Page 332 - Process Modelling and Simulation With Finite Element Methods
P. 332

Electrokinetic Flow                 319
          Now for our clarifications of this list in light of our example:

                 Strong  and  weak  constraints  should  not  be  mixed  on  adjacent
                 boundaries.  But Neurnann boundary conditions do not count as strong
                 (automatically weak), so  they can  be  mixed  on adjacent boundaries.
                 Our “electrodes”  were surrounded  by  Neumann  BC  segments with no
                 apparent difficulty.  This is consistent with the policy that Neumann
                 boundary conditions do not count as a constraint for the purposes
                 of a weak boundary constraint.
                 You must always have a constraint on boundaries when you enable the
                 weak boundary constraint.  We used three zero boundary conditions for
                 boundaries  bnds  5,6, 21  and  still  got the  correct answer.  So even  a
                 homogeneous constraint still counts as a constraint.

          9.3  Electrokinetic Flow

          9.3.1  Background
          Electrokinetic flow is produced by the interaction of an electric field and charged
          (ion) species in a liquid.  Two distinct interactions are present: the electric force
          on the liquid in the double layer region adjacent to wall surfaces where there is a
          net charge and the movement of individual ions in the bulk of the flow (outside
          the  double layer  region)  where  there  is generally  no  net  charge.  The double
          layer may be taken as infinitesimal for channel sizes of interest (say greater than
          about  1 pm) and  its effect  on the  flow is then  equivalent  (MacInnes,  2002) to
          application  of  the  boundary  conditions  for velocity,  u;, electric  field,  4, and
          mass fraction of a relevant chemical species,  Y :





          where  ni is the unit normal vector to the wall surface.
             The  system  of  equations  that  must  be  solved  comprises  the  momentum
          equation, the continuity of mass equation,  the charge continuity equation  and  a
          species equation.  A simplest case may be expressed in non-dimensional form by
             Momentum transport and continuity (Navier-Stokes):
   327   328   329   330   331   332   333   334   335   336   337