// MFEM Example 5 // // Compile with: make ex5 // // Sample runs: ex5 -m ../data/square-disc.mesh // ex5 -m ../data/star.mesh // ex5 -m ../data/star.mesh -pa // ex5 -m ../data/beam-tet.mesh // ex5 -m ../data/beam-hex.mesh // ex5 -m ../data/beam-hex.mesh -pa // ex5 -m ../data/escher.mesh // ex5 -m ../data/fichera.mesh // // Device sample runs: // ex5 -m ../data/star.mesh -pa -d cuda // ex5 -m ../data/star.mesh -pa -d raja-cuda // ex5 -m ../data/star.mesh -pa -d raja-omp // ex5 -m ../data/beam-hex.mesh -pa -d cuda // // Description: This example code solves a simple 2D mixed electromagnetic // diffusion problem corresponding to the mixed system // // sigma E - curl B = f // curl E + B = g // // with essential boundary condition E x n = . // Here, we use a given exact solution (E,B) and compute the // corresponding r.h.s. (f,g). We discretize with Nedelec // finite elements (electric field E) and piecewise discontinuous // integral polynomials (magnetic field B). // // The example demonstrates the use of the DarcyForm class, as // well as the collective saving of several grid functions in // VisIt (visit.llnl.gov) and ParaView (paraview.org) formats. // // We recommend viewing examples 1-4 before viewing this example. #include "mfem.hpp" #include #include #include using namespace std; using namespace mfem; // Define the analytical solution and forcing terms / boundary conditions void EFun_ex(const Vector & x, Vector & E); real_t BFun_ex(const Vector & x); void fFun(const Vector & x, Vector & f); real_t gFun(const Vector & x); real_t freq = 1.0, kappa; int main(int argc, char *argv[]) { StopWatch chrono; // 1. Parse command-line options. const char *mesh_file = ""; int nx = 0; int ny = 0; int order = 1; bool hybridization = false; bool pa = false; const char *device_config = "cpu"; bool visualization = 1; OptionsParser args(argc, argv); args.AddOption(&mesh_file, "-m", "--mesh", "Mesh file to use."); args.AddOption(&nx, "-nx", "--ncells-x", "Number of cells in x."); args.AddOption(&ny, "-ny", "--ncells-y", "Number of cells in y."); args.AddOption(&order, "-o", "--order", "Finite element order (polynomial degree)."); args.AddOption(&freq, "-f", "--frequency", "Set the frequency for the exact" " solution."); args.AddOption(&hybridization, "-hb", "--hybridization", "-no-hb", "--no-hybridization", "Enable hybridization."); args.AddOption(&pa, "-pa", "--partial-assembly", "-no-pa", "--no-partial-assembly", "Enable Partial Assembly."); args.AddOption(&device_config, "-d", "--device", "Device configuration string, see Device::Configure()."); args.AddOption(&visualization, "-vis", "--visualization", "-no-vis", "--no-visualization", "Enable or disable GLVis visualization."); args.Parse(); if (!args.Good()) { args.PrintUsage(cout); return 1; } args.PrintOptions(cout); kappa = freq * M_PI; // 2. Enable hardware devices such as GPUs, and programming models such as // CUDA, OCCA, RAJA and OpenMP based on command line options. Device device(device_config); device.Print(); // 3. Read the mesh from the given mesh file. We can handle triangular, // quadrilateral, tetrahedral, hexahedral, surface and volume meshes with // the same code. if (ny <= 0) { ny = nx; } Mesh *mesh = NULL; if (strlen(mesh_file) > 0) { mesh = new Mesh(mesh_file, 1, 1); } else { mesh = new Mesh(Mesh::MakeCartesian2D(nx, ny, Element::QUADRILATERAL)); } int dim = mesh->Dimension(); // 4. Refine the mesh to increase the resolution. In this example we do // 'ref_levels' of uniform refinement. We choose 'ref_levels' to be the // largest number that gives a final mesh with no more than 10,000 // elements. if (strlen(mesh_file) > 0) { int ref_levels = (int)floor(log(10000./mesh->GetNE())/log(2.)/dim); for (int l = 0; l < ref_levels; l++) { mesh->UniformRefinement(); } } // 5. Define a finite element space on the mesh. Here we use the // Raviart-Thomas finite elements of the specified order. FiniteElementCollection *R_coll(new ND_FECollection(order+1, dim)); FiniteElementCollection *W_coll(new L2_FECollection(order, dim, 0, FiniteElement::INTEGRAL)); FiniteElementSpace *R_space = new FiniteElementSpace(mesh, R_coll); FiniteElementSpace *W_space = new FiniteElementSpace(mesh, W_coll); DarcyForm *darcy = new DarcyForm(R_space, W_space); // 6. Define the BlockStructure of the problem, i.e. define the array of // offsets for each variable. The last component of the Array is the sum // of the dimensions of each block. const Array &block_offsets = darcy->GetOffsets(); std::cout << "***********************************************************\n"; std::cout << "dim(R) = " << block_offsets[1] - block_offsets[0] << "\n"; std::cout << "dim(W) = " << block_offsets[2] - block_offsets[1] << "\n"; std::cout << "dim(R+W) = " << block_offsets.Last() << "\n"; std::cout << "***********************************************************\n"; // 7. Define the coefficients, analytical solution, and rhs of the PDE. ConstantCoefficient muinvsqrt(1.0); ConstantCoefficient sigma(1.0); VectorFunctionCoefficient fcoeff(dim, fFun); FunctionCoefficient gcoeff(gFun); VectorFunctionCoefficient Ecoeff(dim, EFun_ex); FunctionCoefficient Bcoeff(BFun_ex); // 8. Allocate memory (x, rhs) for the analytical solution and the right hand // side. Define the GridFunction E,B for the finite element solution and // linear forms fform and gform for the right hand side. The data // allocated by x and rhs are passed as a reference to the grid functions // (E,B) and the linear forms (fform, gform). MemoryType mt = device.GetMemoryType(); BlockVector x(block_offsets, mt), rhs(block_offsets, mt); LinearForm *fform(new LinearForm); fform->Update(R_space, rhs.GetBlock(0), 0); fform->AddDomainIntegrator(new VectorFEDomainLFIntegrator(fcoeff)); fform->Assemble(); fform->SyncAliasMemory(rhs); LinearForm *gform(new LinearForm); gform->Update(W_space, rhs.GetBlock(1), 0); gform->AddDomainIntegrator(new DomainLFIntegrator(gcoeff)); gform->Assemble(); gform->SyncAliasMemory(rhs); // 9. Assemble the finite element matrices for the Darcy operator // // D = [ M C^T ] // [ C 0 ] // where: // // M = \int_\Omega \sigma E_h \cdot v_h d\Omega E_h, v_h \in R_h // C = \int_\Omega \curl E_h q_h d\Omega E_h \in R_h, q_h \in W_h //BilinearForm *mEVarf(new BilinearForm(R_space)); //MixedBilinearForm *cVarf(new MixedBilinearForm(R_space, W_space)); BilinearForm *mEVarf = darcy->GetFluxMassForm(); MixedBilinearForm *cVarf = darcy->GetFluxDivForm(); BilinearForm *mBVarf = darcy->GetPotentialMassForm(); //if (pa) { mEVarf->SetAssemblyLevel(AssemblyLevel::PARTIAL); } mEVarf->AddDomainIntegrator(new VectorFEMassIntegrator(sigma)); //mEVarf->Assemble(); //if (!pa) { mEVarf->Finalize(); } //if (pa) { cVarf->SetAssemblyLevel(AssemblyLevel::PARTIAL); } cVarf->AddDomainIntegrator(new MixedScalarCurlIntegrator(muinvsqrt)); //cVarf->Assemble(); //if (!pa) { cVarf->Finalize(); } mBVarf->AddDomainIntegrator(new MassIntegrator()); //set essential boundary condition GridFunction E, B; E.MakeRef(R_space, x.GetBlock(0), 0); B.MakeRef(W_space, x.GetBlock(1), 0); Array ess_flux_tdofs_list; if (mesh->bdr_attributes.Size()) { Array ess_bdr(mesh->bdr_attributes.Max()); ess_bdr = 1; R_space->GetEssentialTrueDofs(ess_bdr, ess_flux_tdofs_list); E.ProjectBdrCoefficientTangent(Ecoeff, ess_bdr); } //set hybridization / assembly level FiniteElementCollection *trace_coll = NULL; FiniteElementSpace *trace_space = NULL; chrono.Clear(); chrono.Start(); if (hybridization) { trace_coll = new ND_Trace_FECollection(order+1, dim); trace_space = new FiniteElementSpace(mesh, trace_coll); darcy->EnableHybridization(trace_space, new TangentTraceJumpIntegrator(), ess_flux_tdofs_list); } if (pa) { darcy->SetAssemblyLevel(AssemblyLevel::PARTIAL); } darcy->Assemble(); //if (!pa) { darcy->Finalize(); } OperatorHandle pDarcyOp; Vector X, RHS; //darcy->FormSystemMatrix(ess_flux_tdofs_list, pDarcyOp); darcy->FormLinearSystem(ess_flux_tdofs_list, x, rhs, pDarcyOp, X, RHS); chrono.Stop(); std::cout << "Assembly took " << chrono.RealTime() << "s.\n"; int maxIter(1000); real_t rtol(1.e-6); real_t atol(1.e-10); if (hybridization) { // 10. Construct the preconditioner GSSmoother prec(*pDarcyOp.As()); // 11. Solve the linear system with GMRES. // Check the norm of the unpreconditioned residual. chrono.Clear(); chrono.Start(); GMRESSolver solver; solver.SetAbsTol(atol); solver.SetRelTol(rtol); solver.SetMaxIter(maxIter); solver.SetOperator(*pDarcyOp); solver.SetPreconditioner(prec); solver.SetPrintLevel(1); solver.Mult(RHS, X); darcy->RecoverFEMSolution(X, rhs, x); chrono.Stop(); if (solver.GetConverged()) { std::cout << "GMRES converged in " << solver.GetNumIterations() << " iterations with a residual norm of " << solver.GetFinalNorm() << ".\n"; } else { std::cout << "GMRES did not converge in " << solver.GetNumIterations() << " iterations. Residual norm is " << solver.GetFinalNorm() << ".\n"; } std::cout << "GMRES solver took " << chrono.RealTime() << "s.\n"; } else { // 10. Construct the operators for preconditioner // // P = [ diag(M) 0 ] // [ 0 C diag(M)^-1 C^T ] // // Here we use Symmetric Gauss-Seidel to approximate the inverse of the // magnetic field Schur Complement SparseMatrix *MinvBt = NULL; Vector Md(mEVarf->Height()); BlockDiagonalPreconditioner darcyPrec(block_offsets); Solver *invM, *invS; SparseMatrix *S = NULL; if (pa) { mEVarf->AssembleDiagonal(Md); auto Md_host = Md.HostRead(); Vector invMd(mEVarf->Height()); for (int i=0; iHeight(); ++i) { invMd(i) = 1.0 / Md_host[i]; } Vector BMBt_diag(cVarf->Height()); cVarf->AssembleDiagonal_ADAt(invMd, BMBt_diag); Array ess_tdof_list; // empty invM = new OperatorJacobiSmoother(Md, ess_tdof_list); invS = new OperatorJacobiSmoother(BMBt_diag, ess_tdof_list); } else { SparseMatrix &M(mEVarf->SpMat()); M.GetDiag(Md); Md.HostReadWrite(); SparseMatrix &C(cVarf->SpMat()); MinvBt = Transpose(C); for (int i = 0; i < Md.Size(); i++) { MinvBt->ScaleRow(i, 1./Md(i)); } S = Mult(C, *MinvBt); if (mBVarf) { SparseMatrix &Mtm(mBVarf->SpMat()); SparseMatrix *Snew = Add(Mtm, *S); delete S; S = Snew; } invM = new DSmoother(M); #ifndef MFEM_USE_SUITESPARSE invS = new GSSmoother(*S); #else invS = new UMFPackSolver(*S); #endif } invM->iterative_mode = false; invS->iterative_mode = false; darcyPrec.SetDiagonalBlock(0, invM); darcyPrec.SetDiagonalBlock(1, invS); // 11. Solve the linear system with MINRES. // Check the norm of the unpreconditioned residual. chrono.Clear(); chrono.Start(); FGMRESSolver solver; solver.SetAbsTol(atol); solver.SetRelTol(rtol); solver.SetMaxIter(maxIter); solver.SetOperator(*pDarcyOp); solver.SetPreconditioner(darcyPrec); solver.SetPrintLevel(1); solver.Mult(RHS, X); darcy->RecoverFEMSolution(X, rhs, x); if (device.IsEnabled()) { x.HostRead(); } chrono.Stop(); if (solver.GetConverged()) { std::cout << "GMRES converged in " << solver.GetNumIterations() << " iterations with a residual norm of " << solver.GetFinalNorm() << ".\n"; } else { std::cout << "GMRES did not converge in " << solver.GetNumIterations() << " iterations. Residual norm is " << solver.GetFinalNorm() << ".\n"; } std::cout << "MINRES solver took " << chrono.RealTime() << "s.\n"; delete invM; delete invS; delete S; //delete Bt; delete MinvBt; } // 12. Create the grid functions E and B. Compute the L2 error norms. int order_quad = max(2, 2*order+1); const IntegrationRule *irs[Geometry::NumGeom]; for (int i=0; i < Geometry::NumGeom; ++i) { irs[i] = &(IntRules.Get(i, order_quad)); } real_t err_E = E.ComputeL2Error(Ecoeff, irs); real_t norm_E = ComputeLpNorm(2., Ecoeff, *mesh, irs); real_t err_B = B.ComputeL2Error(Bcoeff, irs); real_t norm_B = ComputeLpNorm(2., Bcoeff, *mesh, irs); std::cout << "|| E_h - E_ex || / || E_ex || = " << err_E / norm_E << "\n"; std::cout << "|| B_h - B_ex || / || B_ex || = " << err_B / norm_B << "\n"; // 13. Save the mesh and the solution. This output can be viewed later using // GLVis: "glvis -m ex5.mesh -g sol_u.gf" or "glvis -m ex5.mesh -g // sol_p.gf". { ofstream mesh_ofs("ex5.mesh"); mesh_ofs.precision(8); mesh->Print(mesh_ofs); ofstream E_ofs("sol_E.gf"); E_ofs.precision(8); E.Save(E_ofs); ofstream B_ofs("sol_B.gf"); B_ofs.precision(8); B.Save(B_ofs); } // 14. Save data in the VisIt format VisItDataCollection visit_dc("Example5", mesh); visit_dc.RegisterField("electric field", &E); visit_dc.RegisterField("magnetic field", &B); visit_dc.Save(); // 15. Save data in the ParaView format ParaViewDataCollection paraview_dc("Example5", mesh); paraview_dc.SetPrefixPath("ParaView"); paraview_dc.SetLevelsOfDetail(order); paraview_dc.SetCycle(0); paraview_dc.SetDataFormat(VTKFormat::BINARY); paraview_dc.SetHighOrderOutput(true); paraview_dc.SetTime(0.0); // set the time paraview_dc.RegisterField("electric field",&E); paraview_dc.RegisterField("magnetic field",&B); paraview_dc.Save(); // 16. Send the solution by socket to a GLVis server. if (visualization) { char vishost[] = "localhost"; int visport = 19916; socketstream E_sock(vishost, visport); E_sock.precision(8); E_sock << "solution\n" << *mesh << E << "window_title 'Electric field'" << endl; E_sock << "keys Rljvvvvvmmc" << endl; socketstream B_sock(vishost, visport); B_sock.precision(8); B_sock << "solution\n" << *mesh << B << "window_title 'Magnetic field'" << endl; B_sock << "keys Rljmmc" << endl; } // 17. Free the used memory. delete fform; delete gform; //delete mEVarf; //delete cVarf; delete darcy; delete W_space; delete R_space; delete trace_space; delete W_coll; delete R_coll; delete trace_coll; delete mesh; return 0; } void EFun_ex(const Vector & x, Vector & E) { const int dim = x.Size(); if (dim == 3) { E(0) = sin(kappa * x(1)); E(1) = sin(kappa * x(2)); E(2) = sin(kappa * x(0)); } else { E(0) = sin(kappa * x(1)); E(1) = sin(kappa * x(0)); if (x.Size() == 3) { E(2) = 0.0; } } } real_t BFun_ex(const Vector & x) { return kappa * (-cos(kappa * x(0)) + cos(kappa * x(1))); } void fFun(const Vector & x, Vector & f) { const int dim = x.Size(); if (dim == 3) { f(0) = (1. + kappa * kappa) * sin(kappa * x(1)); f(1) = (1. + kappa * kappa) * sin(kappa * x(2)); f(2) = (1. + kappa * kappa) * sin(kappa * x(0)); } else { f(0) = (1. + kappa * kappa) * sin(kappa * x(1)); f(1) = (1. + kappa * kappa) * sin(kappa * x(0)); if (x.Size() == 3) { f(2) = 0.0; } } } real_t gFun(const Vector & x) { return 0.; }