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RT

Example

Velocity fieldPressure

download example: aaRT.edp or return to 2D examples

verbosity=4;

mesh Th=square(10,10,[10*x,5*y]);
fespace Vh(Th,RT0);
fespace Rh(Th,RT0Ortho);
fespace Ph(Th,P0);

Vh [u1,u2],[v1,v2];
Rh [r1,r2];
Ph p,q; 
cout << 1. / 2. << endl;
[u1,u2]= [1+x,2+y];
[r1,r2]= [-2-y,1+x];
//  verification of the finite function 
cout << "   [u1,u2]  = ["<< u1(1,2) << "," << u2(1,2) << "]  == [2,4] \n";
cout << "dx([u1,u2]) = ["<< dx(u1)(1,2) << "," << dx(u2)(1,2) << "]  == [1,0] \n";
cout << "dy([u1,u2]) = ["<< dy(u1)(1,2) << "," << dy(u2)(1,2) << "]  == [0,1] \n";
//  verification of the finite function 
cout << "   [r1,r2]  = ["<< r1(1,2) << "," << r2(1,2) << "]  == [-4,2] \n";
cout << "dx([r1,r2]) = ["<< dx(r1)(1,2) << "," << dx(r2)(1,2) << "]  == [0,1] \n";
cout << "dy([r1,r2]) = ["<< dy(r1)(1,2) << "," << dy(r2)(1,2) << "]  == [-1,0] \n";

plot(u1,u2,[u1,u2],wait=1);
plot(r1,r2,[r1,r2],wait=1);

problem Probem1(u1,u2,v1,v2,solver=LU,eps=-1.0e-6) =
    int2d(Th)(  u1*v1+u2*v2 + dx(u1)*v1+ u2*dx(v2)) 
  + int2d(Th) ( x*v1+y*v2 + v1 + y*dx(v2) ) 

  + on(1,2,3,4,u1=-x,u2=-y)  ;

problem Probem2(p,q,solver=LU,eps=-1.0e-6) =
    int2d(Th)(  p*q ) + int2d(Th) ( q ) 
  ;

cout << " probem 1 \n";
Probem1; // solve problem1
cout << " probem 2 \n";
Probem2; // solve problem2

plot(u1,u2,[u1,u2], wait=1,cmm="Ver");

problem lap(u1,u2,p,v1,v2,q,solver=LU,eps=1.0e-30) =
    int2d(Th)( p*q*1e-10+ u1*v1 + u2*v2 + p*(dx(v1)+dy(v2)) + (dx(u1)+dy(u2))*q )
    + int2d(Th) ( q)
   + int1d(Th)( (v1*N.x +v2*N.y)/-2);

cout << " lap RT \n";

lap;

plot([u1,u2],wait=1,cmm="Ver [u1,u2]"); 

plot(p,fill=1,wait=1,cmm="Ver p");    

cout << " int2d(Th)(p-0.5) " << int2d(Th)(p-0.5) << "  == 0 " << endl;

cout << " int2d(Th)(x+y) " << int2d(Th)(x+y) << " ==  " << (10*5)*(10+5)/2 <<  endl;
cout << " -------------\n\n " << endl;

return to 2D examples

Page last modified on June 27, 2018, at 03:34 PM