FEATool Multiphysics  v1.13
Finite Element Analysis Toolbox
ex_poisson8.m File Reference

Description

EX_POISSON8 2D Poisson equation example on a unit square with integral constraint.

[ FEA, OUT ] = EX_POISSON8( VARARGIN ) Poisson equation on a [0..1]^2 unit square with all Neumann boundary conditions, integral constraint, and exponential source term.

Ref. https://fenicsproject.org/docs/dolfin/latest/python/demos/neumann-poisson/demo_neumann-poisson.py.html

Input       Value/{Default}        Description
-----------------------------------------------------------------------------------
igrid       scalar 1/{0}           Cell type (0=quadrilaterals, 1=triangles)
hmax        scalar {0.1}           Max grid cell size
sfun        string {sflag1}        Shape function
ischeme     scalar {0}             Time stepping scheme (0 = stationary)
solver      string fenics/{} Use   FEniCS or default solver
iplot       scalar 0/{1}           Plot solution (=1)
                                                                                  .
Output      Value/(Size)           Description
-----------------------------------------------------------------------------------
fea         struct                 Problem definition struct
out         struct                 Output struct

Code listing

 cOptDef = { ...
             'igrid',    0;
             'hmax',     0.1;
             'sfun',     'sflag1';
             'ischeme',  0;
             'solver',   '';
             'iplot',    1;
             'tol',      0.02;
             'fid',      1 };
 [got,opt] = parseopt(cOptDef,varargin{:});
 fid       = opt.fid;


% Geometry definition.
 fea.geom.objects = { gobj_rectangle() };


% Grid generation.
 switch( opt.igrid )
   case -1
     fea.grid = rectgrid(round(1/opt.hmax),round(1/opt.hmax),[0 1;0 1]);
     fea.grid = quad2tri(fea.grid);
   case 0
     fea.grid = rectgrid(round(1/opt.hmax),round(1/opt.hmax),[0 1;0 1]);
   case 1
     fea.grid = gridgen(fea,'hmax',opt.hmax,'fid',fid);
 end


% Problem definition.
 fea.sdim  = { 'x', 'y' };               % Coordinate names.

 fea = addphys(fea,@poisson);            % Add Poisson equation physics mode.
 fea.phys.poi.sfun = { opt.sfun };       % Set shape function.
 fea.phys.poi.eqn.coef{3,end}{1} = '10*exp(-((x-0.5)^2+(y-0.5)^2)/0.02)';
 fea.phys.poi.bdr.sel(:) = 2;
 [fea.phys.poi.bdr.coef{2,end}{:}] = deal('-sin(5*x)');
 fea = parsephys(fea);                   % Check and parse physics modes.

% Add integral constraint.
 constr.type = 'intsubd';
 constr.dvar = 'u';
 constr.expr = 0;
 fea.constr  = constr;


% Parse and solve problem.
 fea = parseprob( fea );               % Check and parse problem struct.
 if( strcmp(opt.solver,'fenics') )
   fea = fenics( fea, 'fid', fid, 'ischeme', opt.ischeme, 'tstep', 0.1, 'tmax', 1 );
 else
   if( opt.ischeme==0 )
     fea.sol.u = solvestat( fea, 'fid', fid );
   else
     fea.sol.u = solvetime( fea, 'fid', fid, 'ischeme', opt.ischeme, 'tstep', 0.1, 'tmax', 1 );
   end
 end


% Postprocessing.
 if( opt.iplot>0 )
   postplot( fea, 'surfexpr', 'u', 'surfhexpr', 'u' )
 end


% Error checking.
 [u_min,u_max] = minmaxsubd( 'u', fea );
 err = mean( [ abs(u_max-u_min-1.037)/1.037, ...
               intsubd( 'u', fea ), ...
               abs(fea.sol.u(end)-1.3007)/1.3007 ] );

 out.err  = err;
 out.tol  = opt.tol;
 out.pass = out.err<opt.tol;
 if( nargout==0 )
   clear fea out
 end