Page 340 - Process Modelling and Simulation With Finite Element Methods
P. 340

Electrokinetic Flow                 327

          they  contribute  to  the  stiffness  matrix  and  residual  instead  of  the  constraint
          matrices  [l].  So  one  expects  that  the  outlet  species  concentration,  though
          nonlinear, may be treated satisfactorily by the standard handling of  constraints.
          Very simply,  as a Neumann  condition,  it does not  count as a  weak  boundary
          constraint - it is naturally in FEM (see chapter 2) so it automatically is treated
          correctly.
          (2) Implementing constraints using derivatives
          In  FEMLAB  2.2  and  later,  the  derivatives  of  the  dependent  variables  are
          available also on the boundary. Constraints on only the tangential component of
          the derivative work when using standard constraints, whereas here it is necessary
          to  use  a  weak  constraint  to  be  able  to  handle  non-tangential  constraints  (the
          velocity BCs on the walls).

          Condition (3) is clearly satisfied, yet condition (2) is not violated with the caveat
          that  Neumann  constraints  do not  count.  We  should  not  need  to  use  a  weak
          boundary  constraint  on  the  outlet  boundary  (bnd  4)  for  the  species transport
          equation, we did not, and it works.  When we tried a weak boundary constraint,
          it failed.
          From (9.6), we defined for our species general mode



          as  the  straightforward  way  of  dealing  with  the  electrophoretic  term.
          Consequently, our boundary condition on the outlet takes the form

                                                                       (9.9)
          Equation (9.9) is a non-zero Neumann condition with regard to the flux I-.  But
          since Neumann  conditions do not  count as constraints, the standard BC works
          fine.
          Figure 9.5 shows convincingly that the expected value with uniform Y and phix
          on the outlet boundary is achieved by the model at all times.


          9.3.4  Links to physical boundaries

          Current  microchannel  devices  may  consist  of  many  distinct channel  segments
         joined  at  several  junctions.   Future  ones  may  well  comprise  hundreds  of
          segments joined  at a similar number of junctions.  Detailed  computation of  the
          flow  in  such  a  system  is  unlikely  to be feasible  for  some time  to  come and,
          indeed,  is  probably  not  desirable.  Rather,  an  approach  in  which  a  particular
         junction of interest or perhaps an evolving mixing zone such as that considered
          in MacInnes et al. (2003) is probably appropriate.  The approach emerges from
   335   336   337   338   339   340   341   342   343   344   345