) t , and may be characterized as the ‘‘con-  in which
            centration profile’’ at a designated time, t.          Z is the distance along column from entrance (m)
              If the reactor is steady state, such as a trickling filter with    v is the velocity within column (m=s)
            no change in Q or C 0 with time, then the profile will remain  A is the cross-sectional area of column (m )
                                                                                                   2
            constant. But if the porous media becomes saturated with  t is the elapsed time from beginning of operation (s)
            time, such as with GAC, an ion-exchange bed, or a rapid
                                                                  C in is the concentration of given contaminant into the
            rate filter, then the profile will advance downstream with time.             3
                                                                    infinitesimal slice (kg=m )
              In addition to packed-bed reactors, this same schematic,
                                                                  C out is the concentration of given contaminant leaving the
            that is, Figure 4.6, is applicable to a ‘‘plug flow’’ type of               3
                                                                    infinitesimal slice (kg=m )
            fluidized reactor. The latter may include reactors that are                                     2
                                                                  j in is the dispersion flux density into element (kg=m =s)
            long and narrow, such as ‘‘conventional’’ activated sludge.
                                                                  j out is the dispersion flux density leaving element
            A river would also fit in this category.                      2
                                                                    (kg=m =s)
            4.3.3.3.4  Homogeneity Requirement
            As noted previously, the materials balance equation is valid
                                                                           Convection in  Dispersion in
            only for a homogeneous volume element. Figure 4.6 shows            –
                                                                          –   ∂(vC)  ΔZ    ∂j ΔZ
                                                                          vC–        A  + j –   A
                                                                               ∂Z  2       ∂Z 2
                                            C
                                  0                        C 0
                                                                                                      Z
                                                                                 –
                                                                                 vCA +  jA
                                                                  ΔZ
                                                                   2
                      Z                                        ΔZ                                         ∂C  ΔZA
                                                                                                           ∂t  r
                                                                  ΔZ                                    Reaction
              Column length  ΔZ            C(Z) t
                                                                   2
                                                                               –
                                                                          –   ∂(vC) ΔZ     ∂j ΔZ
                                                                          vC–        A  + j–    A
                                                                               ∂Z  2       ∂Z 2
                                                                           Convection out  Dispersion out
                                                Inflection point
                                                               FIGURE 4.7 Materials balance on infinitesimal column slice of
                                                               thickness, DZ, and area, A showing terms for derivation of materials
            FIGURE 4.6 Concentration profile in a packed-bed reactor.  balance equation.
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