Page 271 - APPLIED PROCESS DESIGN FOR CHEMICAL AND PETROCHEMICAL PLANTS, Volume 1, 3rd Edition
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Mechanical  Separations                                    241
             For an aqueous-hydrocarbon or organic solvent mixture:   Optimum vessel  diameter:
                                                                   Assume  20%  cross-sectional  area  is  occupied  by  an
          The top layer will be hydrocarbon, with the aqueous layer   emulsion  and  is  recognized  as  a  "dead volume." This  is
           droplets settling through the  hydrocarbon.  111e  terminal   actually the height over which the interface level will vary
          velocity is:                                          during normal  operations  [26].

             vhc  =  12.86  (6SpGr)/µhc,  in./min       (4-21)                                                (4-24)

             vhc  =  terminal settling velocity of aqueous droplets in   0 =  ± [a/2 ±  (a 2  - 4b)  112 /2]  112,  ft   (4-25)
                  hydrocarbon phase in  top of vessel, in./min
          6SpGr =  differences in  specific gravity of the particle and sur-                                  (4-26)
                  rounding fluid
                                                                                                              (4-27)
             µhe  =  viscosity of surrounding fluid,  cp
                                                                   The economical vessel ratio is L/D =  r
             Height of hydrocarbon layer to the interface:
                                                                Modified Method of Happel and Jordan  [29]
                                                       (4-21A)
                                                                   This  method  is  a  modification  of the  earlier method
             h,  =  38.4 A/  (rcO)  +  1.20            (4-l5A)   [30]  by  Reference  [26], as  follows,  and  can  be  less  con-
                                                                servative  [26]  than  the  original  method  [30].  A  basic
           ht= height of continuous  hydrocarbon  phase in the  top of   assumption  is  that  particles  must rise/fall  through  one-
               vessel, in.                                      half of the drum vertical  cross-sectional area  [26].


                                                        (4-22)     t  =  h/v

           A 1  =  cross-sectional area at top of vessel  occupied by  the con-   t =  (1/2) (7.48) [0.8 1t0 2 L/4]F,   (4-28)
               tinuous  hydrocarbon  phase,  sq ft
          Ab  =  cross-sectional  area at bottom of vessel  occupied by con-   F,  =  flow rate  of both phases
               tinuous aqueous phase, sq ft                     v,  =  v  =  terminal settling velocity,  in./min

                                                                This assumes 20% of the cross-sectional even as "dead vol-
             For the bottom aqueous phase:
                                                                ume." The height from  the interface can  be  determined
          hydrocarbon  droplets  settle  out of the  continuous  aque-   by combining the above  equations:
          ous  phase.  The  terminal  velocity  is  for  hydrocarbon
           droplets:                                               h  =  (0.748)TC0 2 Lv/F,                   ( 4-29)
                                                                   The height for each interface is:
             "•q  =  12.86  (6SpGr)/µ.iq,  in./min      (4-23)
                                                                                                              (4-30)
           Vaq  =  terminal  settling velocity of hydrocarbon droplets in
               aqueous phase in bottom of vessel, in./min          hb  =  (0.748)  TC0 Lvaq/F,                ( 4-31)
                                                                               2
          µaq  =  viscosity of aqueous phase, cp
                                                                  A,= [(0.748)  TC0 2 Lvhc/F,  - 1.20]  TCD/38.4   ( 4-32)
             Height of aqueous layer to the interface:
                                                                  Ab= [(0.748)  TC0 2 Lvaq/F, - l.20]  TCD/38.4   (4-33)

                                                       (4-21A)   Example 4-3: Horizontal Gravity Settlers

                                                       (4-15A)     Using  the  data  from  Sigales  [31]  and  following  the
                                                                design  of [26]:
           hb  =  height of  continuous aqueous  phase in bottom of vessel,   Data for propane/caustic wash:
               in.                                                 Fhc  =  95  GP:tv1
          Ab  =  cross-sectional area al bottom of vessel occupied by con-   Faq  =  39 GPM
               tinuous aqueous phase,  sq ft
                                                                   Vaq  =  5  in./rnin
                                                                   Vhc  =  120 in./min
             Ab= l.20[(7.48)Lvaq(f,gF,g)  - 38.4/(TC0)]- 1   (4-22)   r =  3.4
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