ex16p.cpp

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//                       MFEM Example 16 - Parallel Version
//
// Compile with: make ex16p
//
// Sample runs:  mpirun -np 4 ex16p
//               mpirun -np 4 ex16p -m ../data/inline-tri.mesh
//               mpirun -np 4 ex16p -m ../data/disc-nurbs.mesh -tf 2
//               mpirun -np 4 ex16p -s 1 -a 0.0 -k 1.0
//               mpirun -np 4 ex16p -s 2 -a 1.0 -k 0.0
//               mpirun -np 8 ex16p -s 3 -a 0.5 -k 0.5 -o 4
//               mpirun -np 4 ex16p -s 14 -dt 1.0e-4 -tf 4.0e-2 -vs 40
//               mpirun -np 16 ex16p -m ../data/fichera-q2.mesh
//               mpirun -np 16 ex16p -m ../data/fichera-mixed.mesh
//               mpirun -np 16 ex16p -m ../data/escher-p2.mesh
//               mpirun -np 8 ex16p -m ../data/beam-tet.mesh -tf 10 -dt 0.1
//               mpirun -np 4 ex16p -m ../data/amr-quad.mesh -o 4 -rs 0 -rp 0
//               mpirun -np 4 ex16p -m ../data/amr-hex.mesh -o 2 -rs 0 -rp 0
//
// Description:  This example solves a time dependent nonlinear heat equation
//               problem of the form du/dt = C(u), with a non-linear diffusion
//               operator C(u) = \nabla \cdot (\kappa + \alpha u) \nabla u.
//
//               The example demonstrates the use of nonlinear operators (the
//               class ConductionOperator defining C(u)), as well as their
//               implicit time integration. Note that implementing the method
//               ConductionOperator::ImplicitSolve is the only requirement for
//               high-order implicit (SDIRK) time integration. In this example,
//               the diffusion operator is linearized by evaluating with the
//               lagged solution from the previous timestep, so there is only
//               a linear solve. Optional saving with ADIOS2
//               (adios2.readthedocs.io) is also illustrated.
//
//               We recommend viewing examples 2, 9 and 10 before viewing this
//               example.
 
#include "mfem.hpp"
#include <fstream>
#include <iostream>
 
using namespace std;
using namespace mfem;
 
/** After spatial discretization, the conduction model can be written as:
 *
 *     du/dt = M^{-1}(-Ku)
 *
 *  where u is the vector representing the temperature, M is the mass matrix,
 *  and K is the diffusion operator with diffusivity depending on u:
 *  (\kappa + \alpha u).
 *
 *  Class ConductionOperator represents the right-hand side of the above ODE.
 */
class ConductionOperator : public TimeDependentOperator
{
protected:
   ParFiniteElementSpace &fespace;
   Array<int> ess_tdof_list; // this list remains empty for pure Neumann b.c.
 
   ParBilinearForm *M;
   ParBilinearForm *K;
 
   HypreParMatrix Mmat;
   HypreParMatrix Kmat;
   HypreParMatrix *T; // T = M + dt K
   real_t current_dt;
 
   CGSolver M_solver;    // Krylov solver for inverting the mass matrix M
   HypreSmoother M_prec; // Preconditioner for the mass matrix M
 
   CGSolver T_solver;    // Implicit solver for T = M + dt K
   HypreSmoother T_prec; // Preconditioner for the implicit solver
 
   real_t alpha, kappa;
 
   mutable Vector z; // auxiliary vector
 
public:
   ConductionOperator(ParFiniteElementSpace &f, real_t alpha, real_t kappa,
                      const Vector &u);
 
   virtual void Mult(const Vector &u, Vector &du_dt) const;
   /** Solve the Backward-Euler equation: k = f(u + dt*k, t), for the unknown k.
       This is the only requirement for high-order SDIRK implicit integration.*/
   virtual void ImplicitSolve(const real_t dt, const Vector &u, Vector &k);
 
   /// Update the diffusion BilinearForm K using the given true-dof vector `u`.
   void SetParameters(const Vector &u);
 
   virtual ~ConductionOperator();
};
 
real_t InitialTemperature(const Vector &x);
 
int main(int argc, char *argv[])
{
   // 1. Initialize MPI and HYPRE.
   Mpi::Init(argc, argv);
   int num_procs = Mpi::WorldSize();
   int myid = Mpi::WorldRank();
   Hypre::Init();
 
   // 2. Parse command-line options.
   const char *mesh_file = "../data/star.mesh";
   int ser_ref_levels = 2;
   int par_ref_levels = 1;
   int order = 2;
   int ode_solver_type = 3;
   real_t t_final = 0.5;
   real_t dt = 1.0e-2;
   real_t alpha = 1.0e-2;
   real_t kappa = 0.5;
   bool visualization = true;
   bool visit = false;
   int vis_steps = 5;
   bool adios2 = false;
 
   int precision = 8;
   cout.precision(precision);
 
   OptionsParser args(argc, argv);
   args.AddOption(&mesh_file, "-m", "--mesh",
                  "Mesh file to use.");
   args.AddOption(&ser_ref_levels, "-rs", "--refine-serial",
                  "Number of times to refine the mesh uniformly in serial.");
   args.AddOption(&par_ref_levels, "-rp", "--refine-parallel",
                  "Number of times to refine the mesh uniformly in parallel.");
   args.AddOption(&order, "-o", "--order",
                  "Order (degree) of the finite elements.");
   args.AddOption(&ode_solver_type, "-s", "--ode-solver",
                  "ODE solver: 1 - Backward Euler, 2 - SDIRK2, 3 - SDIRK3,\n\t"
                  "\t   11 - Forward Euler, 12 - RK2, 13 - RK3 SSP, 14 - RK4.");
   args.AddOption(&t_final, "-tf", "--t-final",
                  "Final time; start time is 0.");
   args.AddOption(&dt, "-dt", "--time-step",
                  "Time step.");
   args.AddOption(&alpha, "-a", "--alpha",
                  "Alpha coefficient.");
   args.AddOption(&kappa, "-k", "--kappa",
                  "Kappa coefficient offset.");
   args.AddOption(&visualization, "-vis", "--visualization", "-no-vis",
                  "--no-visualization",
                  "Enable or disable GLVis visualization.");
   args.AddOption(&visit, "-visit", "--visit-datafiles", "-no-visit",
                  "--no-visit-datafiles",
                  "Save data files for VisIt (visit.llnl.gov) visualization.");
   args.AddOption(&vis_steps, "-vs", "--visualization-steps",
                  "Visualize every n-th timestep.");
   args.AddOption(&adios2, "-adios2", "--adios2-streams", "-no-adios2",
                  "--no-adios2-streams",
                  "Save data using adios2 streams.");
   args.Parse();
   if (!args.Good())
   {
      args.PrintUsage(cout);
      return 1;
   }
 
   if (myid == 0)
   {
      args.PrintOptions(cout);
   }
 
   // 3. Read the serial mesh from the given mesh file on all processors. We can
   //    handle triangular, quadrilateral, tetrahedral and hexahedral meshes
   //    with the same code.
   Mesh *mesh = new Mesh(mesh_file, 1, 1);
   int dim = mesh->Dimension();
 
   // 4. Define the ODE solver used for time integration. Several implicit
   //    singly diagonal implicit Runge-Kutta (SDIRK) methods, as well as
   //    explicit Runge-Kutta methods are available.
   ODESolver *ode_solver;
   switch (ode_solver_type)
   {
      // Implicit L-stable methods
      case 1:  ode_solver = new BackwardEulerSolver; break;
      case 2:  ode_solver = new SDIRK23Solver(2); break;
      case 3:  ode_solver = new SDIRK33Solver; break;
      // Explicit methods
      case 11: ode_solver = new ForwardEulerSolver; break;
      case 12: ode_solver = new RK2Solver(0.5); break; // midpoint method
      case 13: ode_solver = new RK3SSPSolver; break;
      case 14: ode_solver = new RK4Solver; break;
      case 15: ode_solver = new GeneralizedAlphaSolver(0.5); break;
      // Implicit A-stable methods (not L-stable)
      case 22: ode_solver = new ImplicitMidpointSolver; break;
      case 23: ode_solver = new SDIRK23Solver; break;
      case 24: ode_solver = new SDIRK34Solver; break;
      default:
         cout << "Unknown ODE solver type: " << ode_solver_type << '\n';
         delete mesh;
         return 3;
   }
 
   // 5. Refine the mesh in serial to increase the resolution. In this example
   //    we do 'ser_ref_levels' of uniform refinement, where 'ser_ref_levels' is
   //    a command-line parameter.
   for (int lev = 0; lev < ser_ref_levels; lev++)
   {
      mesh->UniformRefinement();
   }
 
   // 6. Define a parallel mesh by a partitioning of the serial mesh. Refine
   //    this mesh further in parallel to increase the resolution. Once the
   //    parallel mesh is defined, the serial mesh can be deleted.
   ParMesh *pmesh = new ParMesh(MPI_COMM_WORLD, *mesh);
   delete mesh;
   for (int lev = 0; lev < par_ref_levels; lev++)
   {
      pmesh->UniformRefinement();
   }
 
   // 7. Define the vector finite element space representing the current and the
   //    initial temperature, u_ref.
   H1_FECollection fe_coll(order, dim);
   ParFiniteElementSpace fespace(pmesh, &fe_coll);
 
   HYPRE_BigInt fe_size = fespace.GlobalTrueVSize();
   if (myid == 0)
   {
      cout << "Number of temperature unknowns: " << fe_size << endl;
   }
 
   ParGridFunction u_gf(&fespace);
 
   // 8. Set the initial conditions for u. All boundaries are considered
   //    natural.
   FunctionCoefficient u_0(InitialTemperature);
   u_gf.ProjectCoefficient(u_0);
   Vector u;
   u_gf.GetTrueDofs(u);
 
   // 9. Initialize the conduction operator and the VisIt visualization.
   ConductionOperator oper(fespace, alpha, kappa, u);
 
   u_gf.SetFromTrueDofs(u);
   {
      ostringstream mesh_name, sol_name;
      mesh_name << "ex16-mesh." << setfill('0') << setw(6) << myid;
      sol_name << "ex16-init." << setfill('0') << setw(6) << myid;
      ofstream omesh(mesh_name.str().c_str());
      omesh.precision(precision);
      pmesh->Print(omesh);
      ofstream osol(sol_name.str().c_str());
      osol.precision(precision);
      u_gf.Save(osol);
   }
 
   VisItDataCollection visit_dc("Example16-Parallel", pmesh);
   visit_dc.RegisterField("temperature", &u_gf);
   if (visit)
   {
      visit_dc.SetCycle(0);
      visit_dc.SetTime(0.0);
      visit_dc.Save();
   }
 
   // Optionally output a BP (binary pack) file using ADIOS2. This can be
   // visualized with the ParaView VTX reader.
#ifdef MFEM_USE_ADIOS2
   ADIOS2DataCollection* adios2_dc = NULL;
   if (adios2)
   {
      std::string postfix(mesh_file);
      postfix.erase(0, std::string("../data/").size() );
      postfix += "_o" + std::to_string(order);
      postfix += "_solver" + std::to_string(ode_solver_type);
      const std::string collection_name = "ex16-p-" + postfix + ".bp";
 
      adios2_dc = new ADIOS2DataCollection(MPI_COMM_WORLD, collection_name, pmesh);
      adios2_dc->SetParameter("SubStreams", std::to_string(num_procs/2) );
      adios2_dc->RegisterField("temperature", &u_gf);
      adios2_dc->SetCycle(0);
      adios2_dc->SetTime(0.0);
      adios2_dc->Save();
   }
#endif
 
   socketstream sout;
   if (visualization)
   {
      char vishost[] = "localhost";
      int  visport   = 19916;
      sout.open(vishost, visport);
      sout << "parallel " << num_procs << " " << myid << endl;
      int good = sout.good(), all_good;
      MPI_Allreduce(&good, &all_good, 1, MPI_INT, MPI_MIN, pmesh->GetComm());
      if (!all_good)
      {
         sout.close();
         visualization = false;
         if (myid == 0)
         {
            cout << "Unable to connect to GLVis server at "
                 << vishost << ':' << visport << endl;
            cout << "GLVis visualization disabled.\n";
         }
      }
      else
      {
         sout.precision(precision);
         sout << "solution\n" << *pmesh << u_gf;
         sout << "pause\n";
         sout << flush;
         if (myid == 0)
         {
            cout << "GLVis visualization paused."
                 << " Press space (in the GLVis window) to resume it.\n";
         }
      }
   }
 
   // 10. Perform time-integration (looping over the time iterations, ti, with a
   //     time-step dt).
   ode_solver->Init(oper);
   real_t t = 0.0;
 
   bool last_step = false;
   for (int ti = 1; !last_step; ti++)
   {
      if (t + dt >= t_final - dt/2)
      {
         last_step = true;
      }
 
      ode_solver->Step(u, t, dt);
 
      if (last_step || (ti % vis_steps) == 0)
      {
         if (myid == 0)
         {
            cout << "step " << ti << ", t = " << t << endl;
         }
 
         u_gf.SetFromTrueDofs(u);
         if (visualization)
         {
            sout << "parallel " << num_procs << " " << myid << "\n";
            sout << "solution\n" << *pmesh << u_gf << flush;
         }
 
         if (visit)
         {
            visit_dc.SetCycle(ti);
            visit_dc.SetTime(t);
            visit_dc.Save();
         }
 
#ifdef MFEM_USE_ADIOS2
         if (adios2)
         {
            adios2_dc->SetCycle(ti);
            adios2_dc->SetTime(t);
            adios2_dc->Save();
         }
#endif
      }
      oper.SetParameters(u);
   }
 
#ifdef MFEM_USE_ADIOS2
   if (adios2)
   {
      delete adios2_dc;
   }
#endif
 
   // 11. Save the final solution in parallel. This output can be viewed later
   //     using GLVis: "glvis -np <np> -m ex16-mesh -g ex16-final".
   {
      ostringstream sol_name;
      sol_name << "ex16-final." << setfill('0') << setw(6) << myid;
      ofstream osol(sol_name.str().c_str());
      osol.precision(precision);
      u_gf.Save(osol);
   }
 
   // 12. Free the used memory.
   delete ode_solver;
   delete pmesh;
 
   return 0;
}
 
ConductionOperator::ConductionOperator(ParFiniteElementSpace &f, real_t al,
                                       real_t kap, const Vector &u)
   : TimeDependentOperator(f.GetTrueVSize(), (real_t) 0.0), fespace(f),
     M(NULL), K(NULL), T(NULL), current_dt(0.0),
     M_solver(f.GetComm()), T_solver(f.GetComm()), z(height)
{
   const real_t rel_tol = 1e-8;
 
   M = new ParBilinearForm(&fespace);
   M->AddDomainIntegrator(new MassIntegrator());
   M->Assemble(0); // keep sparsity pattern of M and K the same
   M->FormSystemMatrix(ess_tdof_list, Mmat);
 
   M_solver.iterative_mode = false;
   M_solver.SetRelTol(rel_tol);
   M_solver.SetAbsTol(0.0);
   M_solver.SetMaxIter(100);
   M_solver.SetPrintLevel(0);
   M_prec.SetType(HypreSmoother::Jacobi);
   M_solver.SetPreconditioner(M_prec);
   M_solver.SetOperator(Mmat);
 
   alpha = al;
   kappa = kap;
 
   T_solver.iterative_mode = false;
   T_solver.SetRelTol(rel_tol);
   T_solver.SetAbsTol(0.0);
   T_solver.SetMaxIter(100);
   T_solver.SetPrintLevel(0);
   T_solver.SetPreconditioner(T_prec);
 
   SetParameters(u);
}
 
void ConductionOperator::Mult(const Vector &u, Vector &du_dt) const
{
   // Compute:
   //    du_dt = M^{-1}*-Ku
   // for du_dt, where K is linearized by using u from the previous timestep
   Kmat.Mult(u, z);
   z.Neg(); // z = -z
   M_solver.Mult(z, du_dt);
}
 
void ConductionOperator::ImplicitSolve(const real_t dt,
                                       const Vector &u, Vector &du_dt)
{
   // Solve the equation:
   //    du_dt = M^{-1}*[-K(u + dt*du_dt)]
   // for du_dt, where K is linearized by using u from the previous timestep
   if (!T)
   {
      T = Add(1.0, Mmat, dt, Kmat);
      current_dt = dt;
      T_solver.SetOperator(*T);
   }
   MFEM_VERIFY(dt == current_dt, ""); // SDIRK methods use the same dt
   Kmat.Mult(u, z);
   z.Neg();
   T_solver.Mult(z, du_dt);
}
 
void ConductionOperator::SetParameters(const Vector &u)
{
   ParGridFunction u_alpha_gf(&fespace);
   u_alpha_gf.SetFromTrueDofs(u);
   for (int i = 0; i < u_alpha_gf.Size(); i++)
   {
      u_alpha_gf(i) = kappa + alpha*u_alpha_gf(i);
   }
 
   delete K;
   K = new ParBilinearForm(&fespace);
 
   GridFunctionCoefficient u_coeff(&u_alpha_gf);
 
   K->AddDomainIntegrator(new DiffusionIntegrator(u_coeff));
   K->Assemble(0); // keep sparsity pattern of M and K the same
   K->FormSystemMatrix(ess_tdof_list, Kmat);
   delete T;
   T = NULL; // re-compute T on the next ImplicitSolve
}
 
ConductionOperator::~ConductionOperator()
{
   delete T;
   delete M;
   delete K;
}
 
real_t InitialTemperature(const Vector &x)
{
   if (x.Norml2() < 0.5)
   {
      return 2.0;
   }
   else
   {
      return 1.0;
   }
}