FEATool Multiphysics
v1.17.2
Finite Element Analysis Toolbox
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EX_DARCY1 Darcy's law for a porous packed bed reactor.
[ FEA, OUT ] = EX_DARCY1( VARARGIN ) Example using Darcy's law to study the cross sectional flow in the porous material of a packed bed reactor.
Accepts the following property/value pairs.
Input Value/{Default} Description ----------------------------------------------------------------------------------- hmax scalar {2e-4} Grid size sfun string {sflag2} Shape function for pressure iplot scalar 0/{1} Plot solution (=1) . Output Value/(Size) Description ----------------------------------------------------------------------------------- fea struct Problem definition struct out struct Output struct
cOptDef = { 'hmax', 2e-4; 'sfun', 'sflag2'; 'iplot', 1; 'tol', 5e-3; 'fid', 1 }; [got,opt] = parseopt(cOptDef,varargin{:}); fid = opt.fid; % Model constants. p0 = 1e5; % Reference pressure. kap = 1.2e-13; % Permeability. eta = 1.6e-5; % Viscosity. M = 16e-3; % Molar mass. R = 8.32; % Ideal gas constant. T = 344; % Temperature. % Geometry and grid generation. fea.sdim = { 'x' 'y' }; fea.geom.objects = { gobj_polygon([0 2.3e-3 2.3e-3 2.3e-3 2.3e-3 0 0 0 0; -6e-3 -6e-3 -5e-3 -4e-3 6e-3 6e-3 5e-3 3.5e-3 -6e-3]') }; fea.grid = gridgen( fea, 'hmax', opt.hmax, 'fid', opt.fid ); % Problem definition. fea = addphys( fea, @darcyslaw ); % Add Darcy's law physics mode. % Modify equation kappa -> p*kappa (introduce nonlinearity in equation, not coefficient). fea.phys.dl.eqn.seqn = strrep(fea.phys.dl.eqn.seqn,'kap_dl','p*kap_dl'); fea.phys.dl.eqn.coef{2,end} = { kap*M/R/T }; fea.phys.dl.eqn.coef{3,end} = { eta }; fea.phys.dl.sfun = { opt.sfun }; % Set pressure 1.7 times higher on the inflow. i_inflow = 7; i_outflow = 3; fea.phys.dl.bdr.sel(i_inflow) = 1; fea.phys.dl.bdr.sel(i_outflow) = 1; fea.phys.dl.bdr.coef{1,end}{1,i_inflow} = p0*1.7; fea.phys.dl.bdr.coef{1,end}{1,i_outflow} = p0; % Parse and solve problem. fea = parsephys( fea ); fea = parseprob( fea ); % Check and parse problem struct. fea.sol.u = solvestat( fea, 'init', {p0}, 'fid', opt.fid ); % Call to stationary solver. % Postprocessing. s_velmag = ['sqrt(((',num2str(-kap/eta),')^2)*(px^2+py^2))']; if( opt.iplot>0 ) figure postplot( fea, 'surfexpr', ['min(0.1,',s_velmag,')'], ... 'arrowexpr', {[num2str(-kap/eta),'*px'] [num2str(-kap/eta),'*py']} ) title( 'Velocity field' ) end % Error checking. u_vel = intsubd( s_velmag, fea ); p_in = intbdr( 'p', fea, i_inflow ); p_out = intbdr( 'p', fea, i_outflow ); out.err = [ abs(u_vel-1.205e-6)/1.205e-6; abs(p_in-255)/255 ; abs(p_out-100)/100 ]; out.pass = all( out.err < opt.tol ); if ( nargout==0 ) clear fea out end