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Screening                                                                                         91


              HLR is by definition:                             which is essentially the same as the mass removal rate, since
                                                               C   0, is obtained by multiplying both sides of Equation
                                      Q                        Ex5.3.20 by C r . The resulting equation is merely a derivative
                                                   (Ex5:3:18)
                                     LQ M r                    of Equation Ex5.3.20 and is not shown.
                               HLR ¼
                                                                  The ‘‘passive’’ variables in Equation Ex5.3.20 may be
              Combining (Ex5.3.17) and (Ex5.3.18) gives
                                                               consolidated into a single coefficient, K, which must be deter-
                                                               mined by pilot plant testing, or from data obtained from a full-
                                           0:5
                            2rvk(mat)h L (mat)                 scale plant. The variable, Q M , is also consolidated in the
                                                   (Ex5:3:19)
                     HLR ¼
                                Q M C r                        coefficient. The result is an equation that has more utility, i.e.,
              Again, to simplify, substitute Equation Ex5.3.13 for h L (mat)              0:5 0:5
              to give                                                            HLR ¼ Kv h  L          (Ex5:3:21)
                                         0:5                   Figure 5.12a and b shows plots of HLR vs. h L and HLR vs. v,
                              2rvk(mat)h L
                                                   (Ex5:3:20)                          4
                       HLR ¼                                   respectively for K ¼ 3.6   10  m=s. Figure 5.12a shows that
                                Q M C r
                                                               increasing headloss toward the higher end of practice can
                                                               yield significantly higher HLR. Figure 5.12b shows that pro-
                                                               viding for a several-fold increase in v can permit significantly
            5.5.7.1  Interpretation of Model Results           higher HLR, which would therefore be an important variable
            Equation Ex5.3.20 says that the HLR for design is a function  in operation.
            of the variables listed in the equation to the 1=2 power. The  By the same token, since A ¼ Q=v, the plots, Figure 5.13a
            two design-independent variables are h L and Q M , while v is  and b, respectively, are derivatives of Figure 5.12a and b,
            an operating variable, and r, k(mat) and C r are ‘‘passive’’  respectively. Figure 5.13a shows that the required area for a
                                                                     3
            variables, i.e., those that are ambient or are otherwise not  0.31 m =s (7 mgd) flow declines exponentially with an
            controlled. The mass loading rate per unit area (MLR),  increase in headloss applied to the design. Also, if v is applied


                    0.010                                          0.010
                    0.009                                          0.009
                    0.008                                          0.008
                    0.007
                   HLR (m 3 /s/m 2 )  0.006  y=0.006147*x^(0.49875)  HLR (m 3 /s/m 2 )  0.006  y =0.010393*x^(0.48944)
                                                                   0.007
                    0.005
                                                                   0.005
                                                                   0.004
                    0.004
                    0.003
                                                                   0.002
                    0.002    Range of                              0.003   Range of practice
                              practice
                    0.001                                          0.001
                    0.000                                          0.000
                        0.0   0.5   1.0   1.5  2.0   2.5   3.0         0  0.1 0.2 0.3 0.4 0.5 0.6 0.7 0.8 0.9  1
                 (a)                    h  (m)                  (b)                   ω (rad/s)
                                         L
            FIGURE 5.12  Microscreen calculated HLRs for K (50%). (a) HLR versus h L for h L ¼ 0.3 m. (b) HLR versus v for v ¼ 0.1 rad=s.


                     150                                          150
                                          y=50.087*x^(–0.49912)                        y=29.608*x^(–0.48992)

                    A(net) (m 2 )  100                           A(net) (m 2 )  100



                      50
                          Range of                                 50
                          practice                                       Range of practice

                      0                                             0
                       0.0   0.5   1.0   1.5   2.0   2.5   3.0       0.0 0.1 0.2 0.3 0.4 0.5 0.6 0.7 0.8 0.9 1.0
                  (a)                   h  (m)                  (b)                 ω (rad/s)
                                         L
            FIGURE 5.13  Microscreen calculated net screen area for K (50%). (a) A(net) versus h L for h L ¼ 0.3 m. (b) A(net) versus v for
            v ¼ 0.1 rad=s.
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