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3.1  FLOW AT THE MICRO LEVEL                                          45


             Laminar flow  (Re  < Rel).  Deviations from  the Darcy's law for  very small
         values of the flow rate are usually explained by the formation of the bounded fluid
         layers on  the surfaces of pores  (capillaries).  These layers can fill  a  good  part of
         the pore space and can decrease the permeability of the medium significantly, up
         to the total termination of the flow  [50].
            Results  of a  series  of experiments on  the  flow  in  homogeneous  media under
         small pressure gradients can  be  found  in  [54].  Present the empirical dependence
         that describes these results  [50]

                                                                            (3.12)

            Here  Go  is  the  minimal  pressure  gradient,  when  the  flow  begins;  Ko  is  the
         permeability for pressure gradients G » G0 ,  where Darcy's law is valid.  Assuming
         that the pore space of a homogeneous medium consists of capillaries with radii r
         close to the average radius, after substitutions




         in  (3.12)  and  some  transformations,  we  can obtain  the following  correlation  be-
         tween the pressure gradient in  the capillary and the value of flow  in it

                                                                            (3.13)

            Here  g0 ( r)  has  the  meaning  of the  minimal  pressure  gradient in  a  capillary.
         When qf » r 4 go(r)  we get the well-known Poiseuille's formula



            Transient regime of flow (Re1  :$Re:$ Re2).  The flow in this domain is inter-
         mediate from laminar and turbulent (Nikuradze's saddle [12]).  It does not depend
         on the roughness of the capillary and can be described  by  a certain approximate
         formula.  The  latter is  obtained  after studying  the  plots  of hydraulic  resistance
         against the Reynolds number

                                                                           (3.14)

            Here i =  2 + 4,  j  =  4 + 8,  Km is a dimensioned constant which depends on  PI
         and JL.
            Turbulent flow (Re > Re2).  For a rough capillary, the following approximate
         formula can be used
                                                                           (3.15)
            Here s =  1.8 +  2.5;  h =  4 +  6,  Kt is a dimensioned constant which depends on
         p  f, JL,  and the degree and the type of roughness.
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