Page 164 - Reservoir Formation Damage
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146   Reservoir Formation Damage

                dimensionless  group,  which  relates  the  Stokes  and  convection  velocities
                as  (Ives,  1985):



                                                                           (8-3a)
                         18jiv fl

                Centrifugal  Forces.  The  centrifugal  forces  are  generated  by  external
                acceleration.  The  centrifugal force  created  with  an  angular velocity  of  w
                and  a  radius  of  R  is  expressed  in  dimensionless  form  by



                  G  =                                                     (8-3b)


               Diffusion  Force.  Particles  smaller  than  1  mm  diameter  tend  to  move
                irregularly  in  a  liquid  media  and  disperse  randomly.  This  phenomena  is
                called  the  Brownian notion.  The  diffusivity  of  fine  particles  undergoing
                a  Brownian  notion  is  given  by  Einstein  (McDowell-Boyer  et  al.,  1986):

                                                                            (8-4)

                The  diffusion  force  can  be  expressed  by  the  Peclet  number  as  the  ratio
                of  the  convection  velocity  to  the  average  Brownian  velocity  given  by
                (Ives,  1985).


                                                                            (8-5)
                         KT
                                                  ,-23
                where  TI = 3.1459...  and  K  =  1.38 x  10  is  Boltzmann's  constant.
               Hydrodynamic  Force.   Hydrodynamic  forces  are  the  fluid  shearing  and
               pressure  forces  (Wojtanowicz  et  al.,  1987,  1988).  Ives  (1985)  explains
               that  during  fluid  flow  secondary  circulation  flows  can  be  formed  around
               the  particles,  which  can  generate  out-of-balance  hydrodynamic  forces
                acting  on  the  particles  to  move  them  across  the  flow  field.  Ives  (1985)
                states  that  a  proper  dimensionless  group  rigorously  expressing  the
               hydrodynamic  force  is  not  available.  Ives  (1985)  points  out  that  the
               Reynolds  number  given  by:


                                                                            (8-6)
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