pmortarassembler.hpp

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// Copyright (c) 2010-2022, Lawrence Livermore National Security, LLC. Produced
// at the Lawrence Livermore National Laboratory. All Rights reserved. See files
// LICENSE and NOTICE for details. LLNL-CODE-806117.
//
// This file is part of the MFEM library. For more information and source code
// availability visit https://mfem.org.
//
// MFEM is free software; you can redistribute it and/or modify it under the
// terms of the BSD-3 license. We welcome feedback and contributions, see file
// CONTRIBUTING.md for details.

#ifndef MFEM_L2P_PAR_MORTAR_ASSEMBLER_HPP
#define MFEM_L2P_PAR_MORTAR_ASSEMBLER_HPP

#include "../../config/config.hpp"

#ifdef MFEM_USE_MPI

#include <memory>
#include <vector>

#include "../fem.hpp"
#include "mortarintegrator.hpp"

namespace mfem
{

/*!
 * @brief This class implements the parallel variational transfer between finite
 * element spaces. Variational transfer has been shown to have better
 * approximation properties than standard interpolation. This facilities can be
 * used for supporting applications which require the handling of non matching
 * meshes. For instance: General multi-physics problems, fluid structure
 * interaction, or even visualization of average quantities within subvolumes. This
 * particular code is also used with LLNL for large scale multilevel Monte Carlo
 * simulations.
 * This algorithm allows to perform quadrature in the intersection of elements
 * of two separate, unrelated, and arbitrarily distributed meshes.
 * It generates quadrature rules in the intersection which allows us to
 * integrate with to machine precision using the mfem::MortarIntegrator
 * interface. See https://doi.org/10.1137/15M1008361 for and in-depth
 * explanation. At this time curved elements are not supported.
 * Convex non-affine elements are partially supported, however, high order (>3)
 * finite element discretizations or nonlinear geometric transformations might
 * generate undesired oscillations. Discontinuous fields in general can only
 * be mapped to order 0 destination fields.
 * For such cases localized versions of the projection will have to be developed.
 */
class ParMortarAssembler
{
public:
   /*!
    * @brief constructs the object with source and destination spaces
    * @param source the source space from where we want to transfer the discrete
    * field
    * @param destination the source space to where we want to transfer the
    * discrete field
    */
   ParMortarAssembler(const std::shared_ptr<ParFiniteElementSpace> &source,
                      const std::shared_ptr<ParFiniteElementSpace> &destination);

   ~ParMortarAssembler();

   /*!
    * @brief assembles the coupling matrix B. B : source -> destination If u is a
    * coefficient associated with source and v with destination Then v = M^(-1) *
    * B * u; where M is the mass matrix in destination. Works with
    * L2_FECollection, H1_FECollection and DG_FECollection (experimental with
    * RT_FECollection and ND_FECollection).
    * @param B the assembled coupling operator. B can be passed uninitialized.
    * @return true if there was an intersection and the operator has been
    * assembled. False otherwise.
    */
   bool Assemble(std::shared_ptr<HypreParMatrix> &B);

   /*!
    * @brief transfer a function from source to destination. if the transfer is
    * to be performed multiple times use Assemble or Update/Apply instead
    * @param src_fun the function associated with the source finite element space
    * @param[out] dest_fun the function associated with the destination finite
    * element space
    * @return true if there was an intersection and the output can be used.
    */
   bool Transfer(const ParGridFunction &src_fun, ParGridFunction &dest_fun);

   /*!
    * @brief transfer a function from source to destination. It requires that
    * the Update function is called before
    * @param src_fun the function associated with the source finite element space
    * @param[out] dest_fun the function associated with the destination finite element space
    * @return true if the transfer was successful, fail otherwise.
    */
   bool Apply(const ParGridFunction &src_fun, ParGridFunction &dest_fun);

   /*!
    * @brief assembles the various components necessary for the transfer.
    * To be called before calling the Apply function if the mesh geometry
    * changed, after previous call. Works with L2_FECollection, H1_FECollection
    * and DG_FECollection (experimental with RT_FECollection and
    * ND_FECollection).
    * @return true if there was an intersection and the operator has been
    * assembled. False otherwise.
    */
   bool Update();

   /*!
    * @brief This method must be called before Assemble or Transfer.
    * It will assemble the operator in all intersections found.
    * @param integrator the integrator object
    */
   void AddMortarIntegrator(const std::shared_ptr<MortarIntegrator> &integrator);

   /*!
    * @brief Expose process details with verbose output
    * @param verbose set to true for verbose output
    */
   void SetVerbose(const bool verbose);


   /*!
    * @brief Control if the Mass matrix is computed together with the coupling
    * operator every time.
    * @param value is set to true for computing the mass matrix operator with
    * the coupling operator, false otherwise.  The option is true by default,
    * set to false if only the coupling operator is needed.
    */
   void SetAssembleMassAndCouplingTogether(const bool value);


   /*!
    * @brief Control the maximum numbers of conjugate gradients steps for mass
    * matrix inversion
    * @param max_solver_iterations the maximum number of iterations
    */
   void SetMaxSolverIterations(const int max_solver_iterations);

   /*!
    * @brief Changes the solver to be used for solving the mass-matrix linear
    * system
    * @param solver new strategy
    */
   void SetSolver(const std::shared_ptr<IterativeSolver> &solver);


   struct Impl;

   private:
   std::unique_ptr<Impl> impl_;
};

} // namespace mfem

#endif // MFEM_USE_MPI
#endif // MFEM_L2P_PAR_MORTAR_ASSEMBLER_HPP