Page 260 - Process Modelling and Simulation With Finite Element Methods
P. 260

Coupling Variables Revisited            247

         multiphysics  is  not  an  afterthought  for  dealing  with  awkward  situations.  It
         permits  treating  discrete  systems  on  an  even  footing  with  continuum  systems
         characterized  not  only  by  pde  constraints,  but  by  integral  constraints  as  well.
         Essentially, coupling variables permit nonlocal and discrete modelling.
             In  sections  7.3  (scalar),  7.4  (projection)  and  7.5  (extrusion)  we  revisit
         coupling  variables  to  explore  FEMLAB  treatment  of  inverse  problems,  line
         integrals, and integralhtegro-differential  equations, respectively.
         Scalar Coupling Variables

         Undoubtedly,  scalar coupling variables are the conceptually easiest to grasp.  In
         chapter  4, scalar  coupling  variables  were used to link up a recycle  stream in a
         flowsheet  for  a  heterogeneous  chemical  reactor  - the  output  of  the  reactor,
          suitably  scaled,  re-enters  with  the  feed  stream.  An  abstract  0-D  element  in a
          second  geometry  was  created  for  the  purpose  of  modeling  a  buffer  tank  that
          achieved  the  algebraic  relationship  between  the  recycle  stream and the reactor
          outlet.  Very simply, a scalar coupling is a single value passed to the destination
          domain,  subdomain,  boundary,  or  edge,  where  it  is  used  anywhere  in  the
          description  of  the  domain  FEM  residuals.  The  scalar  coupling  variable  is
          created  by an integration  on the source domain.  Since in our example,  sources
          were  0-D  (endpoints  or  the  single  element  construct),  the  integrations  were
          trivially  the  same  as  the  integrand.  Furthermore,  that  buffer  tank  model  was
          artificial since the recycle relations could have been more readily incorporated in
          a weak boundary constraint without recourse to the second domain. So we have
         yet to see an example of scalar coupling  variables where the  source integration
          was  non-trivial  and  the  coupling  itself  essential.  In  the  next  subsection,  we
          tackle an inverse problem  where coupling is essential and intricate.  An inverse
          problem has the connotation  that there is an associated forward problem that is
          well-posed,  but  that  the  inverse  problem  is  ill-posed.  Our  selected  inverse
          problem is a tomographic inversion for electrical capacitance tomography.

          Electrical Capacitance Tomography
          Process  tomography  has matured  as an engineering  science in the past  decade.
          One of  the  most  common  configurations  is electrical  capacitance  tomography,
          frequently  used  for  imaging  processes  with  multiphase  flows  in  cylindrical
          pipelines.  Sensing of  multiphase  pipeline  flows  with  information  about  the
          distributed  flow of dispersed  phases can be crucial to tight control  of chemical
          and processing  unit  operations.  Non-invasive  and non-intrusive  measurements
          of  two-phase  flow  are  notoriously  difficult  to  obtain.  The  difficulty  is  often
          exacerbated  by  the  highly  time-varying  flows  some  times  encountered  in  gas-
          liquid  flows  in  the  oil and  gas production  industry.  Accurate  measurements  of
          transients in the flow and instantaneous  phase distributions cannot be achieved.
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