ContField.cpp

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///////////////////////////////////////////////////////////////////////////////
//
// File ContField.cpp
//
// For more information, please see: http://www.nektar.info
//
// The MIT License
//
// Copyright (c) 2006 Division of Applied Mathematics, Brown University (USA),
// Department of Aeronautics, Imperial College London (UK), and Scientific
// Computing and Imaging Institute, University of Utah (USA).
//
// Permission is hereby granted, free of charge, to any person obtaining a
// copy of this software and associated documentation files (the "Software"),
// to deal in the Software without restriction, including without limitation
// the rights to use, copy, modify, merge, publish, distribute, sublicense,
// and/or sell copies of the Software, and to permit persons to whom the
// Software is furnished to do so, subject to the following conditions:
//
// The above copyright notice and this permission notice shall be included
// in all copies or substantial portions of the Software.
//
// THE SOFTWARE IS PROVIDED "AS IS", WITHOUT WARRANTY OF ANY KIND, EXPRESS
// OR IMPLIED, INCLUDING BUT NOT LIMITED TO THE WARRANTIES OF MERCHANTABILITY,
// FITNESS FOR A PARTICULAR PURPOSE AND NONINFRINGEMENT. IN NO EVENT SHALL
// THE AUTHORS OR COPYRIGHT HOLDERS BE LIABLE FOR ANY CLAIM, DAMAGES OR OTHER
// LIABILITY, WHETHER IN AN ACTION OF CONTRACT, TORT OR OTHERWISE, ARISING
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// DEALINGS IN THE SOFTWARE.
//
// Description: Field definition for a continuous domain with boundary
// conditions
//
///////////////////////////////////////////////////////////////////////////////
 
#include <MultiRegions/AssemblyMap/AssemblyMapCG.h>
#include <MultiRegions/ContField.h>
#include <tuple>
 
using namespace std;
 
namespace Nektar
{
namespace MultiRegions
{
/**
 * @class ContField
 * The class #ContField is
 * able to incorporate the boundary conditions imposed to the problem
 * to be solved. Therefore, the class is equipped with three additional
 * data members:
 * - #m_bndCondExpansions
 * - #m_bndTypes
 * - #m_bndCondEquations
 *
 * The first data structure, #m_bndCondExpansions, contains the
 * one-dimensional spectral/hp expansion on the boundary,  #m_bndTypes
 * stores information about the type of boundary condition on the
 * different parts of the boundary while #m_bndCondEquations holds the
 * equation of the imposed boundary conditions.
 *
 * Furthermore, in case of Dirichlet boundary conditions, this class is
 * capable of lifting a known solution satisfying these boundary
 * conditions. If we denote the unknown solution by
 * \f$u^{\mathcal{H}}(\boldsymbol{x})\f$ and the known Dirichlet
 * boundary conditions by \f$u^{\mathcal{D}}(\boldsymbol{x})\f$, the
 * expansion then can be decomposed as
 * \f[ u^{\delta}(\boldsymbol{x}_i)=u^{\mathcal{D}}(\boldsymbol{x}_i)+
 * u^{\mathcal{H}}(\boldsymbol{x}_i)=\sum_{n=0}^{N^{\mathcal{D}}-1}
 * \hat{u}_n^{\mathcal{D}}\Phi_n(\boldsymbol{x}_i)+
 * \sum_{n={N^{\mathcal{D}}}}^{N_{\mathrm{dof}}-1}
 *  \hat{u}_n^{\mathcal{H}} \Phi_n(\boldsymbol{x}_i).\f]
 * This lifting is accomplished by ordering the known global degrees of
 * freedom, prescribed by the Dirichlet boundary conditions, first in
 * the global array
 * \f$\boldsymbol{\hat{u}}\f$, that is,
 * \f[\boldsymbol{\hat{u}}=\left[ \begin{array}{c}
 * \boldsymbol{\hat{u}}^{\mathcal{D}}\\
 * \boldsymbol{\hat{u}}^{\mathcal{H}}
 * \end{array} \right].\f]
 * Such kind of expansions are also referred to as continuous fields.
 * This class should be used when solving 2D problems using a standard
 * Galerkin approach.
 */
 
/**
 *
 */
ContField::ContField()
    : DisContField(), m_locToGloMap(), m_globalMat(),
      m_globalLinSysManager(
          std::bind(&ContField::GenGlobalLinSys, this, std::placeholders::_1),
          std::string("GlobalLinSys"))
{
}
 
/**
 * Given a mesh \a graph, containing information about the domain and
 * the spectral/hp element expansion, this constructor fills the list
 * of local expansions #m_exp with the proper expansions, calculates
 * the total number of quadrature points \f$\boldsymbol{x}_i\f$ and
 * local expansion coefficients \f$\hat{u}^e_n\f$ and allocates memory
 * for the arrays #m_coeffs and #m_phys. Furthermore, it constructs the
 * mapping array (contained in #m_locToGloMap) for the transformation
 * between local elemental level and global level, it calculates the
 * total number global expansion coefficients \f$\hat{u}_n\f$ and
 * allocates memory for the array #m_contCoeffs. The constructor also
 * discretises the boundary conditions, specified by the argument \a
 * bcs, by expressing them in terms of the coefficient of the expansion
 * on the boundary.
 *
 * @param   graph       A mesh, containing information about the domain
 *                      and the spectral/hp element expansion.
 * @param   bcs         The boundary conditions.
 * @param   variable    An optional parameter to indicate for which
 *                      variable the field should be constructed.
 */
ContField::ContField(const LibUtilities::SessionReaderSharedPtr &pSession,
                     const SpatialDomains::MeshGraphSharedPtr &graph,
                     const std::string &variable,
                     const bool DeclareCoeffPhysArrays,
                     const bool CheckIfSingularSystem,
                     const Collections::ImplementationType ImpType)
    : DisContField(pSession, graph, variable, false, DeclareCoeffPhysArrays,
                   ImpType),
      m_globalMat(MemoryManager<GlobalMatrixMap>::AllocateSharedPtr()),
      m_globalLinSysManager(
          std::bind(&ContField::GenGlobalLinSys, this, std::placeholders::_1),
          std::string("GlobalLinSys"))
{
    m_locToGloMap = MemoryManager<AssemblyMapCG>::AllocateSharedPtr(
        m_session, m_ncoeffs, *this, m_bndCondExpansions, m_bndConditions,
        CheckIfSingularSystem, variable, m_periodicVerts, m_periodicEdges,
        m_periodicFaces);
 
    if (m_session->DefinesCmdLineArgument("verbose"))
    {
        m_locToGloMap->PrintStats(std::cout, variable);
    }
}
 
/**
 * Given a mesh \a graph, containing information about the domain and
 * the spectral/hp element expansion, this constructor fills the list
 * of local expansions #m_exp with the proper expansions, calculates
 * the total number of quadrature points \f$\boldsymbol{x}_i\f$ and
 * local expansion coefficients \f$\hat{u}^e_n\f$ and allocates memory
 * for the arrays #m_coeffs and #m_phys. Furthermore, it constructs the
 * mapping array (contained in #m_locToGloMap) for the transformation
 * between local elemental level and global level, it calculates the
 * total number global expansion coefficients \f$\hat{u}_n\f$ and
 * allocates memory for the array #m_coeffs. The constructor also
 * discretises the boundary conditions, specified by the argument \a
 * bcs, by expressing them in terms of the coefficient of the expansion
 * on the boundary.
 *
 * @param   In          Existing ContField object used to provide the
 *                      local to global mapping information and
 *                      global solution type.
 * @param   graph     A mesh, containing information about the domain
 *                      and the spectral/hp element expansion.
 * @param   bcs         The boundary conditions.
 * @param   bc_loc
 */
ContField::ContField(const ContField &In,
                     const SpatialDomains::MeshGraphSharedPtr &graph,
                     const std::string &variable, bool DeclareCoeffPhysArrays,
                     const bool CheckIfSingularSystem)
    : DisContField(In, graph, variable, false, DeclareCoeffPhysArrays),
      m_globalMat(MemoryManager<GlobalMatrixMap>::AllocateSharedPtr()),
      m_globalLinSysManager(
          std::bind(&ContField::GenGlobalLinSys, this, std::placeholders::_1),
          std::string("GlobalLinSys")),
      m_GJPData(In.m_GJPData)
{
    if (!SameTypeOfBoundaryConditions(In) || CheckIfSingularSystem)
    {
        m_locToGloMap = MemoryManager<AssemblyMapCG>::AllocateSharedPtr(
            m_session, m_ncoeffs, *this, m_bndCondExpansions, m_bndConditions,
            CheckIfSingularSystem, variable, m_periodicVerts, m_periodicEdges,
            m_periodicFaces);
 
        if (m_session->DefinesCmdLineArgument("verbose"))
        {
            m_locToGloMap->PrintStats(std::cout, variable);
        }
    }
    else
    {
        m_locToGloMap = In.m_locToGloMap;
    }
}
 
/**
 * Initialises the object as a copy of an existing ContField object.
 * @param   In                       Existing ContField object.
 * @param DeclareCoeffPhysArrays     bool to declare if \a m_phys
 * and \a m_coeffs should be declared. Default is true
 */
ContField::ContField(const ContField &In, bool DeclareCoeffPhysArrays)
    : DisContField(In, DeclareCoeffPhysArrays), m_locToGloMap(In.m_locToGloMap),
      m_globalMat(In.m_globalMat),
      m_globalLinSysManager(In.m_globalLinSysManager), m_GJPData(In.m_GJPData)
{
}
 
/**
 * Constructs a continuous field as a copy of an existing
 * explist  field and adding all the boundary conditions.
 *
 * @param In Existing explist1D field .
 */
ContField::ContField(const LibUtilities::SessionReaderSharedPtr &pSession,
                     const ExpList &In)
    : DisContField(In), m_locToGloMap(),
      m_globalLinSysManager(
          std::bind(&ContField::GenGlobalLinSys, this, std::placeholders::_1),
          std::string("GlobalLinSys"))
{
    m_locToGloMap = MemoryManager<AssemblyMapCG>::AllocateSharedPtr(
        pSession, m_ncoeffs, In);
}
 
/**
 *
 */
ContField::~ContField()
{
}
 
/**
 * Given a function \f$f(\boldsymbol{x})\f$ defined at the quadrature
 * points, this function determines the unknown global coefficients
 * \f$\boldsymbol{\hat{u}}^{\mathcal{H}}\f$ employing a discrete
 * Galerkin projection from physical space to coefficient
 * space. The operation is evaluated by the function #GlobalSolve using
 * the global mass matrix.
 *
 * The values of the function \f$f(\boldsymbol{x})\f$ evaluated at the
 * quadrature points \f$\boldsymbol{x}_i\f$ should be contained in the
 * variable #m_phys of the ExpList object \a Sin. The resulting global
 * coefficients \f$\hat{u}_g\f$ are stored in the array #m_coeffs.
 *
 * @param   Sin         An ExpList, containing the discrete evaluation
 *                      of \f$f(\boldsymbol{x})\f$ at the quadrature
 *                      points in its array #m_phys.
 */
void ContField::FwdTrans(const Array<OneD, const NekDouble> &inarray,
                         Array<OneD, NekDouble> &outarray)
 
{
    // Inner product of forcing
    Array<OneD, NekDouble> wsp(m_ncoeffs);
    IProductWRTBase(inarray, wsp);
 
    // Solve the system
    GlobalLinSysKey key(StdRegions::eMass, m_locToGloMap);
 
    GlobalSolve(key, wsp, outarray);
}
 
/**
 *
 */
void ContField::v_SmoothField(Array<OneD, NekDouble> &field)
{
    int Ncoeffs = m_locToGloMap->GetNumLocalCoeffs();
    Array<OneD, NekDouble> tmp1(Ncoeffs);
    Array<OneD, NekDouble> tmp2(Ncoeffs);
 
    IProductWRTBase(field, tmp1);
    MultiplyByInvMassMatrix(tmp1, tmp2);
    BwdTrans(tmp2, field);
}
 
/**
 * Computes the matrix vector product
 * @f$ \mathbf{y} = \mathbf{M}^{-1}\mathbf{x} @f$.
 *
 * @param   inarray     Input vector @f$\mathbf{x}@f$.
 * @param   outarray    Output vector @f$\mathbf{y}@f$.
 */
void ContField::MultiplyByInvMassMatrix(
    const Array<OneD, const NekDouble> &inarray,
    Array<OneD, NekDouble> &outarray)
 
{
 
    GlobalLinSysKey key(StdRegions::eMass, m_locToGloMap);
    GlobalSolve(key, inarray, outarray);
}
 
/**
 * Consider the two dimensional Laplace equation,
 * \f[\nabla\cdot\left(\boldsymbol{\sigma}\nabla
 * u(\boldsymbol{x})\right) = f(\boldsymbol{x}),\f] supplemented with
 * appropriate boundary conditions (which are contained in the data
 * member #m_bndCondExpansions). In the equation above
 * \f$\boldsymbol{\sigma}\f$ is the (symmetric positive definite)
 * diffusion tensor:
 * \f[ \sigma = \left[ \begin{array}{cc}
 * \sigma_{00}(\boldsymbol{x},t) & \sigma_{01}(\boldsymbol{x},t) \\
 * \sigma_{01}(\boldsymbol{x},t) & \sigma_{11}(\boldsymbol{x},t)
 * \end{array} \right]. \f]
 * Applying a \f$C^0\f$ continuous Galerkin discretisation, this
 * equation leads to the following linear system:
 * \f[\boldsymbol{L}
 * \boldsymbol{\hat{u}}_g=\boldsymbol{\hat{f}}\f]
 * where \f$\boldsymbol{L}\f$ is the Laplacian matrix. This function
 * solves the system above for the global coefficients
 * \f$\boldsymbol{\hat{u}}\f$ by a call to the function #GlobalSolve.
 *
 * The values of the function \f$f(\boldsymbol{x})\f$ evaluated at the
 * quadrature points \f$\boldsymbol{x}_i\f$ should be contained in the
 * variable #m_phys of the ExpList object \a Sin. The resulting global
 * coefficients \f$\boldsymbol{\hat{u}}_g\f$ are stored in the array
 * #m_coeffs.
 *
 * @param   Sin         An ExpList, containing the discrete evaluation
 *                      of the forcing function \f$f(\boldsymbol{x})\f$
 *                      at the quadrature points in its array #m_phys.
 * @param   variablecoeffs The (optional) parameter containing the
 *                      coefficients evaluated at the quadrature
 *                      points. It is an Array of (three) arrays which
 *                      stores the laplacian coefficients in the
 *                      following way
 * \f[\mathrm{variablecoeffs} = \left[ \begin{array}{c}
 * \left[\sigma_{00}(\boldsymbol{x_i},t)\right]_i \\
 * \left[\sigma_{01}(\boldsymbol{x_i},t)\right]_i \\
 * \left[\sigma_{11}(\boldsymbol{x_i},t)\right]_i
 * \end{array}\right]
 * \f]
 * If this argument is not passed to the function, the following
 * equation will be solved:
 * \f[\nabla^2u(\boldsymbol{x}) = f(\boldsymbol{x}),\f]
 *
 * @param   time        The time-level at which the coefficients are
 *                      evaluated
 */
void ContField::LaplaceSolve(
    const Array<OneD, const NekDouble> &inarray,
    Array<OneD, NekDouble> &outarray,
    const Array<OneD, const NekDouble> &dirForcing,
    const Array<OneD, Array<OneD, NekDouble>> &variablecoeffs, NekDouble time)
{
    // Inner product of forcing
    Array<OneD, NekDouble> wsp(m_ncoeffs);
    IProductWRTBase(inarray, wsp);
 
    // Note -1.0 term necessary to invert forcing function to
    // be consistent with matrix definition
    Vmath::Neg(m_ncoeffs, wsp, 1);
 
    // Forcing function with weak boundary conditions
    int i, j;
    int bndcnt = 0;
    Array<OneD, NekDouble> sign =
        m_locToGloMap->GetBndCondCoeffsToLocalCoeffsSign();
    const Array<OneD, const int> map =
        m_locToGloMap->GetBndCondCoeffsToLocalCoeffsMap();
 
    // Add weak boundary conditions to forcing
    for (i = 0; i < m_bndCondExpansions.size(); ++i)
    {
        if (m_bndConditions[i]->GetBoundaryConditionType() ==
                SpatialDomains::eNeumann ||
            m_bndConditions[i]->GetBoundaryConditionType() ==
                SpatialDomains::eRobin)
        {
            const Array<OneD, NekDouble> bndcoeff =
                (m_bndCondExpansions[i])->GetCoeffs();
 
            if (m_locToGloMap->GetSignChange())
            {
                for (j = 0; j < (m_bndCondExpansions[i])->GetNcoeffs(); j++)
                {
                    wsp[map[bndcnt + j]] += sign[bndcnt + j] * bndcoeff[j];
                }
            }
            else
            {
                for (j = 0; j < (m_bndCondExpansions[i])->GetNcoeffs(); j++)
                {
                    wsp[map[bndcnt + j]] += bndcoeff[bndcnt + j];
                }
            }
        }
 
        bndcnt += m_bndCondExpansions[i]->GetNcoeffs();
    }
 
    StdRegions::VarCoeffMap varcoeffs;
    varcoeffs[StdRegions::eVarCoeffD00] = variablecoeffs[0];
    varcoeffs[StdRegions::eVarCoeffD01] = variablecoeffs[1];
    varcoeffs[StdRegions::eVarCoeffD11] = variablecoeffs[3];
    varcoeffs[StdRegions::eVarCoeffD22] = variablecoeffs[5];
    StdRegions::ConstFactorMap factors;
    factors[StdRegions::eFactorTime] = time;
 
    // Solve the system
    GlobalLinSysKey key(StdRegions::eLaplacian, m_locToGloMap, factors,
                        varcoeffs);
 
    GlobalSolve(key, wsp, outarray, dirForcing);
}
 
/**
 * Constructs the GlobalLinearSysKey for the linear advection operator
 * with the supplied parameters, and computes the eigenvectors and
 * eigenvalues of the associated matrix.
 * @param   ax          Advection parameter, x.
 * @param   ay          Advection parameter, y.
 * @param   Real        Computed eigenvalues, real component.
 * @param   Imag        Computed eigenvalues, imag component.
 * @param   Evecs       Computed eigenvectors.
 */
void ContField::LinearAdvectionEigs(const NekDouble ax, const NekDouble ay,
                                    Array<OneD, NekDouble> &Real,
                                    Array<OneD, NekDouble> &Imag,
                                    Array<OneD, NekDouble> &Evecs)
{
    // Solve the system
    Array<OneD, Array<OneD, NekDouble>> vel(2);
    Array<OneD, NekDouble> vel_x(m_npoints, ax);
    Array<OneD, NekDouble> vel_y(m_npoints, ay);
    vel[0] = vel_x;
    vel[1] = vel_y;
 
    StdRegions::VarCoeffMap varcoeffs;
    varcoeffs[StdRegions::eVarCoeffVelX] =
        Array<OneD, NekDouble>(m_npoints, ax);
    varcoeffs[StdRegions::eVarCoeffVelY] =
        Array<OneD, NekDouble>(m_npoints, ay);
    StdRegions::ConstFactorMap factors;
    factors[StdRegions::eFactorTime] = 0.0;
    GlobalLinSysKey key(StdRegions::eLinearAdvectionReaction, m_locToGloMap,
                        factors, varcoeffs);
 
    DNekMatSharedPtr Gmat = GenGlobalMatrixFull(key, m_locToGloMap);
    Gmat->EigenSolve(Real, Imag, Evecs);
}
 
/**
 * Given a linear system specified by the key \a key,
 * \f[\boldsymbol{M}\boldsymbol{\hat{u}}_g=\boldsymbol{\hat{f}},\f]
 * this function solves this linear system taking into account the
 * boundary conditions specified in the data member
 * #m_bndCondExpansions. Therefore, it adds an array
 * \f$\boldsymbol{\hat{g}}\f$ which represents the non-zero surface
 * integral resulting from the weak boundary conditions (e.g. Neumann
 * boundary conditions) to the right hand side, that is,
 * \f[\boldsymbol{M}\boldsymbol{\hat{u}}_g=\boldsymbol{\hat{f}}+
 * \boldsymbol{\hat{g}}.\f]
 * Furthermore, it lifts the known degrees of freedom which are
 * prescribed by the Dirichlet boundary conditions. As these known
 * coefficients \f$\boldsymbol{\hat{u}}^{\mathcal{D}}\f$ are numbered
 * first in the global coefficient array \f$\boldsymbol{\hat{u}}_g\f$,
 * the linear system can be decomposed as,
 * \f[\left[\begin{array}{cc}
 * \boldsymbol{M}^{\mathcal{DD}}&\boldsymbol{M}^{\mathcal{DH}}\\
 * \boldsymbol{M}^{\mathcal{HD}}&\boldsymbol{M}^{\mathcal{HH}}
 * \end{array}\right]
 * \left[\begin{array}{c}
 * \boldsymbol{\hat{u}}^{\mathcal{D}}\\
 * \boldsymbol{\hat{u}}^{\mathcal{H}}
 * \end{array}\right]=
 * \left[\begin{array}{c}
 * \boldsymbol{\hat{f}}^{\mathcal{D}}\\
 * \boldsymbol{\hat{f}}^{\mathcal{H}}
 * \end{array}\right]+
 * \left[\begin{array}{c}
 * \boldsymbol{\hat{g}}^{\mathcal{D}}\\
 * \boldsymbol{\hat{g}}^{\mathcal{H}}
 * \end{array}\right]
 * \f]
 * which will then be solved for the unknown coefficients
 * \f$\boldsymbol{\hat{u}}^{\mathcal{H}}\f$ as,
 * \f[
 * \boldsymbol{M}^{\mathcal{HH}}\boldsymbol{\hat{u}}^{\mathcal{H}}=
 * \boldsymbol{\hat{f}}^{\mathcal{H}}+
 * \boldsymbol{\hat{g}}^{\mathcal{H}}-
 * \boldsymbol{M}^{\mathcal{HD}}\boldsymbol{\hat{u}}^{\mathcal{D}}\f]
 *
 * @param   mkey        This key uniquely defines the linear system to
 *                      be solved.
 * @param   locrhs      contains the forcing term in local coefficient space
 * @note    inout contains initial guess and final output in local coeffs.
 */
void ContField::GlobalSolve(const GlobalLinSysKey &key,
                            const Array<OneD, const NekDouble> &locrhs,
                            Array<OneD, NekDouble> &inout,
                            const Array<OneD, const NekDouble> &dirForcing)
{
    int NumDirBcs   = m_locToGloMap->GetNumGlobalDirBndCoeffs();
    int contNcoeffs = m_locToGloMap->GetNumGlobalCoeffs();
 
    // STEP 1: SET THE DIRICHLET DOFS TO THE RIGHT VALUE
    //         IN THE SOLUTION ARRAY
    v_ImposeDirichletConditions(inout);
 
    // STEP 2: CALCULATE THE HOMOGENEOUS COEFFICIENTS
    if (contNcoeffs - NumDirBcs > 0)
    {
        GlobalLinSysSharedPtr LinSys = GetGlobalLinSys(key);
        LinSys->Solve(locrhs, inout, m_locToGloMap, dirForcing);
    }
}
 
/**
 * Returns the global matrix associated with the given GlobalMatrixKey.
 * If the global matrix has not yet been constructed on this field,
 * it is first constructed using GenGlobalMatrix().
 * @param   mkey        Global matrix key.
 * @returns Assocated global matrix.
 */
GlobalMatrixSharedPtr ContField::GetGlobalMatrix(const GlobalMatrixKey &mkey)
{
    ASSERTL1(mkey.LocToGloMapIsDefined(),
             "To use method must have a AssemblyMap "
             "attached to key");
 
    GlobalMatrixSharedPtr glo_matrix;
    auto matrixIter = m_globalMat->find(mkey);
 
    if (matrixIter == m_globalMat->end())
    {
        glo_matrix           = GenGlobalMatrix(mkey, m_locToGloMap);
        (*m_globalMat)[mkey] = glo_matrix;
    }
    else
    {
        glo_matrix = matrixIter->second;
    }
 
    return glo_matrix;
}
 
/**
 * The function searches the map #m_globalLinSys to see if the
 * global matrix has been created before. If not, it calls the function
 * #GenGlobalLinSys to generate the requested global system.
 *
 * @param   mkey        This key uniquely defines the requested
 *                      linear system.
 */
GlobalLinSysSharedPtr ContField::GetGlobalLinSys(const GlobalLinSysKey &mkey)
{
    return m_globalLinSysManager[mkey];
}
 
GlobalLinSysSharedPtr ContField::GenGlobalLinSys(const GlobalLinSysKey &mkey)
{
    ASSERTL1(mkey.LocToGloMapIsDefined(),
             "To use method must have a AssemblyMap "
             "attached to key");
    return ExpList::GenGlobalLinSys(mkey, m_locToGloMap);
}
 
/**
 *
 */
void ContField::v_FwdTrans(const Array<OneD, const NekDouble> &inarray,
                           Array<OneD, NekDouble> &outarray)
{
    FwdTrans(inarray, outarray);
}
 
void ContField::v_ImposeDirichletConditions(Array<OneD, NekDouble> &outarray)
{
    int i, j;
    int bndcnt = 0;
 
    Array<OneD, NekDouble> sign =
        m_locToGloMap->GetBndCondCoeffsToLocalCoeffsSign();
    const Array<OneD, const int> map =
        m_locToGloMap->GetBndCondCoeffsToLocalCoeffsMap();
 
    for (i = 0; i < m_bndCondExpansions.size(); ++i)
    {
        if (m_bndConditions[i]->GetBoundaryConditionType() ==
            SpatialDomains::eDirichlet)
        {
            const Array<OneD, NekDouble> bndcoeff =
                (m_bndCondExpansions[i])->GetCoeffs();
 
            if (m_locToGloMap->GetSignChange())
            {
                for (j = 0; j < (m_bndCondExpansions[i])->GetNcoeffs(); j++)
                {
                    outarray[map[bndcnt + j]] = sign[bndcnt + j] * bndcoeff[j];
                }
            }
            else
            {
                for (j = 0; j < (m_bndCondExpansions[i])->GetNcoeffs(); j++)
                {
                    outarray[map[bndcnt + j]] = bndcoeff[j];
                }
            }
        }
        bndcnt += m_bndCondExpansions[i]->GetNcoeffs();
    }
 
    // communicate local Dirichlet coeffs that are just
    // touching a dirichlet boundary on another partition
    set<int> &ParallelDirBndSign = m_locToGloMap->GetParallelDirBndSign();
 
    for (auto &it : ParallelDirBndSign)
    {
        outarray[it] *= -1;
    }
 
    m_locToGloMap->UniversalAbsMaxBnd(outarray);
 
    for (auto &it : ParallelDirBndSign)
    {
        outarray[it] *= -1;
    }
 
    set<ExtraDirDof> &copyLocalDirDofs = m_locToGloMap->GetCopyLocalDirDofs();
    for (auto &it : copyLocalDirDofs)
    {
        outarray[std::get<0>(it)] = outarray[std::get<1>(it)] * std::get<2>(it);
    }
}
 
void ContField::v_FillBndCondFromField(void)
{
    int bndcnt = 0;
 
    Array<OneD, NekDouble> sign =
        m_locToGloMap->GetBndCondCoeffsToLocalCoeffsSign();
    const Array<OneD, const int> bndmap =
        m_locToGloMap->GetBndCondCoeffsToLocalCoeffsMap();
 
    for (int i = 0; i < m_bndCondExpansions.size(); ++i)
    {
        Array<OneD, NekDouble> &coeffs = m_bndCondExpansions[i]->UpdateCoeffs();
 
        if (m_locToGloMap->GetSignChange())
        {
            for (int j = 0; j < (m_bndCondExpansions[i])->GetNcoeffs(); ++j)
            {
                coeffs[j] = sign[bndcnt + j] * m_coeffs[bndmap[bndcnt + j]];
            }
        }
        else
        {
            for (int j = 0; j < (m_bndCondExpansions[i])->GetNcoeffs(); ++j)
            {
                coeffs[j] = m_coeffs[bndmap[bndcnt + j]];
            }
        }
 
        bndcnt += m_bndCondExpansions[i]->GetNcoeffs();
    }
}
 
void ContField::v_FillBndCondFromField(const int nreg)
{
    int bndcnt = 0;
 
    ASSERTL1(nreg < m_bndCondExpansions.size(),
             "nreg is out or range since this many boundary "
             "regions to not exist");
 
    Array<OneD, NekDouble> sign =
        m_locToGloMap->GetBndCondCoeffsToLocalCoeffsSign();
    const Array<OneD, const int> bndmap =
        m_locToGloMap->GetBndCondCoeffsToLocalCoeffsMap();
 
    // Now fill in all other Dirichlet coefficients.
    Array<OneD, NekDouble> &coeffs = m_bndCondExpansions[nreg]->UpdateCoeffs();
 
    for (int j = 0; j < nreg; ++j)
    {
        bndcnt += m_bndCondExpansions[j]->GetNcoeffs();
    }
 
    if (m_locToGloMap->GetSignChange())
    {
        for (int j = 0; j < (m_bndCondExpansions[nreg])->GetNcoeffs(); ++j)
        {
            coeffs[j] = sign[bndcnt + j] * m_coeffs[bndmap[bndcnt + j]];
        }
    }
    else
    {
        for (int j = 0; j < (m_bndCondExpansions[nreg])->GetNcoeffs(); ++j)
        {
            coeffs[j] = m_coeffs[bndmap[bndcnt + j]];
        }
    }
}
 
/**
 * This operation is evaluated as:
 * \f{tabbing}
 * \hspace{1cm}  \= Do \= $e=$  $1, N_{\mathrm{el}}$ \\
 * > > Do \= $i=$  $0,N_m^e-1$ \\
 * > > > $\boldsymbol{\hat{u}}^{e}[i] = \mbox{sign}[e][i] \cdot
 * \boldsymbol{\hat{u}}_g[\mbox{map}[e][i]]$ \\
 * > > continue \\
 * > continue
 * \f}
 * where \a map\f$[e][i]\f$ is the mapping array and \a
 * sign\f$[e][i]\f$ is an array of similar dimensions ensuring the
 * correct modal connectivity between the different elements (both
 * these arrays are contained in the data member #m_locToGloMap). This
 * operation is equivalent to the scatter operation
 * \f$\boldsymbol{\hat{u}}_l=\mathcal{A}\boldsymbol{\hat{u}}_g\f$,
 * where \f$\mathcal{A}\f$ is the
 * \f$N_{\mathrm{eof}}\times N_{\mathrm{dof}}\f$ permutation matrix.
 *
 * @note The array #m_coeffs should be filled with the global
 * coefficients \f$\boldsymbol{\hat{u}}_g\f$ and that the resulting
 * local coefficients \f$\boldsymbol{\hat{u}}_l\f$ will be stored in
 * #m_coeffs.
 */
void ContField::v_GlobalToLocal(const Array<OneD, const NekDouble> &inarray,
                                Array<OneD, NekDouble> &outarray)
{
    m_locToGloMap->GlobalToLocal(inarray, outarray);
}
 
void ContField::v_GlobalToLocal(void)
{
    m_locToGloMap->GlobalToLocal(m_coeffs, m_coeffs);
}
 
/**
 * This operation is evaluated as:
 * \f{tabbing}
 * \hspace{1cm}  \= Do \= $e=$  $1, N_{\mathrm{el}}$ \\
 * > > Do \= $i=$  $0,N_m^e-1$ \\
 * > > > $\boldsymbol{\hat{u}}_g[\mbox{map}[e][i]] =
 * \mbox{sign}[e][i] \cdot \boldsymbol{\hat{u}}^{e}[i]$\\
 * > > continue\\
 * > continue
 * \f}
 * where \a map\f$[e][i]\f$ is the mapping array and \a
 * sign\f$[e][i]\f$ is an array of similar dimensions ensuring the
 * correct modal connectivity between the different elements (both
 * these arrays are contained in the data member #m_locToGloMap). This
 * operation is equivalent to the gather operation
 * \f$\boldsymbol{\hat{u}}_g=\mathcal{A}^{-1}\boldsymbol{\hat{u}}_l\f$,
 * where \f$\mathcal{A}\f$ is the
 * \f$N_{\mathrm{eof}}\times N_{\mathrm{dof}}\f$ permutation matrix.
 *
 * @note The array #m_coeffs should be filled with the local
 *          coefficients \f$\boldsymbol{\hat{u}}_l\f$ and that
 *          the resulting global coefficients
 *          \f$\boldsymbol{\hat{u}}_g\f$ will be stored in
 *          #m_coeffs. Also if useComm is set to false then no
 *          communication call will be made to check if all
 *          values are consistent over processors
 */
 
void ContField::v_LocalToGlobal(const Array<OneD, const NekDouble> &inarray,
                                Array<OneD, NekDouble> &outarray, bool useComm)
{
    m_locToGloMap->LocalToGlobal(inarray, outarray, useComm);
}
 
void ContField::v_LocalToGlobal(bool useComm)
 
{
    m_locToGloMap->LocalToGlobal(m_coeffs, m_coeffs, useComm);
}
 
/**
 *
 */
void ContField::v_MultiplyByInvMassMatrix(
    const Array<OneD, const NekDouble> &inarray,
    Array<OneD, NekDouble> &outarray)
{
    MultiplyByInvMassMatrix(inarray, outarray);
}
 
/**
 * Consider the two dimensional Helmholtz equation,
 * \f[\nabla^2u(\boldsymbol{x})-\lambda u(\boldsymbol{x})
 * = f(\boldsymbol{x}),\f] supplemented with appropriate boundary
 * conditions (which are contained in the data member
 * #m_bndCondExpansions). Applying a \f$C^0\f$ continuous Galerkin
 * discretisation, this equation leads to the following linear system:
 * \f[\left(\boldsymbol{L}+\lambda\boldsymbol{M}\right)
 * \boldsymbol{\hat{u}}_g=\boldsymbol{\hat{f}}\f] where
 * \f$\boldsymbol{L}\f$ and \f$\boldsymbol{M}\f$ are the Laplacian and
 * mass matrix respectively. This function solves the system above for
 * the global coefficients \f$\boldsymbol{\hat{u}}\f$ by a call to the
 * function #GlobalSolve. It is assumed #m_coeff contains an
 * initial estimate for the solution.
 *
 * The values of the function \f$f(\boldsymbol{x})\f$
 * evaluated at the quadrature points \f$\boldsymbol{x}_i\f$
 * should be contained in the variable #m_phys of the ExpList
 * object \a inarray.
 *
 * @param   inarray     An ExpList, containing the discrete evaluation
 *                      of the forcing function \f$f(\boldsymbol{x})\f$
 *                      at the quadrature points in its array #m_phys.
 * @param   factors    The parameter \f$\lambda\f$ of the Helmholtz
 *                      equation is specified through the factors map
 */
void ContField::v_HelmSolve(const Array<OneD, const NekDouble> &inarray,
                            Array<OneD, NekDouble> &outarray,
                            const StdRegions::ConstFactorMap &factors,
                            const StdRegions::VarCoeffMap &pvarcoeff,
                            const MultiRegions::VarFactorsMap &varfactors,
                            const Array<OneD, const NekDouble> &dirForcing,
                            const bool PhysSpaceForcing)
 
{
    int i, j;
 
    //----------------------------------
    //  Setup RHS Inner product
    //----------------------------------
    // Inner product of forcing
    Array<OneD, NekDouble> wsp(m_ncoeffs);
    if (PhysSpaceForcing)
    {
        IProductWRTBase(inarray, wsp);
        // Note -1.0 term necessary to invert forcing function to
        // be consistent with matrix definition
        Vmath::Neg(m_ncoeffs, wsp, 1);
    }
    else
    {
        Vmath::Smul(m_ncoeffs, -1.0, inarray, 1, wsp, 1);
    }
 
    int bndcnt = 0;
    Array<OneD, NekDouble> sign =
        m_locToGloMap->GetBndCondCoeffsToLocalCoeffsSign();
    const Array<OneD, const int> map =
        m_locToGloMap->GetBndCondCoeffsToLocalCoeffsMap();
    // Add weak boundary conditions to forcing
    for (i = 0; i < m_bndCondExpansions.size(); ++i)
    {
        if (m_bndConditions[i]->GetBoundaryConditionType() ==
                SpatialDomains::eNeumann ||
            m_bndConditions[i]->GetBoundaryConditionType() ==
                SpatialDomains::eRobin)
        {
            const Array<OneD, NekDouble> bndcoeff =
                (m_bndCondExpansions[i])->GetCoeffs();
 
            if (m_locToGloMap->GetSignChange())
            {
                for (j = 0; j < (m_bndCondExpansions[i])->GetNcoeffs(); j++)
                {
                    wsp[map[bndcnt + j]] += sign[bndcnt + j] * bndcoeff[j];
                }
            }
            else
            {
                for (j = 0; j < (m_bndCondExpansions[i])->GetNcoeffs(); j++)
                {
                    wsp[map[bndcnt + j]] += bndcoeff[j];
                }
            }
        }
        bndcnt += m_bndCondExpansions[i]->GetNcoeffs();
    }
 
    StdRegions::MatrixType mtype = StdRegions::eHelmholtz;
 
    StdRegions::VarCoeffMap varcoeff(pvarcoeff);
    if (factors.count(StdRegions::eFactorGJP))
    {
        // initialize if required
        if (!m_GJPData)
        {
            m_GJPData = MemoryManager<GJPStabilisation>::AllocateSharedPtr(
                GetSharedThisPtr());
        }
 
        if (m_GJPData->IsSemiImplicit())
        {
            mtype = StdRegions::eHelmholtzGJP;
        }
 
        // to set up forcing need initial guess in physical space
        Array<OneD, NekDouble> phys(m_npoints), tmp;
        BwdTrans(outarray, phys);
        NekDouble scale = -1.0 * factors.find(StdRegions::eFactorGJP)->second;
 
        m_GJPData->Apply(
            phys, wsp,
            pvarcoeff.count(StdRegions::eVarCoeffGJPNormVel)
                ? pvarcoeff.find(StdRegions::eVarCoeffGJPNormVel)->second
                : NullNekDouble1DArray,
            scale);
 
        varcoeff.erase(StdRegions::eVarCoeffGJPNormVel);
    }
 
    GlobalLinSysKey key(mtype, m_locToGloMap, factors, varcoeff, varfactors);
 
    GlobalSolve(key, wsp, outarray, dirForcing);
}
 
/**
 * First compute the inner product of forcing function with respect to
 * base, and then solve the system with the linear advection operator.
 * @param   velocity    Array of advection velocities in physical space
 * @param   inarray     Forcing function.
 * @param   outarray    Result.
 * @param   lambda      reaction coefficient
 * @param   dirForcing  Dirichlet Forcing.
 */
 
// could combine this with HelmholtzCG.
void ContField::v_LinearAdvectionDiffusionReactionSolve(
    const Array<OneD, Array<OneD, NekDouble>> &velocity,
    const Array<OneD, const NekDouble> &inarray,
    Array<OneD, NekDouble> &outarray, const NekDouble lambda,
    const Array<OneD, const NekDouble> &dirForcing)
{
    // Inner product of forcing
    Array<OneD, NekDouble> wsp(m_ncoeffs);
    IProductWRTBase(inarray, wsp);
 
    // Note -1.0 term necessary to invert forcing function to
    // be consistent with matrix definition
    Vmath::Neg(m_ncoeffs, wsp, 1);
 
    // Forcing function with weak boundary conditions
    int i, j;
    int bndcnt = 0;
    Array<OneD, NekDouble> sign =
        m_locToGloMap->GetBndCondCoeffsToLocalCoeffsSign();
    const Array<OneD, const int> map =
        m_locToGloMap->GetBndCondCoeffsToLocalCoeffsMap();
    // Add weak boundary conditions to forcing
    for (i = 0; i < m_bndCondExpansions.size(); ++i)
    {
        if (m_bndConditions[i]->GetBoundaryConditionType() ==
                SpatialDomains::eNeumann ||
            m_bndConditions[i]->GetBoundaryConditionType() ==
                SpatialDomains::eRobin)
        {
            const Array<OneD, NekDouble> bndcoeff =
                (m_bndCondExpansions[i])->GetCoeffs();
 
            if (m_locToGloMap->GetSignChange())
            {
                for (j = 0; j < (m_bndCondExpansions[i])->GetNcoeffs(); j++)
                {
                    wsp[map[bndcnt + j]] += sign[bndcnt + j] * bndcoeff[j];
                }
            }
            else
            {
                for (j = 0; j < (m_bndCondExpansions[i])->GetNcoeffs(); j++)
                {
                    wsp[map[bndcnt + j]] += bndcoeff[bndcnt + j];
                }
            }
        }
 
        bndcnt += m_bndCondExpansions[i]->GetNcoeffs();
    }
 
    // Solve the system
    StdRegions::ConstFactorMap factors;
    factors[StdRegions::eFactorLambda] = lambda;
    StdRegions::VarCoeffMap varcoeffs;
    varcoeffs[StdRegions::eVarCoeffVelX] = velocity[0];
    varcoeffs[StdRegions::eVarCoeffVelY] = velocity[1];
    if (m_expType == e3D)
    {
        varcoeffs[StdRegions::eVarCoeffVelZ] = velocity[2];
    }
 
    GlobalLinSysKey key(StdRegions::eLinearAdvectionDiffusionReaction,
                        m_locToGloMap, factors, varcoeffs);
 
    GlobalSolve(key, wsp, outarray, dirForcing);
}
 
/**
 * First compute the inner product of forcing function with respect to
 * base, and then solve the system with the linear advection operator.
 * @param   velocity    Array of advection velocities in physical space
 * @param   inarray     Forcing function.
 * @param   outarray    Result.
 * @param   lambda      reaction coefficient
 * @param   dirForcing  Dirichlet Forcing.
 */
void ContField::v_LinearAdvectionReactionSolve(
    const Array<OneD, Array<OneD, NekDouble>> &velocity,
    const Array<OneD, const NekDouble> &inarray,
    Array<OneD, NekDouble> &outarray, const NekDouble lambda,
    const Array<OneD, const NekDouble> &dirForcing)
{
    // Inner product of forcing
    Array<OneD, NekDouble> wsp(m_ncoeffs);
    IProductWRTBase(inarray, wsp);
 
    // Solve the system
    StdRegions::ConstFactorMap factors;
    factors[StdRegions::eFactorLambda] = lambda;
    StdRegions::VarCoeffMap varcoeffs;
    varcoeffs[StdRegions::eVarCoeffVelX] = velocity[0];
    varcoeffs[StdRegions::eVarCoeffVelY] = velocity[1];
    GlobalLinSysKey key(StdRegions::eLinearAdvectionReaction, m_locToGloMap,
                        factors, varcoeffs);
 
    GlobalSolve(key, wsp, outarray, dirForcing);
}
 
/**
 *
 */
const Array<OneD, const SpatialDomains::BoundaryConditionShPtr>
    &ContField::v_GetBndConditions()
{
    return GetBndConditions();
}
 
/**
 * Reset the GlobalLinSys Manager
 */
void ContField::v_ClearGlobalLinSysManager(void)
{
    m_globalLinSysManager.ClearManager("GlobalLinSys");
}
 
} // namespace MultiRegions
} // namespace Nektar