xref: /libCEED/examples/petsc/qfunctions/area/areasphere.h (revision 32d2ee49b14cb706f4f808410107441006454a20)

// Copyright (c) 2017, Lawrence Livermore National Security, LLC. Produced at
// the Lawrence Livermore National Laboratory. LLNL-CODE-734707. All Rights
// reserved. See files LICENSE and NOTICE for details.
//
// This file is part of CEED, a collection of benchmarks, miniapps, software
// libraries and APIs for efficient high-order finite element and spectral
// element discretizations for exascale applications. For more information and
// source code availability see http://github.com/ceed.
//
// The CEED research is supported by the Exascale Computing Project 17-SC-20-SC,
// a collaborative effort of two U.S. Department of Energy organizations (Office
// of Science and the National Nuclear Security Administration) responsible for
// the planning and preparation of a capable exascale ecosystem, including
// software, applications, hardware, advanced system engineering and early
// testbed platforms, in support of the nation's exascale computing imperative.

/// @file
/// libCEED QFunctions for mass operator example for a scalar field on the sphere using PETSc

#ifndef __CUDACC__
#  include <math.h>
#endif

// *****************************************************************************
// This QFunction sets up the geometric factor required for integration when
//   reference coordinates have a different dimension than the one of
//   pysical coordinates
//
// Reference (parent) 2D coordinates: X \in [-1, 1]^2
//
// Global 3D physical coordinates given by the mesh: xx \in [-R, R]^3
//   with R radius of the sphere
//
// Local 3D physical coordinates on the 2D manifold: x \in [-l, l]^3
//   with l half edge of the cube inscribed in the sphere
//
// Change of coordinates matrix computed by the library:
//   (pysical 3D coords relative to reference 2D coords)
//   dxx_j/dX_i (indicial notation) [3 * 2]
//
// Change of coordinates x (on the 2D manifold) relative to xx (phyisical 3D):
//   dx_i/dxx_j (indicial notation) [3 * 3]
//
// Change of coordinates x (on the 2D manifold) relative to X (reference 2D):
//   (by chain rule)
//   dx_i/dX_j = dx_i/dxx_k * dxx_k/dX_j [3 * 2]
//
// detJ is given by the magnitude of the cross product of the columns of dx_i/dX_j
//
// The quadrature data is stored in the array qdata.
//
// We require the determinant of the Jacobian to properly compute integrals of
//   the form: int( u v )
//
// Qdata: detJ * w
//
// *****************************************************************************

// -----------------------------------------------------------------------------
CEED_QFUNCTION(SetupMassGeoSphere)(void *ctx, const CeedInt Q,
                             const CeedScalar *const *in,
                             CeedScalar *const *out) {
  // Inputs
  const CeedScalar *X = in[0], *J = in[1], *w = in[2];
  // Outputs
  CeedScalar *qdata = out[0];

  // Quadrature Point Loop
  CeedPragmaSIMD
  for (CeedInt i=0; i<Q; i++) {
    // Read global Cartesian coordinates
    const CeedScalar xx[3][1] = {{X[i+0*Q]},
                                 {X[i+1*Q]},
                                 {X[i+2*Q]}
                                };

    // Read dxxdX Jacobian entries, stored as
    // 0 3
    // 1 4
    // 2 5
    const CeedScalar dxxdX[3][2] = {{J[i+Q*0],
                                     J[i+Q*3]},
                                    {J[i+Q*1],
                                     J[i+Q*4]},
                                    {J[i+Q*2],
                                     J[i+Q*5]}
                                   };

    // Setup
    const CeedScalar modxxsq = xx[0][0]*xx[0][0]+xx[1][0]*xx[1][0]+xx[2][0]*xx[2][0];
    CeedScalar xxsq[3][3];
    for (int j=0; j<3; j++)
      for (int k=0; k<3; k++) {
        xxsq[j][k] = 0;
        for (int l=0; l<1; l++)
          xxsq[j][k] += xx[j][l]*xx[k][l] / (sqrt(modxxsq) * modxxsq);
      }

    const CeedScalar dxdxx[3][3] = {{1./sqrt(modxxsq) - xxsq[0][0],
                                     -xxsq[0][1],
                                     -xxsq[0][2]},
                                    {-xxsq[1][0],
                                     1./sqrt(modxxsq) - xxsq[1][1],
                                     -xxsq[1][2]},
                                    {-xxsq[2][0],
                                     -xxsq[2][1],
                                     1./sqrt(modxxsq) - xxsq[2][2]}
                                   };

    CeedScalar dxdX[3][2];
    for (int j=0; j<3; j++)
      for (int k=0; k<2; k++) {
        dxdX[j][k] = 0;
        for (int l=0; l<3; l++)
          dxdX[j][k] += dxdxx[j][l]*dxxdX[l][k];
      }

    // J is given by the cross product of the columns of dxdX
    const CeedScalar J[3][1] = {{dxdX[1][0]*dxdX[2][1] - dxdX[2][0]*dxdX[1][1]},
                                {dxdX[2][0]*dxdX[0][1] - dxdX[0][0]*dxdX[2][1]},
                                {dxdX[0][0]*dxdX[1][1] - dxdX[1][0]*dxdX[0][1]}
                               };
    // Use the magnitude of J as our detJ (volume scaling factor)
    const CeedScalar modJ = sqrt(J[0][0]*J[0][0]+J[1][0]*J[1][0]+J[2][0]*J[2][0]);
    qdata[i+Q*0] = modJ * w[i];

  } // End of Quadrature Point Loop
  return 0;
}
// -----------------------------------------------------------------------------