static char help[] = "Poisson Problem in mixed form with 2d and 3d with finite elements.\n\ We solve the Poisson problem in a rectangular\n\ domain, using a parallel unstructured mesh (DMPLEX) to discretize it.\n\ This example supports automatic convergence estimation\n\ and Hdiv elements.\n\n\n"; /* The mixed form of Poisson's equation, e.g. https://firedrakeproject.org/demos/poisson_mixed.py.html, is given in the strong form by \begin{align} \vb{q} - \nabla u &= 0 \\ \nabla \cdot \vb{q} &= f \end{align} where $u$ is the potential, as in the original problem, but we also discretize the gradient of potential $\vb{q}$, or flux, directly. The weak form is then \begin{align} + <\nabla \cdot t, u> - _\Gamma &= 0 \\ &= \end{align} For the original Poisson problem, the Dirichlet boundary forces an essential boundary condition on the potential space, and the Neumann boundary gives a natural boundary condition in the weak form. In the mixed formulation, the Neumann boundary gives an essential boundary condition on the flux space, $\vb{q} \cdot \vu{n} = h$, and the Dirichlet condition becomes a natural condition in the weak form, _\Gamma. */ #include #include #include #include typedef enum { SOL_LINEAR, SOL_QUADRATIC, SOL_QUARTIC, SOL_QUARTIC_NEUMANN, SOL_UNKNOWN, NUM_SOLTYPE } SolType; const char *SolTypeNames[NUM_SOLTYPE + 3] = {"linear", "quadratic", "quartic", "quartic_neumann", "unknown", "SolType", "SOL_", NULL}; typedef struct { SolType solType; /* The type of exact solution */ } AppCtx; static void f0_u(PetscInt dim, PetscInt Nf, PetscInt NfAux, const PetscInt uOff[], const PetscInt uOff_x[], const PetscScalar u[], const PetscScalar u_t[], const PetscScalar u_x[], const PetscInt aOff[], const PetscInt aOff_x[], const PetscScalar a[], const PetscScalar a_t[], const PetscScalar a_x[], PetscReal t, const PetscReal x[], PetscInt numConstants, const PetscScalar constants[], PetscScalar f0[]) { PetscInt d; for (d = 0; d < dim; ++d) f0[0] += u_x[uOff_x[0] + d * dim + d]; } /* 2D Dirichlet potential example u = x q = <1, 0> f = 0 We will need a boundary integral of u over \Gamma. */ static PetscErrorCode linear_u(PetscInt dim, PetscReal time, const PetscReal x[], PetscInt Nc, PetscScalar *u, void *ctx) { u[0] = x[0]; return PETSC_SUCCESS; } static PetscErrorCode linear_q(PetscInt dim, PetscReal time, const PetscReal x[], PetscInt Nc, PetscScalar *u, void *ctx) { PetscInt c; for (c = 0; c < Nc; ++c) u[c] = c ? 0.0 : 1.0; return PETSC_SUCCESS; } static void f0_linear_u(PetscInt dim, PetscInt Nf, PetscInt NfAux, const PetscInt uOff[], const PetscInt uOff_x[], const PetscScalar u[], const PetscScalar u_t[], const PetscScalar u_x[], const PetscInt aOff[], const PetscInt aOff_x[], const PetscScalar a[], const PetscScalar a_t[], const PetscScalar a_x[], PetscReal t, const PetscReal x[], PetscInt numConstants, const PetscScalar constants[], PetscScalar f0[]) { f0[0] = 0.0; f0_u(dim, Nf, NfAux, uOff, uOff_x, u, u_t, u_x, aOff, aOff_x, a, a_t, a_x, t, x, numConstants, constants, f0); } static void f0_bd_linear_q(PetscInt dim, PetscInt Nf, PetscInt NfAux, const PetscInt uOff[], const PetscInt uOff_x[], const PetscScalar u[], const PetscScalar u_t[], const PetscScalar u_x[], const PetscInt aOff[], const PetscInt aOff_x[], const PetscScalar a[], const PetscScalar a_t[], const PetscScalar a_x[], PetscReal t, const PetscReal x[], const PetscReal n[], PetscInt numConstants, const PetscScalar constants[], PetscScalar f0[]) { PetscScalar potential; PetscInt d; PetscCallAbort(PETSC_COMM_SELF, linear_u(dim, t, x, dim, &potential, NULL)); for (d = 0; d < dim; ++d) f0[d] = -potential * n[d]; } /* 2D Dirichlet potential example u = x^2 + y^2 q = <2x, 2y> f = 4 We will need a boundary integral of u over \Gamma. */ static PetscErrorCode quadratic_u(PetscInt dim, PetscReal time, const PetscReal x[], PetscInt Nc, PetscScalar *u, void *ctx) { PetscInt d; u[0] = 0.0; for (d = 0; d < dim; ++d) u[0] += x[d] * x[d]; return PETSC_SUCCESS; } static PetscErrorCode quadratic_q(PetscInt dim, PetscReal time, const PetscReal x[], PetscInt Nc, PetscScalar *u, void *ctx) { PetscInt c; for (c = 0; c < Nc; ++c) u[c] = 2.0 * x[c]; return PETSC_SUCCESS; } static void f0_quadratic_u(PetscInt dim, PetscInt Nf, PetscInt NfAux, const PetscInt uOff[], const PetscInt uOff_x[], const PetscScalar u[], const PetscScalar u_t[], const PetscScalar u_x[], const PetscInt aOff[], const PetscInt aOff_x[], const PetscScalar a[], const PetscScalar a_t[], const PetscScalar a_x[], PetscReal t, const PetscReal x[], PetscInt numConstants, const PetscScalar constants[], PetscScalar f0[]) { f0[0] = -4.0; f0_u(dim, Nf, NfAux, uOff, uOff_x, u, u_t, u_x, aOff, aOff_x, a, a_t, a_x, t, x, numConstants, constants, f0); } static void f0_bd_quadratic_q(PetscInt dim, PetscInt Nf, PetscInt NfAux, const PetscInt uOff[], const PetscInt uOff_x[], const PetscScalar u[], const PetscScalar u_t[], const PetscScalar u_x[], const PetscInt aOff[], const PetscInt aOff_x[], const PetscScalar a[], const PetscScalar a_t[], const PetscScalar a_x[], PetscReal t, const PetscReal x[], const PetscReal n[], PetscInt numConstants, const PetscScalar constants[], PetscScalar f0[]) { PetscScalar potential; PetscInt d; PetscCallAbort(PETSC_COMM_SELF, quadratic_u(dim, t, x, dim, &potential, NULL)); for (d = 0; d < dim; ++d) f0[d] = -potential * n[d]; } /* 2D Dirichlet potential example u = x (1-x) y (1-y) q = <(1-2x) y (1-y), x (1-x) (1-2y)> f = -y (1-y) - x (1-x) u|_\Gamma = 0 so that the boundary integral vanishes */ static PetscErrorCode quartic_u(PetscInt dim, PetscReal time, const PetscReal x[], PetscInt Nc, PetscScalar *u, void *ctx) { PetscInt d; u[0] = 1.0; for (d = 0; d < dim; ++d) u[0] *= x[d] * (1.0 - x[d]); return PETSC_SUCCESS; } static PetscErrorCode quartic_q(PetscInt dim, PetscReal time, const PetscReal x[], PetscInt Nc, PetscScalar *u, void *ctx) { PetscInt c, d; for (c = 0; c < Nc; ++c) { u[c] = 1.0; for (d = 0; d < dim; ++d) { if (c == d) u[c] *= 1 - 2.0 * x[d]; else u[c] *= x[d] * (1.0 - x[d]); } } return PETSC_SUCCESS; } static void f0_quartic_u(PetscInt dim, PetscInt Nf, PetscInt NfAux, const PetscInt uOff[], const PetscInt uOff_x[], const PetscScalar u[], const PetscScalar u_t[], const PetscScalar u_x[], const PetscInt aOff[], const PetscInt aOff_x[], const PetscScalar a[], const PetscScalar a_t[], const PetscScalar a_x[], PetscReal t, const PetscReal x[], PetscInt numConstants, const PetscScalar constants[], PetscScalar f0[]) { PetscInt d; f0[0] = 0.0; for (d = 0; d < dim; ++d) f0[0] += 2.0 * x[d] * (1.0 - x[d]); f0_u(dim, Nf, NfAux, uOff, uOff_x, u, u_t, u_x, aOff, aOff_x, a, a_t, a_x, t, x, numConstants, constants, f0); } /* 2D Dirichlet potential example u = x (1-x) y (1-y) q = <(1-2x) y (1-y), x (1-x) (1-2y)> f = -y (1-y) - x (1-x) du/dn_\Gamma = {(1-2x) y (1-y), x (1-x) (1-2y)} . n produces an essential condition on q */ static void f0_q(PetscInt dim, PetscInt Nf, PetscInt NfAux, const PetscInt uOff[], const PetscInt uOff_x[], const PetscScalar u[], const PetscScalar u_t[], const PetscScalar u_x[], const PetscInt aOff[], const PetscInt aOff_x[], const PetscScalar a[], const PetscScalar a_t[], const PetscScalar a_x[], PetscReal t, const PetscReal x[], PetscInt numConstants, const PetscScalar constants[], PetscScalar f0[]) { PetscInt c; for (c = 0; c < dim; ++c) f0[c] = u[uOff[0] + c]; } /* <\nabla\cdot w, u> = <\nabla w, Iu> */ static void f1_q(PetscInt dim, PetscInt Nf, PetscInt NfAux, const PetscInt uOff[], const PetscInt uOff_x[], const PetscScalar u[], const PetscScalar u_t[], const PetscScalar u_x[], const PetscInt aOff[], const PetscInt aOff_x[], const PetscScalar a[], const PetscScalar a_t[], const PetscScalar a_x[], PetscReal t, const PetscReal x[], PetscInt numConstants, const PetscScalar constants[], PetscScalar f1[]) { PetscInt c; for (c = 0; c < dim; ++c) f1[c * dim + c] = u[uOff[1]]; } /* */ static void g0_qq(PetscInt dim, PetscInt Nf, PetscInt NfAux, const PetscInt uOff[], const PetscInt uOff_x[], const PetscScalar u[], const PetscScalar u_t[], const PetscScalar u_x[], const PetscInt aOff[], const PetscInt aOff_x[], const PetscScalar a[], const PetscScalar a_t[], const PetscScalar a_x[], PetscReal t, PetscReal u_tShift, const PetscReal x[], PetscInt numConstants, const PetscScalar constants[], PetscScalar g0[]) { PetscInt c; for (c = 0; c < dim; ++c) g0[c * dim + c] = 1.0; } /* <\nabla\cdot t, u> = <\nabla t, Iu> */ static void g2_qu(PetscInt dim, PetscInt Nf, PetscInt NfAux, const PetscInt uOff[], const PetscInt uOff_x[], const PetscScalar u[], const PetscScalar u_t[], const PetscScalar u_x[], const PetscInt aOff[], const PetscInt aOff_x[], const PetscScalar a[], const PetscScalar a_t[], const PetscScalar a_x[], PetscReal t, PetscReal u_tShift, const PetscReal x[], PetscInt numConstants, const PetscScalar constants[], PetscScalar g2[]) { PetscInt d; for (d = 0; d < dim; ++d) g2[d * dim + d] = 1.0; } /* */ static void g1_uq(PetscInt dim, PetscInt Nf, PetscInt NfAux, const PetscInt uOff[], const PetscInt uOff_x[], const PetscScalar u[], const PetscScalar u_t[], const PetscScalar u_x[], const PetscInt aOff[], const PetscInt aOff_x[], const PetscScalar a[], const PetscScalar a_t[], const PetscScalar a_x[], PetscReal t, PetscReal u_tShift, const PetscReal x[], PetscInt numConstants, const PetscScalar constants[], PetscScalar g1[]) { PetscInt d; for (d = 0; d < dim; ++d) g1[d * dim + d] = 1.0; } static PetscErrorCode ProcessOptions(MPI_Comm comm, AppCtx *options) { PetscFunctionBeginUser; options->solType = SOL_LINEAR; PetscOptionsBegin(comm, "", "Poisson Problem Options", "DMPLEX"); PetscCall(PetscOptionsEnum("-sol_type", "Type of exact solution", "ex24.c", SolTypeNames, (PetscEnum)options->solType, (PetscEnum *)&options->solType, NULL)); PetscOptionsEnd(); PetscFunctionReturn(PETSC_SUCCESS); } static PetscErrorCode CreateMesh(MPI_Comm comm, AppCtx *user, DM *dm) { PetscFunctionBeginUser; PetscCall(DMCreate(comm, dm)); PetscCall(DMSetType(*dm, DMPLEX)); PetscCall(PetscObjectSetName((PetscObject)*dm, "Example Mesh")); PetscCall(DMSetApplicationContext(*dm, user)); PetscCall(DMSetFromOptions(*dm)); PetscCall(DMViewFromOptions(*dm, NULL, "-dm_view")); PetscFunctionReturn(PETSC_SUCCESS); } static PetscErrorCode SetupPrimalProblem(DM dm, AppCtx *user) { PetscDS ds; DMLabel label; PetscWeakForm wf; const PetscInt id = 1; PetscInt bd; PetscFunctionBeginUser; PetscCall(DMGetLabel(dm, "marker", &label)); PetscCall(DMGetDS(dm, &ds)); PetscCall(PetscDSSetResidual(ds, 0, f0_q, f1_q)); PetscCall(PetscDSSetJacobian(ds, 0, 0, g0_qq, NULL, NULL, NULL)); PetscCall(PetscDSSetJacobian(ds, 0, 1, NULL, NULL, g2_qu, NULL)); PetscCall(PetscDSSetJacobian(ds, 1, 0, NULL, g1_uq, NULL, NULL)); switch (user->solType) { case SOL_LINEAR: PetscCall(PetscDSSetResidual(ds, 1, f0_linear_u, NULL)); PetscCall(DMAddBoundary(dm, DM_BC_NATURAL, "Dirichlet Bd Integral", label, 1, &id, 0, 0, NULL, NULL, NULL, user, &bd)); PetscCall(PetscDSGetBoundary(ds, bd, &wf, NULL, NULL, NULL, NULL, NULL, NULL, NULL, NULL, NULL, NULL, NULL)); PetscCall(PetscWeakFormSetIndexBdResidual(wf, label, 1, 0, 0, 0, f0_bd_linear_q, 0, NULL)); PetscCall(PetscDSSetExactSolution(ds, 0, linear_q, user)); PetscCall(PetscDSSetExactSolution(ds, 1, linear_u, user)); break; case SOL_QUADRATIC: PetscCall(PetscDSSetResidual(ds, 1, f0_quadratic_u, NULL)); PetscCall(DMAddBoundary(dm, DM_BC_NATURAL, "Dirichlet Bd Integral", label, 1, &id, 0, 0, NULL, NULL, NULL, user, &bd)); PetscCall(PetscDSGetBoundary(ds, bd, &wf, NULL, NULL, NULL, NULL, NULL, NULL, NULL, NULL, NULL, NULL, NULL)); PetscCall(PetscWeakFormSetIndexBdResidual(wf, label, 1, 0, 0, 0, f0_bd_quadratic_q, 0, NULL)); PetscCall(PetscDSSetExactSolution(ds, 0, quadratic_q, user)); PetscCall(PetscDSSetExactSolution(ds, 1, quadratic_u, user)); break; case SOL_QUARTIC: PetscCall(PetscDSSetResidual(ds, 1, f0_quartic_u, NULL)); PetscCall(PetscDSSetExactSolution(ds, 0, quartic_q, user)); PetscCall(PetscDSSetExactSolution(ds, 1, quartic_u, user)); break; case SOL_QUARTIC_NEUMANN: PetscCall(PetscDSSetResidual(ds, 1, f0_quartic_u, NULL)); PetscCall(PetscDSSetExactSolution(ds, 0, quartic_q, user)); PetscCall(PetscDSSetExactSolution(ds, 1, quartic_u, user)); PetscCall(DMAddBoundary(dm, DM_BC_ESSENTIAL, "Flux condition", label, 1, &id, 0, 0, NULL, (void (*)(void))quartic_q, NULL, user, NULL)); break; default: SETERRQ(PetscObjectComm((PetscObject)dm), PETSC_ERR_ARG_WRONG, "Invalid exact solution type %s", SolTypeNames[PetscMin(user->solType, SOL_UNKNOWN)]); } PetscFunctionReturn(PETSC_SUCCESS); } static PetscErrorCode SetupDiscretization(DM dm, PetscErrorCode (*setup)(DM, AppCtx *), AppCtx *user) { DM cdm = dm; PetscFE feq, feu; DMPolytopeType ct; PetscBool simplex; PetscInt dim, cStart; PetscFunctionBeginUser; PetscCall(DMGetDimension(dm, &dim)); PetscCall(DMPlexGetHeightStratum(dm, 0, &cStart, NULL)); PetscCall(DMPlexGetCellType(dm, cStart, &ct)); simplex = DMPolytopeTypeGetNumVertices(ct) == DMPolytopeTypeGetDim(ct) + 1 ? PETSC_TRUE : PETSC_FALSE; /* Create finite element */ PetscCall(PetscFECreateDefault(PETSC_COMM_SELF, dim, dim, simplex, "field_", -1, &feq)); PetscCall(PetscObjectSetName((PetscObject)feq, "field")); PetscCall(PetscFECreateDefault(PETSC_COMM_SELF, dim, 1, simplex, "potential_", -1, &feu)); PetscCall(PetscObjectSetName((PetscObject)feu, "potential")); PetscCall(PetscFECopyQuadrature(feq, feu)); /* Set discretization and boundary conditions for each mesh */ PetscCall(DMSetField(dm, 0, NULL, (PetscObject)feq)); PetscCall(DMSetField(dm, 1, NULL, (PetscObject)feu)); PetscCall(DMCreateDS(dm)); PetscCall((*setup)(dm, user)); while (cdm) { PetscCall(DMCopyDisc(dm, cdm)); PetscCall(DMGetCoarseDM(cdm, &cdm)); } PetscCall(PetscFEDestroy(&feq)); PetscCall(PetscFEDestroy(&feu)); PetscFunctionReturn(PETSC_SUCCESS); } int main(int argc, char **argv) { DM dm; /* Problem specification */ SNES snes; /* Nonlinear solver */ Vec u; /* Solutions */ AppCtx user; /* User-defined work context */ PetscFunctionBeginUser; PetscCall(PetscInitialize(&argc, &argv, NULL, help)); PetscCall(ProcessOptions(PETSC_COMM_WORLD, &user)); /* Primal system */ PetscCall(SNESCreate(PETSC_COMM_WORLD, &snes)); PetscCall(CreateMesh(PETSC_COMM_WORLD, &user, &dm)); PetscCall(SNESSetDM(snes, dm)); PetscCall(SetupDiscretization(dm, SetupPrimalProblem, &user)); PetscCall(DMCreateGlobalVector(dm, &u)); PetscCall(VecSet(u, 0.0)); PetscCall(PetscObjectSetName((PetscObject)u, "potential")); PetscCall(DMPlexSetSNESLocalFEM(dm, PETSC_FALSE, &user)); PetscCall(SNESSetFromOptions(snes)); PetscCall(DMSNESCheckFromOptions(snes, u)); PetscCall(SNESSolve(snes, NULL, u)); PetscCall(SNESGetSolution(snes, &u)); PetscCall(VecViewFromOptions(u, NULL, "-potential_view")); /* Cleanup */ PetscCall(VecDestroy(&u)); PetscCall(SNESDestroy(&snes)); PetscCall(DMDestroy(&dm)); PetscCall(PetscFinalize()); return 0; } /*TEST test: suffix: 2d_bdm1_p0 requires: triangle args: -sol_type linear \ -field_petscspace_degree 1 -field_petscdualspace_type bdm -dm_refine 1 \ -dmsnes_check .001 -snes_error_if_not_converged \ -ksp_rtol 1e-10 -ksp_error_if_not_converged \ -pc_type fieldsplit -pc_fieldsplit_type schur -pc_fieldsplit_schur_factorization_type full -pc_fieldsplit_schur_precondition full \ -fieldsplit_field_pc_type lu \ -fieldsplit_potential_ksp_rtol 1e-10 -fieldsplit_potential_pc_type lu test: nsize: 4 suffix: 2d_bdm1_p0_bddc requires: triangle !single args: -sol_type linear \ -field_petscspace_degree 1 -field_petscdualspace_type bdm -dm_refine 1 \ -dmsnes_check .001 -snes_error_if_not_converged \ -ksp_error_if_not_converged -ksp_type cg \ -petscpartitioner_type simple -dm_mat_type is \ -pc_type bddc -pc_bddc_use_local_mat_graph 0 \ -pc_bddc_benign_trick -pc_bddc_nonetflux -pc_bddc_detect_disconnected -pc_bddc_use_qr_single \ -pc_bddc_coarse_redundant_pc_type svd -pc_bddc_neumann_pc_type svd -pc_bddc_dirichlet_pc_type svd test: nsize: 9 requires: !single suffix: 2d_rt1_p0_bddc args: -sol_type quadratic \ -potential_petscspace_degree 0 \ -potential_petscdualspace_lagrange_use_moments \ -potential_petscdualspace_lagrange_moment_order 2 \ -field_petscfe_default_quadrature_order 1 \ -field_petscspace_degree 1 \ -field_petscspace_type sum \ -field_petscspace_variables 2 \ -field_petscspace_components 2 \ -field_petscspace_sum_spaces 2 \ -field_petscspace_sum_concatenate true \ -field_sumcomp_0_petscspace_variables 2 \ -field_sumcomp_0_petscspace_type tensor \ -field_sumcomp_0_petscspace_tensor_spaces 2 \ -field_sumcomp_0_petscspace_tensor_uniform false \ -field_sumcomp_0_tensorcomp_0_petscspace_degree 1 \ -field_sumcomp_0_tensorcomp_1_petscspace_degree 0 \ -field_sumcomp_1_petscspace_variables 2 \ -field_sumcomp_1_petscspace_type tensor \ -field_sumcomp_1_petscspace_tensor_spaces 2 \ -field_sumcomp_1_petscspace_tensor_uniform false \ -field_sumcomp_1_tensorcomp_0_petscspace_degree 0 \ -field_sumcomp_1_tensorcomp_1_petscspace_degree 1 \ -field_petscdualspace_form_degree -1 \ -field_petscdualspace_order 1 \ -field_petscdualspace_lagrange_trimmed true \ -dm_plex_box_faces 3,3 dm_refine 1 -dm_plex_simplex 0 \ -dmsnes_check .001 -snes_error_if_not_converged \ -ksp_error_if_not_converged -ksp_type cg \ -petscpartitioner_type simple -dm_mat_type is \ -pc_type bddc -pc_bddc_use_local_mat_graph 0 \ -pc_bddc_benign_trick -pc_bddc_nonetflux -pc_bddc_detect_disconnected -pc_bddc_use_qr_single \ -pc_bddc_coarse_redundant_pc_type svd -pc_bddc_neumann_pc_type svd -pc_bddc_dirichlet_pc_type svd test: # Using -dm_refine 2 -convest_num_refine 3 we get L_2 convergence rate: [2.0, 1.0] # Using -sol_type quadratic -dm_refine 2 -convest_num_refine 3 we get L_2 convergence rate: [2.9, 1.0] suffix: 2d_bdm1_p0_conv requires: triangle args: -sol_type quartic \ -field_petscspace_degree 1 -field_petscdualspace_type bdm -dm_refine 0 -convest_num_refine 1 -snes_convergence_estimate \ -snes_error_if_not_converged \ -ksp_rtol 1e-10 -ksp_error_if_not_converged \ -pc_type fieldsplit -pc_fieldsplit_type schur -pc_fieldsplit_schur_factorization_type full -pc_fieldsplit_schur_precondition full \ -fieldsplit_field_pc_type lu \ -fieldsplit_potential_ksp_rtol 1e-10 -fieldsplit_potential_pc_type lu test: # HDF5 output: -dm_view hdf5:${PETSC_DIR}/sol.h5 -potential_view hdf5:${PETSC_DIR}/sol.h5::append -exact_vec_view hdf5:${PETSC_DIR}/sol.h5::append # VTK output: -potential_view vtk: -exact_vec_view vtk: # VTU output: -potential_view vtk:multifield.vtu -exact_vec_view vtk:exact.vtu suffix: 2d_q2_p0 requires: triangle args: -sol_type linear -dm_plex_simplex 0 \ -field_petscspace_degree 2 -dm_refine 0 \ -dmsnes_check .001 -snes_error_if_not_converged \ -ksp_rtol 1e-10 -ksp_error_if_not_converged \ -pc_type fieldsplit -pc_fieldsplit_type schur -pc_fieldsplit_schur_factorization_type full -pc_fieldsplit_schur_precondition full \ -fieldsplit_field_pc_type lu \ -fieldsplit_potential_ksp_rtol 1e-10 -fieldsplit_potential_pc_type lu test: # Using -dm_refine 1 -convest_num_refine 3 we get L_2 convergence rate: [0.0057, 1.0] suffix: 2d_q2_p0_conv requires: triangle args: -sol_type linear -dm_plex_simplex 0 \ -field_petscspace_degree 2 -dm_refine 0 -convest_num_refine 1 -snes_convergence_estimate \ -snes_error_if_not_converged \ -ksp_rtol 1e-10 -ksp_error_if_not_converged \ -pc_type fieldsplit -pc_fieldsplit_type schur -pc_fieldsplit_schur_factorization_type full -pc_fieldsplit_schur_precondition full \ -fieldsplit_field_pc_type lu \ -fieldsplit_potential_ksp_rtol 1e-10 -fieldsplit_potential_pc_type lu test: # Using -dm_refine 1 -convest_num_refine 3 we get L_2 convergence rate: [-0.014, 0.0066] suffix: 2d_q2_p0_neumann_conv requires: triangle args: -sol_type quartic_neumann -dm_plex_simplex 0 \ -field_petscspace_degree 2 -dm_refine 0 -convest_num_refine 1 -snes_convergence_estimate \ -snes_error_if_not_converged \ -ksp_rtol 1e-10 -ksp_error_if_not_converged \ -pc_type fieldsplit -pc_fieldsplit_type schur -pc_fieldsplit_schur_factorization_type full -pc_fieldsplit_schur_precondition full \ -fieldsplit_field_pc_type lu \ -fieldsplit_potential_ksp_rtol 1e-10 -fieldsplit_potential_pc_type svd TEST*/ /* These tests will be active once tensor P^- is working test: suffix: 2d_bdmq1_p0_0 requires: triangle args: -dm_plex_simplex 0 -sol_type linear \ -field_petscspace_poly_type pminus_hdiv -field_petscspace_degree 1 -field_petscdualspace_type bdm -dm_refine 0 -convest_num_refine 3 -snes_convergence_estimate \ -dmsnes_check .001 -snes_error_if_not_converged \ -ksp_rtol 1e-10 -ksp_error_if_not_converged \ -pc_type fieldsplit -pc_fieldsplit_type schur -pc_fieldsplit_schur_factorization_type full -pc_fieldsplit_schur_precondition full \ -fieldsplit_field_pc_type lu \ -fieldsplit_potential_ksp_rtol 1e-10 -fieldsplit_potential_pc_type lu test: suffix: 2d_bdmq1_p0_2 requires: triangle args: -dm_plex_simplex 0 -sol_type quartic \ -field_petscspace_poly_type_no pminus_hdiv -field_petscspace_degree 1 -field_petscdualspace_type bdm -dm_refine 0 -convest_num_refine 3 -snes_convergence_estimate \ -dmsnes_check .001 -snes_error_if_not_converged \ -ksp_rtol 1e-10 -ksp_error_if_not_converged \ -pc_type fieldsplit -pc_fieldsplit_type schur -pc_fieldsplit_schur_factorization_type full -pc_fieldsplit_schur_precondition full \ -fieldsplit_field_pc_type lu \ -fieldsplit_potential_ksp_rtol 1e-10 -fieldsplit_potential_pc_type lu */