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Periodic mesh bugfix and test #884
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@@ -53,13 +53,28 @@ double StateManager::newDataCollection(const std::string& name, const std::optio | |
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// Functional needs the nodal grid function and neighbor data in the mesh | ||
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// Determine if the existing nodal grid function is discontinuous. This | ||
// indicates that the mesh is periodic and the new nodal grid function must also | ||
// be discontinuous. | ||
bool is_discontinuous = false; | ||
auto nodes = mesh(name).GetNodes(); | ||
if (nodes) { | ||
is_discontinuous = nodes->FESpace()->FEColl()->GetContType() == mfem::FiniteElementCollection::DISCONTINUOUS; | ||
SLIC_WARNING_ROOT( | ||
"Periodic mesh detected! This will only work on translational periodic surfaces for vector H1 fields and " | ||
"has not been thoroughly tested. Proceed at your own risk."); | ||
} | ||
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// This mfem call ensures the mesh contains an H1 grid function describing nodal | ||
// cordinates. The parameters do the following: | ||
// 1. Sets the order of the mesh to p = 1 | ||
// 2. Uses a continuous (i.e. H1) finite element space | ||
// 2. Uses the existing continuity of the mesh finite element space (periodic meshes are discontinuous) | ||
// 3. Uses the spatial dimension as the mesh dimension (i.e. it is not a lower dimension manifold) | ||
// 4. Uses nodal instead of VDIM ordering (i.e. xxxyyyzzz instead of xyzxyzxyz) | ||
mesh(name).SetCurvature(1, false, -1, mfem::Ordering::byNODES); | ||
mesh(name).SetCurvature(1, is_discontinuous, -1, mfem::Ordering::byNODES); | ||
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// Sidre will destruct the nodal grid function instead of the mesh | ||
mesh(name).SetNodesOwner(false); | ||
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// Generate the face neighbor information in the mesh. This is needed by the face restriction | ||
// operators used by Functional | ||
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@@ -221,6 +236,29 @@ void StateManager::save(const double t, const int cycle, const std::string& mesh | |
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mfem::ParMesh* StateManager::setMesh(std::unique_ptr<mfem::ParMesh> pmesh, const std::string& mesh_tag) | ||
{ | ||
// Determine if the existing nodal grid function is discontinuous. This | ||
// indicates that the mesh is periodic and the new nodal grid function must also | ||
// be discontinuous. | ||
bool is_discontinuous = false; | ||
auto nodes = pmesh->GetNodes(); | ||
There was a problem hiding this comment. Choose a reason for hiding this commentThe reason will be displayed to describe this comment to others. Learn more. Can't I've asked mfem to clarify the preconditions of this function before, but it's still essentially undocumented. There was a problem hiding this comment. Choose a reason for hiding this commentThe reason will be displayed to describe this comment to others. Learn more. Yes. However, if it is a periodic mesh this will be non-null as it needs the discontinuous basis function. That is why I have the default of false on line 239. There was a problem hiding this comment. Choose a reason for hiding this commentThe reason will be displayed to describe this comment to others. Learn more. Ah, I misunderstood what this was doing |
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if (nodes) { | ||
is_discontinuous = nodes->FESpace()->FEColl()->GetContType() == mfem::FiniteElementCollection::DISCONTINUOUS; | ||
SLIC_WARNING_ROOT( | ||
"Periodic mesh detected! This will only work on translational periodic surfaces for vector H1 fields and " | ||
"has not been thoroughly tested. Proceed at your own risk."); | ||
} | ||
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// This mfem call ensures the mesh contains an H1 grid function describing nodal | ||
// cordinates. The parameters do the following: | ||
// 1. Sets the order of the mesh to p = 1 | ||
// 2. Uses the existing continuity of the mesh finite element space (periodic meshes are discontinuous) | ||
// 3. Uses the spatial dimension as the mesh dimension (i.e. it is not a lower dimension manifold) | ||
// 4. Uses nodal instead of VDIM ordering (i.e. xxxyyyzzz instead of xyzxyzxyz) | ||
pmesh->SetCurvature(1, is_discontinuous, -1, mfem::Ordering::byNODES); | ||
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// Sidre will destruct the nodal grid function instead of the mesh | ||
pmesh->SetNodesOwner(false); | ||
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newDataCollection(mesh_tag); | ||
auto& datacoll = datacolls_.at(mesh_tag); | ||
datacoll.SetMesh(pmesh.release()); | ||
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@@ -229,14 +267,6 @@ mfem::ParMesh* StateManager::setMesh(std::unique_ptr<mfem::ParMesh> pmesh, const | |
// Functional needs the nodal grid function and neighbor data in the mesh | ||
auto& new_pmesh = mesh(mesh_tag); | ||
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// This mfem call ensures the mesh contains an H1 grid function describing nodal | ||
// cordinates. The parameters do the following: | ||
// 1. Sets the order of the mesh to p = 1 | ||
// 2. Uses a continuous (i.e. H1) finite element space | ||
// 3. Uses the spatial dimension as the mesh dimension (i.e. it is not a lower dimension manifold) | ||
// 4. Uses nodal instead of VDIM ordering (i.e. xxxyyyzzz instead of xyzxyzxyz) | ||
new_pmesh.SetCurvature(1, false, -1, mfem::Ordering::byNODES); | ||
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// Generate the face neighbor information in the mesh. This is needed by the face restriction | ||
// operators used by Functional | ||
new_pmesh.ExchangeFaceNbrData(); | ||
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@@ -0,0 +1,129 @@ | ||
// Copyright (c) 2019-2023, Lawrence Livermore National Security, LLC and | ||
// other Serac Project Developers. See the top-level LICENSE file for | ||
// details. | ||
// | ||
// SPDX-License-Identifier: (BSD-3-Clause) | ||
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#include <fstream> | ||
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#include "axom/slic/core/SimpleLogger.hpp" | ||
#include <gtest/gtest.h> | ||
#include "mfem.hpp" | ||
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#include "serac/serac_config.hpp" | ||
#include "serac/mesh/mesh_utils.hpp" | ||
#include "serac/physics/solid_mechanics.hpp" | ||
#include "serac/physics/materials/solid_material.hpp" | ||
#include "serac/physics/materials/parameterized_solid_material.hpp" | ||
#include "serac/physics/state/state_manager.hpp" | ||
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namespace serac { | ||
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using solid_mechanics::default_static_options; | ||
using solid_mechanics::direct_static_options; | ||
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TEST(SolidMechanics, Periodic) | ||
{ | ||
MPI_Barrier(MPI_COMM_WORLD); | ||
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int serial_refinement = 0; | ||
int parallel_refinement = 0; | ||
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// Create DataStore | ||
axom::sidre::DataStore datastore; | ||
serac::StateManager::initialize(datastore, "solid_periodic"); | ||
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// Construct the appropriate dimension mesh and give it to the data store | ||
int nElem = 2; | ||
double lx = 3.0e-1, ly = 3.0e-1, lz = 0.25e-1; | ||
auto initial_mesh = | ||
mfem::Mesh(mfem::Mesh::MakeCartesian3D(4 * nElem, 4 * nElem, nElem, mfem::Element::HEXAHEDRON, lx, ly, lz)); | ||
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// Create translation vectors defining the periodicity | ||
mfem::Vector x_translation({lx, 0.0, 0.0}); | ||
std::vector<mfem::Vector> translations = {x_translation}; | ||
double tol = 1e-6; | ||
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std::vector<int> periodicMap = initial_mesh.CreatePeriodicVertexMapping(translations, tol); | ||
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// Create the periodic mesh using the vertex mapping defined by the translation vectors | ||
auto periodic_mesh = mfem::Mesh::MakePeriodic(initial_mesh, periodicMap); | ||
auto mesh = mesh::refineAndDistribute(std::move(periodic_mesh), serial_refinement, parallel_refinement); | ||
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serac::StateManager::setMesh(std::move(mesh)); | ||
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constexpr int p = 1; | ||
constexpr int dim = 3; | ||
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// Construct and initialized the user-defined moduli to be used as a differentiable parameter in | ||
// the solid physics module. | ||
FiniteElementState user_defined_shear_modulus(StateManager::newState( | ||
FiniteElementState::Options{.order = 1, .element_type = ElementType::L2, .name = "parameterized_shear"})); | ||
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double shear_modulus_value = 1.0; | ||
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user_defined_shear_modulus = shear_modulus_value; | ||
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FiniteElementState user_defined_bulk_modulus(StateManager::newState( | ||
FiniteElementState::Options{.order = 1, .element_type = ElementType::L2, .name = "parameterized_bulk"})); | ||
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double bulk_modulus_value = 1.0; | ||
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user_defined_bulk_modulus = bulk_modulus_value; | ||
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// Construct a functional-based solid solver | ||
SolidMechanics<p, dim, Parameters<L2<p>, L2<p>>> solid_solver(default_static_options, GeometricNonlinearities::On, | ||
"solid_periodic"); | ||
solid_solver.setParameter(0, user_defined_bulk_modulus); | ||
solid_solver.setParameter(1, user_defined_shear_modulus); | ||
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solid_mechanics::ParameterizedNeoHookeanSolid<dim> mat{1.0, 0.0, 0.0}; | ||
solid_solver.setMaterial(DependsOn<0, 1>{}, mat); | ||
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// Boundary conditions: | ||
// Prescribe zero displacement at the supported end of the beam | ||
std::set<int> support = {2}; | ||
auto zero_displacement = [](const mfem::Vector&, mfem::Vector& u) -> void { u = 0.0; }; | ||
solid_solver.setDisplacementBCs(support, zero_displacement); | ||
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double iniDispVal = 5.0e-6; | ||
auto ini_displacement = [iniDispVal](const mfem::Vector&, mfem::Vector& u) -> void { u = iniDispVal; }; | ||
solid_solver.setDisplacement(ini_displacement); | ||
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tensor<double, dim> constant_force; | ||
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constant_force[0] = 0.0; | ||
constant_force[1] = 1.0e-2; | ||
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if (dim == 3) { | ||
constant_force[2] = 0.0; | ||
} | ||
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solid_mechanics::ConstantBodyForce<dim> force{constant_force}; | ||
solid_solver.addBodyForce(force); | ||
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// Finalize the data structures | ||
solid_solver.completeSetup(); | ||
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// Perform the quasi-static solve | ||
double dt = 1.0; | ||
solid_solver.advanceTimestep(dt); | ||
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// Output the sidre-based plot files | ||
solid_solver.outputState(); | ||
} | ||
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} // namespace serac | ||
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int main(int argc, char* argv[]) | ||
{ | ||
::testing::InitGoogleTest(&argc, argv); | ||
MPI_Init(&argc, &argv); | ||
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axom::slic::SimpleLogger logger; | ||
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int result = RUN_ALL_TESTS(); | ||
MPI_Finalize(); | ||
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return result; | ||
} |
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Can these two duplicate sections be unified into a function w/o too much effort?