Page 126 - Process Modelling and Simulation With Finite Element Methods
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Multiphysics                      113


                                                               Max  8 09e-OC
                                 Contour  u2  (u2)
                                                                  10’~
                          I  I  I  I  I  I  I  I  I  I
                                                                 0 6016
              09                                                 1 204
              oa                                                 I  a06
                                                                 2 409
                                                                 3 01 1
              07                                                 3 613
                                                                 4 216
              06                                                 4 aia
                                                                 5 421
              05                                                 6 023
                                                                 6 625
              04                                                 7 228
                                                                 7 a3
              03                                                 a 432
                                                                 9 035
              02                                                 9 637
                                                                 10 24
              01                                                 10 a4
                                                                 11 44
                0                                                12 05
                  03-02-01  0  01 0203040506070a09  I  11 1213   Min  -0 00126
           Figure 3.1  Steady state streamlines of hot walUcold wall buoyancy driven convection for Ra=l.
         Buoyancy Driven Cavity Flow: Parametric Continuation
          Our solution strategy for the hot wallkold wall problem to reach Ra=50 was to
         build up elements of the solution piecemeal.  Were we to try to start at Ra=50
          directly, we would find that FEMLAB cannot find a solution.  Why not?  For a
          nonlinear problem, the initial condition may not be in the “basin  of  attraction”
          for the desired solution, so Newton’s Method could career far off.  For it to work
          well,  Newton’s  Method  must  start  near  a  solution.  For  instance,  the  initial
          solution  for hydrostatic  pressure and  velocity  noise for Ra=O  was  an  essential
          step.  As a fully linear problem, it was readily solvable.  It serves the important
         purpose  of  introducing  an  asymmetric  velocity  profile  (due  to  the  numerical
         noise  of  truncation  error).  This  permits  the  solution  for  Ra=l, which  is
          qualitatively  similar to  the Ra=O in that  it has  a circulation, though a massive
          change in  scale.  Even then,  though qualitatively  similar to  the Ra=l solution,
          Ra=50 was too far a leap from Ra=l to converge.  The notion of traversing the
          solution space to introduce various topological features consistent with the target
          solution so as to be in its basin of attraction is similar to the established concept
          of  parametric  continuation.   In  parametric  continuation,  one  restarts  the
          simulation with a parametric value close to that of the saved, converged solution.
         Because the  solution  at the new parameter values  is not  expected to be  much
          different  than  at the old parameter  values, the Newton  solver  should  converge
         rapidly.  This  methodology  only  fails  if  the  new  parameter  is  close  to  a
         bifurcation point - in which case multiple solutions are possible.  The Jacobian
          used by Newton’s Method is then very close to singular, so convergence may not
         be achieved.  Or if it is, which of the multiple solutions that is selected may not
         be a priori predictable.
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