gsVisitorNavierStokes.h

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#pragma once
 
#include <gsAssembler/gsQuadrature.h>
#include <gsCore/gsFuncData.h>
#include <algorithm>
 
#include <gsElasticity/gsBasePde.h>
 
namespace gismo
{
 
template <class T>
class gsVisitorNavierStokes
{
public:
 
    gsVisitorNavierStokes(const gsPde<T> & pde_, const gsMultiPatch<T> & velocity_,
                          const gsMultiPatch<T> & pressure_)
    : dim(), pde_ptr(static_cast<const gsBasePde<T>*>(&pde_)), assemblyType(), patch(),
      viscosity(), forceScaling(), density(),
      N_V(), N_P(), velocity(velocity_), pressure(pressure_)
    {}
 
    void initialize(const gsBasisRefs<T> & basisRefs,
                    const index_t patchIndex,
                    const gsOptionList & options,
                    gsQuadRule<T> & rule)
    {
        GISMO_UNUSED(patchIndex);
        // parametric dimension of the first displacement component
        dim = basisRefs.front().dim();
        // a quadrature rule is defined by the basis for the first velocity component.
        // the same rule is used for the presure
        rule = gsQuadrature::get(basisRefs.front(), options);
        // saving necessary info
        assemblyType = options.getInt("Assembly");
        viscosity = options.getReal("Viscosity");
        density = options.getReal("Density");
        patch = patchIndex;
        forceScaling = options.getReal("ForceScaling");
        // resize containers for global indices
        globalIndices.resize(dim+1);
        blockNumbers.resize(dim+1);
    }
 
    inline void evaluate(const gsBasisRefs<T> & basisRefs,
                         const gsGeometry<T> & geo,
                         const gsMatrix<T> & quNodes)
    {
        // store quadrature points of the element for geometry evaluation
        md.points = quNodes;
        // NEED_VALUE to get points in the physical domain for evaluation of the RHS
        // NEED_MEASURE to get the Jacobian determinant values for integration
        // NEED_GRAD_TRANSFORM to get the Jacobian matrix to transform gradient from the parametric to physical domain
        // NEED_2ND_DER to transform hessians to physical domain
        md.flags = NEED_VALUE | NEED_MEASURE | NEED_GRAD_TRANSFORM;
        // Compute image of the quadrature points plus gradient, jacobian and other necessary data
        geo.computeMap(md);
        // find local indices of the velocity and pressure basis functions active on the element
        basisRefs.front().active_into(quNodes.col(0),localIndicesVel);
        N_V = localIndicesVel.rows();
        basisRefs.back().active_into(quNodes.col(0), localIndicesPres);
        N_P = localIndicesPres.rows();
        // Evaluate velocity basis functions and their derivatives on the element (and hessians, if SUPG is used)
        basisRefs.front().evalAllDers_into(quNodes,1,basisValuesVel);
        // Evaluate pressure basis functions on the element
        basisRefs.back().eval_into(quNodes,basisValuesPres);
        // Evaluate gradients of pressure basis functions if SUPG is used
        basisRefs.back().deriv_into(quNodes,basisGradsPres);
        // Evaluate right-hand side at the image of the quadrature points
        pde_ptr->rhs()->eval_into(md.values[0],forceValues);
        // store quadrature points of the element for velocity evaluation
        mdVelocity.points = quNodes;
        // NEED_VALUE to compute velocity values
        // NEED_DERIV to compute velocity gradient
        // NEED_2ND_DER to compute velocity hessian
        mdVelocity.flags = NEED_VALUE | NEED_DERIV;
        // evaluate velocity
        velocity.patch(patch).computeMap(mdVelocity);
        // evaluate pressure values; for some reason, pressure evaluation via gsMapData doesn't work
        pressure.patch(patch).eval_into(quNodes,pressureValues);
    }
 
    inline void assemble(gsDomainIterator<T> & element,
                         const gsVector<T> & quWeights)
    {
        GISMO_UNUSED(element);
        if (assemblyType == 0)
            assembleOseen(element,quWeights);
        else if (assemblyType == 1)
            assembleNewtonUpdate(element,quWeights);
        else if (assemblyType == 2)
            assembleNewtonFull(element,quWeights);
    }
 
    inline void localToGlobal(const int patchIndex,
                              const std::vector<gsMatrix<T> > & eliminatedDofs,
                              gsSparseSystem<T> & system)
    {
        // computes global indices for velocity components
        for (short_t d = 0; d < dim; ++d)
        {
            system.mapColIndices(localIndicesVel, patchIndex, globalIndices[d], d);
            blockNumbers.at(d) = d;
        }
        // computes global indices for pressure
        system.mapColIndices(localIndicesPres, patchIndex, globalIndices[dim], dim);
        blockNumbers.at(dim) = dim;
        // push to global system
        system.pushToRhs(localRhs,globalIndices,blockNumbers);
        system.pushToMatrix(localMat,globalIndices,eliminatedDofs,blockNumbers,blockNumbers);
    }
 
protected:
 
    void assembleNewtonUpdate(gsDomainIterator<T> & element,
                              const gsVector<T> & quWeights)
    {
        GISMO_UNUSED(element);
        // Initialize local matrix/rhs                     // A | D
        localMat.setZero(dim*N_V + N_P, dim*N_V + N_P);    // --|--    matrix structure
        localRhs.setZero(dim*N_V + N_P,1);                 // B | 0// roughly estimate h - diameter of the element ( for SUPG)
        // T h = cellSize(element);
        // Loop over the quadrature nodes
        for (index_t q = 0; q < quWeights.rows(); ++q)
        {
            // Multiply quadrature weight by the geometry measure
            const T weight = quWeights[q] * md.measure(q);
            // Compute physical gradients of the velocity basis functions at q as a dim x numActiveFunction matrix
            transformGradients(md, q, basisValuesVel[1], physGradVel);
            // Compute physical Jacobian of the current velocity field
            physJacCurVel = mdVelocity.jacobian(q)*(md.jacobian(q).cramerInverse());
            // matrix A: diffusion
            block = weight*density*viscosity * physGradVel.transpose()*physGradVel;
            for (short_t d = 0; d < dim; ++d)
                localMat.block(d*N_V,d*N_V,N_V,N_V) += block.block(0,0,N_V,N_V);
            // matrix A: advection
            block = weight*basisValuesVel[0].col(q) * (mdVelocity.values[0].col(q).transpose()*physGradVel);
            for (short_t d = 0; d < dim; ++d)
                localMat.block(d*N_V,d*N_V,N_V,N_V) += density*block.block(0,0,N_V,N_V);
            // matrix A: reaction
            block = weight*density*basisValuesVel[0].col(q) * basisValuesVel[0].col(q).transpose();
            for (short_t di = 0; di < dim; ++di)
                for (short_t dj = 0; dj < dim; ++dj)
                    localMat.block(di*N_V,dj*N_V,N_V,N_V) += physJacCurVel(di,dj)*block.block(0,0,N_V,N_V);
            // matrices B and D
            for (short_t d = 0; d < dim; ++d)
            {
                block = weight*basisValuesPres.col(q)*physGradVel.row(d);
                localMat.block(dim*N_V,d*N_V,N_P,N_V) -= block.block(0,0,N_P,N_V); // B
                localMat.block(d*N_V,dim*N_V,N_V,N_P) -= block.transpose().block(0,0,N_V,N_P); // D
            }
            // rhs: force
            for (short_t d = 0; d < dim; ++d)
                localRhs.middleRows(d*N_V,N_V).noalias() += weight *density* forceScaling *
                    forceValues(d,q) * basisValuesVel[0].col(q);
            // rhs: residual diffusion
            for (short_t d = 0; d < dim; ++d)
                localRhs.middleRows(d*N_V,N_V).noalias() -= weight * viscosity * density*
                    (physJacCurVel.row(d)*physGradVel).transpose();
            // rhs: residual nonlinear
            for (short_t d = 0; d < dim; ++d)
                localRhs.middleRows(d*N_V,N_V).noalias() -= weight * density*
                    (physJacCurVel.row(d) * mdVelocity.values[0].col(q))(0,0) * basisValuesVel[0].col(q);
            // rhs: residual pressure
            for (short_t d = 0; d < dim; ++d)
                localRhs.middleRows(d*N_V,N_V).noalias() += weight *
                    pressureValues.at(q) * physGradVel.row(d).transpose();
            // rhs: constraint residual
            localRhs.middleRows(dim*N_V,N_P).noalias() += weight *
                basisValuesPres.col(q) * physJacCurVel.trace();
        }
    }
 
    void assembleNewtonFull(gsDomainIterator<T> & element,
                            const gsVector<T> & quWeights)
    {
        GISMO_UNUSED(element);
        // Initialize local matrix/rhs                     // A | D
        localMat.setZero(dim*N_V + N_P, dim*N_V + N_P);    // --|--    matrix structure
        localRhs.setZero(dim*N_V + N_P,1);                 // B | 0// roughly estimate h - diameter of the element ( for SUPG)
        // T h = cellSize(element);
        // Loop over the quadrature nodes
        for (index_t q = 0; q < quWeights.rows(); ++q)
        {
            // Multiply quadrature weight by the geometry measure
            const T weight = quWeights[q] * md.measure(q);
            // Compute physical gradients of the velocity basis functions at q as a dim x numActiveFunction matrix
            transformGradients(md, q, basisValuesVel[1], physGradVel);
            // Compute physical Jacobian of the current velocity field
            physJacCurVel = mdVelocity.jacobian(q)*(md.jacobian(q).cramerInverse());
            // matrix A: diffusion
            block = weight*density*viscosity * physGradVel.transpose()*physGradVel;
            for (short_t d = 0; d < dim; ++d)
                localMat.block(d*N_V,d*N_V,N_V,N_V) += block.block(0,0,N_V,N_V);
            // matrix A: advection
            block = weight*basisValuesVel[0].col(q) * (mdVelocity.values[0].col(q).transpose()*physGradVel);
            for (short_t d = 0; d < dim; ++d)
                localMat.block(d*N_V,d*N_V,N_V,N_V) += density*block.block(0,0,N_V,N_V);
            // matrix A: reaction
            block = weight*density*basisValuesVel[0].col(q) * basisValuesVel[0].col(q).transpose();
            for (short_t di = 0; di < dim; ++di)
                for (short_t dj = 0; dj < dim; ++dj)
                    localMat.block(di*N_V,dj*N_V,N_V,N_V) += physJacCurVel(di,dj)*block.block(0,0,N_V,N_V);
            // matrices B and D
            for (short_t d = 0; d < dim; ++d)
            {
                block = weight*basisValuesPres.col(q)*physGradVel.row(d);
                localMat.block(dim*N_V,d*N_V,N_P,N_V) -= block.block(0,0,N_P,N_V); // B
                localMat.block(d*N_V,dim*N_V,N_V,N_P) -= block.transpose().block(0,0,N_V,N_P); // D
            }
            // rhs: force
            for (short_t d = 0; d < dim; ++d)
                localRhs.middleRows(d*N_V,N_V).noalias() += weight *density* forceScaling *
                    forceValues(d,q) * basisValuesVel[0].col(q);
            // rhs: residual nonlinear
            for (short_t d = 0; d < dim; ++d)
                localRhs.middleRows(d*N_V,N_V).noalias() += weight * density*
                    (physJacCurVel.row(d) * mdVelocity.values[0].col(q))(0,0) * basisValuesVel[0].col(q);
        }
    }
 
    void assembleOseen(gsDomainIterator<T> & element,
                       const gsVector<T> & quWeights)
    {
        GISMO_UNUSED(element);
        // Initialize local matrix/rhs                     // A | D
        localMat.setZero(dim*N_V + N_P, dim*N_V + N_P);    // --|--    matrix structure
        localRhs.setZero(dim*N_V + N_P,1);                 // B | 0
 
        // Loop over the quadrature nodes
        for (index_t q = 0; q < quWeights.rows(); ++q)
        {
            // Multiply quadrature weight by the geometry measure
            const T weight = quWeights[q] * md.measure(q);
            // Compute physical gradients of the velocity basis functions at q as a dim x numActiveFunction matrix
            transformGradients(md, q, basisValuesVel[1], physGradVel);
            // Compute physical Jacobian of the current velocity field
            physJacCurVel = mdVelocity.jacobian(q)*(md.jacobian(q).cramerInverse());
            // matrix A: diffusion
            block = weight*viscosity *density* physGradVel.transpose()*physGradVel;
            for (short_t d = 0; d < dim; ++d)
                localMat.block(d*N_V,d*N_V,N_V,N_V) += block.block(0,0,N_V,N_V);
            // matrix A: advection
            block = weight*basisValuesVel[0].col(q) *
                    (mdVelocity.values[0].col(q).transpose()*physGradVel);
            for (short_t d = 0; d < dim; ++d)
                localMat.block(d*N_V,d*N_V,N_V,N_V) += density*block.block(0,0,N_V,N_V);
            // matrices B and D
            for (short_t d = 0; d < dim; ++d)
            {
                block = weight*basisValuesPres.col(q)*physGradVel.row(d);
                localMat.block(dim*N_V,d*N_V,N_P,N_V) -= block.block(0,0,N_P,N_V); // B
                localMat.block(d*N_V,dim*N_V,N_V,N_P) -= block.transpose().block(0,0,N_V,N_P); // D
            }
            // rhs: force
            for (short_t d = 0; d < dim; ++d)
                localRhs.middleRows(d*N_V,N_V).noalias() += weight *density* forceScaling *
                    forceValues(d,q) * basisValuesVel[0].col(q);
        }
    }
 
protected:
    // problem info
    short_t dim;
    const gsBasePde<T> * pde_ptr;
    // switch between assembling different linear systems (Newton or Oseen iterations)
    index_t assemblyType;
    index_t patch; // current patch
    // constants: viscosity and the force scaling factor
    T viscosity, forceScaling, density;
    // geometry mapping
    gsMapData<T> md;
    // local components of the global linear system
    gsMatrix<T> localMat;
    gsMatrix<T> localRhs;
    // local indices (at the current patch) of basis functions active at the current element
    gsMatrix<index_t> localIndicesVel;
    gsMatrix<index_t> localIndicesPres;
    // number of velocity and pressure basis functions active at the current element
    index_t N_V, N_P;
    // values and derivatives of velocity basis functions at quadrature points at the current element
    // values are stored as a N_V x numQuadPoints matrix; not sure about derivatives, must be smth like N_V*dim x numQuadPoints
    // if supg is true, also stores the hessian
    std::vector<gsMatrix<T> > basisValuesVel;
    // values of pressure basis functions active at the current element;
    // stores as a N_P x numQuadPoints matrix
    gsMatrix<T> basisValuesPres;
    // if supg is true, stores the derivatives
    gsMatrix<T> basisGradsPres;
    // RHS values at quadrature points at the current element; stored as a dim x numQuadPoints matrix
    gsMatrix<T> forceValues;
    // current displacement field
    const gsMultiPatch<T> & velocity;
    // evaluation data of the current velocity field
    gsMapData<T> mdVelocity;
    // current pressure field
    const gsMultiPatch<T> & pressure;
    // pressure values at the current element; stored as a 1 x numQuadPoints matrix
    gsMatrix<T> pressureValues;
    // pressure gradients at the current element (only for supg); stored as a dim x numQuadPoints matrix
    gsMatrix<T> pressureGrads;
 
    // all temporary matrices defined here for efficiency
    gsMatrix<T> block, physGradVel, physJacCurVel;
    // containers for global indices
    std::vector< gsMatrix<index_t> > globalIndices;
    gsVector<index_t> blockNumbers;
};
 
} // namespace gismo