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298                                                      Chapter 6

           where the subscripts refer to heavy (H), light (L), and continuous phase (C).
                The  drop  diameter,  d,  for  use  in  Equation  6.16  is  difficult  to  determine.
           There  is not a single  drop  size but a distribution  of drop  sizes.  Jacobs  and Penny
            [17]  recommend  a drop  diameter  of  150 micrometers,  which  is conservative  and
            compensates somewhat for the other assumptions in Equation 6.16.
                Once  the  drop  terminal  velocity  is  found,  the  time  taken  for the  dispersed
           phase  to  reach  the  interface  is  given  by  Equation  6.15.8  in  Table  6.15,  and  the
            decanter length required for the droplets to settle is given by Equation 6.15.9. The
           maximum distance that the  disperse phase droplets have to travel  to reach the in-
            terface,  which is located at the center of the  separator,  is D/2.  The  distance varies
            from zero to D/2. Also, the path of the droplets is not straight down or up but will
            curve because of the motion of the phases.
                The  length of the coalescing zone of the decanter is determined by the time
           required for the dispersed phase to coalesce.  Coalescence could occur by drop to
            drop coalescence  and drop to interface  coalescence.  There  is no relationship that
            can  predict  the  time  required  for  coalescence,  which  according  to  Drown  and
           Thomson  [18]  could vary  from  seconds to many hours.  Coalescence  is enhanced
           when  the  continuous  phase  viscosity  is  small,  the  density  difference  between
           phases large, the interfacial  tension large, and the temperature high. Because of the
           time it takes for coalescence, the dispersed phase drops accumulate near the inter-
            face to form a dispersion zone.  Jacobs and Penny  [17] recommend that the disper-
            sion zone thickness be kept to less than or equal to  10% of the decanter  diameter
            as given by Equation 6.15.10. Also, the drops occupy about half of the volume of
            the dispersion zone volume. Neglecting the  curvature  of the separator, the disper-
            sion zone  volume  is equal to  H A], where  H  is the thickness  of the dispersion
                                     D         D
            zone, and AI  is the  area of the interface.  Therefore,  the residence time, IR, of  the
            drops  in the  dispersion zone  is  given by  Equation  6.15.11.  The  residence  time  is
            specified  by experience, and the interfacial  area required  for coalescence is calcu-
            lated.  If  it  is  assumed  that  the  interface  will  be  located  at  the  center  of  the  de-
            canter,  then  the  length  of  the  coalescing  zone,  L D,  is  calculated  from  Equation
            6.15.12. The total length of the decanter is the sum of the lengths required for set-
            tling and coalescence.  The procedure for calculating the dimensions of a decanter
            is given in Table 6.16,  and Example 6.4 illustrates the procedure.

            Table 6.16  Calculation Procedure for Sizing Liquid-Liquid Separators


            1. Calculate 6 to determine the dispersed phase from  Equation 6.15.1 using Table
            6.13.

            2.  Solve Equations  6.15.14,  6.15.16,  6.15.18,  6.15.20  and  6.15.22  for D L, the  in-
            side diameter of the decanter,  assuming that the light phase determines the diame-
            ter.






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