Page 259 - Process Modelling and Simulation With Finite Element Methods
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246        Process Modelling and Simulation with Finite Element Methods


          FEMLAB.  Line integrals, integral  equations, and integro-differential equations
          are the target applications in applied mathematics.  These are all treatable with
          recourse to FEMLAB’s coupling variable capability.  Perhaps  that is reason to
          have titled this chapter “Extended multiphysics 11.”  The title selected, however,
          is  probably  more  descriptive.  As  ever,  we  target  illustrations  in  chemical
          engineering of  the  use  of  the  FEMLAB  features.  The most  important treated
          here  are  using  lidar  to  detect  position  and  spread  of  dense  gas  contaminant
         clouds, population balance equations which are exemplary of IDES, the inverse
          problem in electrical capacitance tomography, and the computation of non-local
          heat transfer in a fiber composite medium.

         Extended Multiphysics Revisited
         When  I  read  through  the  new  features  introduced  with  FEMLAB  2.2, I  must
          admit to being skeptical of extended multiphysics as something that I was likely
          to use.  Eventually,  the utility  of  scalar coupling variables  dawned on me, and
         provided  the  impetus  for  Chapter  4.  It  also  spawned  our  interest  in  a  new
          adventure  for  our  research  team,  modeling  microfluidics  networks.   Yet
          FEMLAB  provides  two  other  conceptual  constructs  for  coupling  variables  -
         extruded  and  projected  coupling  variables.  The examples  of  their  use  in the
         Model  Library are nearly  all  about postprocessing,  i.e. to  express  solutions in
         cross domain functionals to analyze particular features.
             Rarely,  however,  coupling  variables  (extruded  and  projection)  have  been
         incorporated  in  the model  and  solved  for simultaneously  with the independent
         field  variables.  Multi-domain, multiple scale, and multiple process models are
         not  common in engineering mathematics  and mathematical physics.  Typically,
         models  are  local  in  character  - conceived  of  as  a  set  of  (partial)  differential
         equations  and  boundary  and initial  conditions that  are well posed.  These are
         termed  continuum models.  Historically, this  development has been predicated
          on the use of  analysis techniques  that have some scope for treating this class of
          models  in  closed  form.  Computational  models,  even  in  situations  that  are
         treatable by  continuum methods,  are approximated by  discrete interaction  rules
         that need not be local. Smooth particle hydrodynamics  [l] and discrete element
         methods  [2]  are  growing  in  popularity,  but  older  methods  like  molecular
          dynamics simulations 131, Monte  Carlo methods  [4], microhydrodynamics [5],
         cellular automata [6] and exact numerical simulation in gadplasma dynamics [7]
         bridge  the  continuuddiscrete  system  gap  in  modelling  distributed  systems.
          Another  set  of  techniques  is  based  on  optimization  theory  to  satisfy  pde
         constraints - penalizing the degree to which constraints are not satisfied.  Mixed
         integer  nonlinear  programming  [8],  genetic  algorithms  [9]  and  genetic
         programming  [lo]  are  all  suitable  for  treating  models  of  mixed
         discrete/continuum  systems.  FEMLAB  was  formulated  with  a  strong  bias
         towards continuum systems with pde constraints.  Yet,  conceptually, extended
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