thermic-fast.edp

FreeFem++可以生成高质量的有限元网格。可以用于流体力学

// file thermal-fast.edp    same problem than thermal.edp

func fu0 =10+90*x/6;
func k = 1.8*(y<0.5)+0.2;
real ue = 25. , alpha=0.25, T=5, dt=0.1 ;

mesh Th=square(30,5,[6*x,y]);
fespace Vh(Th,P1);

Vh u0=fu0,u=u0;

varf vthermic (u,v)= int2d(Th)(u*v/dt + k*(dx(u) * dx(v) + dy(u) * dy(v)))  
  +  int1d(Th,1,3)(alpha*u*v)
  + on(2,4,u=1); 

varf vthermic0(u,v) =   int1d(Th,1,3)(alpha*ue*v);

varf vMass (u,v)= int2d(Th)( u*v/dt)  + on(2,4,u=1);

real tgv = 1e30;
matrix A= vthermic(Vh,Vh,tgv=tgv,solver=CG);
matrix M= vMass(Vh,Vh);


real[int]  b0  = vthermic0(0,Vh); // constant part of the RHS 
real[int]  bcn = vthermic(0,Vh); //  tgv on Dirichlet boundary  node  ( !=0 )
// we have for the node $i$ : $i\in \Gamma_{24}  \quad \Leftrightarrow \quad bcn[i] \ne 0 $ 
real[int]  bcl=tgv*u0[]; //  the Dirichlet boundary condition part 


ofstream ff("thermic.dat");
for(real t=0;t<T;t+=dt){
    real[int] b = b0 ; // for  the  RHS
    b += M*u[]; //  add the the time dependant part
    // to lock boundary 2,4 part:
    b = bcn ? bcl  : b ; // do $\forall i$:  b[i] =  bcn[i] ? bcl[i] : b[i]  ;      
    u[] = A^-1*b;    
    ff<< t << " " << u(3,0.5) <<endl;
    plot(u);
}
for(int i=0;i<20;i++) 
  cout<<dy(u)(6.0*i/20.0,0.9)<<endl;
plot(u,fill=true,wait=1,ps="thermic.eps");