ex_poisson2.m File Reference

Description

EX_POISSON2 2D Poisson equation example on a circle.

[ FEA, OUT ] = EX_POISSON2( VARARGIN ) Poisson equation on a circle with source term 1 and exact solution u=(1-r^2)/4. Accepts the following property/value pairs.

Input       Value/{Default}        Description
-----------------------------------------------------------------------------------
radi        scalar {1}             Radius of circle
hmax        scalar {0.1}           Max grid cell size
sfun        string {sflag1}        Shape function
iphys       scalar 0/{1}           Use physics mode to define problem    (=1)
                                   or directly define fea.eqn/bdr fields (=0)
igrid       scalar -1/{0}          Cell type (0>=triangles, 0<quadrilaterals)
iplot       scalar 0/{1}           Plot solution (=1)
                                                                                  .
Output      Value/(Size)           Description
-----------------------------------------------------------------------------------
fea         struct                 Problem definition struct
out         struct                 Output struct

Code listing

 cOptDef = { ...
   'radi',     1; ...
   'hmax',     0.1; ...
   'refsol',   '(1-(x^2+y^2))/4'; ...
   'fsrc',     '1'; ...
   'sfun',     'sflag1'; ...
   'iphys',    1; ...
   'icub',     2; ...
   'iplot',    1; ...
   'igrid',    1; ...
   'tol',      1e-1;
   'fid',      1 };
 [got,opt] = parseopt(cOptDef,varargin{:});
 fid       = opt.fid;


% Geometry definition.
 gobj = gobj_circle( [0 0], opt.radi );
 fea.geom.objects = { gobj };


% Grid generation.
 if( opt.igrid<0 )
   fea.grid = circgrid(4,3);
   if( opt.igrid==-2 )
     fea.grid = quad2tri( fea.grid );
   end
 else
   fea.grid = gridgen(fea,'hmax',opt.hmax,'fid',fid,'dprim',false);
 end
 n_bdr = max(fea.grid.b(3,:));        % Number of boundaries.


% Problem definition.
 fea.sdim = { 'x' 'y' };                % Coordinate names.
 if ( opt.iphys==1 )

   fea = addphys(fea,@poisson);          % Add Poisson equation physics mode.
   fea.phys.poi.sfun = { opt.sfun };     % Set shape function.
   fea.phys.poi.eqn.coef{3,4} = { opt.fsrc };   % Set source term coefficient.
   fea.phys.poi.bdr.coef{1,end} = repmat({opt.refsol},1,n_bdr);   % Set Dirichlet boundary coefficient to reference solution.
%  fea.phys.poi.eqn
   fea = parsephys(fea);                 % Check and parse physics modes.
   if( any(strcmp(opt.sfun,{'sf_tri_H3','sf_quad_H3'})) )   % Prescribed derivatives at end points for Hermite elements.
     fea.bdr.d = {{ opt.refsol opt.refsol opt.refsol opt.refsol ;
                    '-x/2' '-x/2' '-x/2' '-x/2' ;
                    '-y/2' '-y/2' '-y/2' '-y/2' }};
   end

 else

   fea.dvar  = { 'u' };                  % Dependent variable name.
   fea.sfun  = { opt.sfun  };            % Shape function.

% Define equation system.
   fea.eqn.a.form = { [2 3;2 3] };       % First row indicates test function space   (2=x-derivative + 3=y-derivative),
% second row indicates trial function space (2=x-derivative + 3=y-derivative).
   fea.eqn.a.coef = { 1 };               % Coefficient used in assembling stiffness matrix.

   fea.eqn.f.form = { 1 };               % Test function space to evaluate in right hand side (1=function values).
   fea.eqn.f.coef = { opt.fsrc };        % Coefficient used in right hand side.

% Define boundary conditions.
   if( any(strcmp(opt.sfun,{'sf_tri_H3','sf_quad_H3'})) )   % Prescribed derivatives at end points for Hermite elements.
     fea.bdr.d = {{ opt.refsol opt.refsol opt.refsol opt.refsol ;
                    '-x/2' '-x/2' '-x/2' '-x/2' ;
                    '-y/2' '-y/2' '-y/2' '-y/2' }};
   else
     fea.bdr.d     = cell(1,n_bdr);
    [fea.bdr.d{:}] = deal(opt.refsol);   % Assign reference solution to all boundaries (Dirichlet).
   end

   fea.bdr.n     = cell(1,n_bdr);        % No Neumann boundaries ('fea.bdr.n' empty).

 end


% Parse and solve problem.
 fea       = parseprob(fea);             % Check and parse problem struct.
 fea.sol.u = solvestat(fea,'fid',fid,'icub',opt.icub);   % Call to stationary solver.


% Postprocessing.
 s_err = ['abs(',opt.refsol,'-u)'];
 if ( opt.iplot>0 )
   figure
   subplot(3,1,1)
   postplot(fea,'surfexpr','u','axequal','on')
   title('Solution u')
   subplot(3,1,2)
   postplot(fea,'surfexpr',opt.refsol,'axequal','on')
   title('Exact solution')
   subplot(3,1,3)
   postplot(fea,'surfexpr',s_err,'axequal','on','evalstyle','exact')
   title('Error')
 end


% Error checking.
 if ( size(fea.grid.c,1)==4 )
   xi = [0;0];
 else
   xi = [1/3;1/3;1/3];
 end
 err = evalexpr0(s_err,xi,1,1:size(fea.grid.c,2),[],fea);
 ref = evalexpr0('u',xi,1,1:size(fea.grid.c,2),[],fea);
 err = sqrt(sum(err.^2)/sum(ref.^2));

 if( ~isempty(fid) )
   fprintf(fid,'\nL2 Error: %f\n',err)
   fprintf(fid,'\n\n')
 end


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