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480                            Fundamentals of Water Treatment Unit Processes: Physical, Chemical, and Biological



            from this L(wave front) gives the length of the saturated                   L(sat)
                                                                                          t
                                                                                   v wf                   (15:46)
            zone at the end of the run, i.e., L(sat) ¼ L(packed bed)
            L(wave front).
                                                               where
                                                                  v wf is the velocity of wave front, both solid phase and
            15.2.4.1  Quick-and-Dirty Mass Balance                  aqueous phase (m=s)
            The solid-phase wave front, X(Z) t , advances at the same  t is the elapsed time from start of run (s)
            velocity as the aqueous-phase wave front, C(Z) t (Section
            15.2.3.4). This provides a basis for estimating the length of  A second relation is to express V t in terms of HLR, A,
            run from only isotherm and flow data.               and t, i.e.,


            15.2.4.1.1  Velocity of Concentration Profiles                        V t ¼ HLR   A   t        (15:47)
                       by Materials Balance
            The materials-balance principle, applied to a packed-bed  Now combining Equations 15.46 and 15.47 with Equation
            reactor column, with an effluent concentration of near-zero,  15.45 gives an expression for the velocity of the wave
            may be stated,                                     front, i.e.,

                                                                                      HLR   C 0
            V t   C 0 ¼ [rA(1   P)]L(sat)X*(C 0 ) þ [rA(1   P)]              v wf                         (15:48)
                                                                                  X*(C 0 )   r   (1   P)
                       ð Z
                         X(Z)dZ                        (15:44)
                                                               Thus, when the L(sat)   L wf , the wave-front velocity, v wf ,
                      L(sat)                                   may be approximated by Equation 15.48.
            where                                              15.2.4.1.2  Length of Packed-Bed Reactor
                                                               The length of the reactor bed at exhaustion, L(reactor), is the
              V t is the volume of adsorbate solution that has flowed into  sum of the length of the saturated zone, L(sat), plus the length
                                            3
                the column after elapsed time, t (m )
                                                               of the wave front, L wf , i.e.,
              L(sat) is the length of saturated zone of column, defined in
                terms of X=X*(C 0 ), e.g., 1.0   X=X*(C 0 )   0.95; the
                second limit is arbitrary.                                   L(reactor) ¼ L(sat) þ L wf   (15:49)
              X*(C 0 ) is the solid-phase adsorbate concentration at satur-
                ation based on feed concentration, C 0 (kg adsorbate=kg  where
                adsorbent)                                        L(reactor) is the length of packed-bed portion of the reactor
              X(Z) is the solid-phase adsorbate concentration as it  column (m)
                varies with Z in the reaction zone of the column  L wf is the length of wave front, defined in terms of C=C 0 ,
                (kg adsorbate=kg adsorbent)                         i.e., 0.01   C=C 0   0.99 (m)

            Equation 15.44 states that the adsorbate mass lost from the  As with L(sat), the definition of L wf is arbitrary and may
            aqueous phase equals that taken up by the solid phase. The  be taken as the distance for which 0.05   C=C 0   0.95.
            first term on the right is the mass of adsorbate in the saturated  Substituting Equation 15.46 for L(sat) in Equation 15.49
            zone of the solid phase of length, Z ¼ L(sat), while the integral  gives
            gives the mass of adsorbate in the mass-transfer zone, i.e., L wf .
            As the column continues operation, the length of the saturated
                                                                             L(reactor)   v wf   t þ L wf  (15:50)
            zone, i.e., L(sat), increases and, therefore, the mass of adsorb-
            ate in the mass-transfer zone of the column, as depicted by the
                                                               where v wf can be calculated by Equation 15.48. If the satur-
            integral, is less, relative to the mass of adsorbate in the
                                                               ated zone is long, relative to the wave-front length, then
            saturated zone. Therefore, for a long column and after a
            long time of operation, the mass transfer to the solid phase  L wf   L(sat), and Equation 15.49 simplifies to give L(reactor)
                                                               L(sat). The term, L wf , may be determined by a pilot plant
            can be approximated by neglecting the integral in Equation
                                                               study, with sample taps at 50 mm increments along the length
            15.44, i.e., L(sat)   L wf , to give
                                                               of the column. Both computer simulations and pilot plant
                                                               measurements using Rhodamine-B dye and Dowex-50 resin
                   V t   C 0   [rA(1   P)]L(sat)X*(C 0 )  (15:45)  and GAC have indicated that L wf   1.0 m. To illustrate the
                                                               significance of the foregoing relations, if a column has a
            The velocities of the wave fronts for both solid phase and the  packed- bed of say 4.0 m (either a continuous bed or several
            aqueous phase are the same and may be approximated by the  in series) about 1.0 m may be allocated to the wave front
            rate of advance of the saturated zone, i.e.,       (lacking specific data from a pilot plant).
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