void Shader::compileFlat() {
if (shader != 0) return;
shader = glCreateShaderObjectARB(shaderType());
if (shader == 0) {
throw std::runtime_error("failed to create shader object");
}
std::list<std::string> all_source;
s_tag++;
_source(all_source);
std::ostringstream _prog;
std::copy(all_source.begin(), all_source.end(), std::ostream_iterator<std::string>(_prog, "\n"));
GLint length = _prog.str().size();
const char *_p = _prog.str().c_str();
glShaderSourceARB(shader, 1, &_p, &length);
glCompileShaderARB(shader);
GLint compile_status = 0;
glGetObjectParameterivARB(shader, GL_OBJECT_COMPILE_STATUS_ARB, &compile_status);
if (compile_status == 0) {
std::ostringstream err;
err << "failed to compile shader:" << std::endl << "----" << std::endl << glsl_log(shader) << std::endl << "----" << std::endl;
glDeleteObjectARB(shader);
shader = 0;
throw std::runtime_error(err.str());
}
}
/**
* @brief Returns the source for some energy group for a flat source region
* @param fsr_id the ID for the FSR of interest
* @param energy_group the energy group of interest
* @return the flat source region source
*/
FP_PRECISION CPUSolver::getFSRSource(int fsr_id, int energy_group) {
/* Error checking */
if (fsr_id >= _num_FSRs)
log_printf(ERROR, "Unable to return a source for FSR ID = %d in energy "
"group %d since the solver only contains FSR with IDs less than "
"or equal to %d", fsr_id, energy_group, _num_FSRs-1);
if (fsr_id < 0)
log_printf(ERROR, "Unable to return a source for FSR ID = %d "
"in energy group %d since FSRs do not have negative IDs",
fsr_id, energy_group);
if (energy_group-1 >= _num_groups)
log_printf(ERROR, "Unable to return a source for FSR ID = %d "
"in energy group %d since the solver only has %d energy "
"groups", fsr_id, energy_group, _num_groups);
if (energy_group <= 0)
log_printf(ERROR, "Unable to return a source for FSR ID = %d "
"in energy group %d since energy groups are greater than "
"or equal to 1", fsr_id, energy_group);
return _source(fsr_id,energy_group-1);
}
/**
* @brief Set the source for each FSR and energy group to some value.
* @param value the value to assign to each FSR source
*/
void CPUSolver::flattenFSRSources(FP_PRECISION value) {
#pragma omp parallel for schedule(guided)
for (int r=0; r < _num_FSRs; r++) {
for (int e=0; e < _num_groups; e++) {
_source(r,e) = value;
_old_source(r,e) = value;
}
}
return;
}
void HeatTransferSource<SourceFunction>::element_time_derivative( bool /*compute_jacobian*/,
AssemblyContext& context,
CachedValues& /*cache*/ )
{
#ifdef GRINS_USE_GRVY_TIMERS
this->_timer->BeginTimer("HeatTransferSource::element_time_derivative");
#endif
// The number of local degrees of freedom in each variable.
const unsigned int n_T_dofs = context.get_dof_indices(_temp_vars.T_var()).size();
// Element Jacobian * quadrature weights for interior integration.
const std::vector<libMesh::Real> &JxW =
context.get_element_fe(_temp_vars.T_var())->get_JxW();
// The temperature shape functions at interior quadrature points.
const std::vector<std::vector<libMesh::Real> >& T_phi =
context.get_element_fe(_temp_vars.T_var())->get_phi();
// Locations of quadrature points
const std::vector<libMesh::Point>& x_qp = context.get_element_fe(_temp_vars.T_var())->get_xyz();
// Get residuals
libMesh::DenseSubVector<libMesh::Number> &FT = context.get_elem_residual(_temp_vars.T_var()); // R_{T}
// Now we will build the element Jacobian and residual.
// Constructing the residual requires the solution and its
// gradient from the previous timestep. This must be
// calculated at each quadrature point by summing the
// solution degree-of-freedom values by the appropriate
// weight functions.
unsigned int n_qpoints = context.get_element_qrule().n_points();
for (unsigned int qp=0; qp != n_qpoints; qp++)
{
libMesh::Real q = _source( x_qp[qp] );
for (unsigned int i=0; i != n_T_dofs; i++)
{
FT(i) += q*T_phi[i][qp]*JxW[qp];
}
}
#ifdef GRINS_USE_GRVY_TIMERS
this->_timer->EndTimer("HeatTransferSource::element_time_derivative");
#endif
return;
}
/**
* @brief Computes the total source (fission and scattering) in each FSR.
* @details This method computes the total source in each FSR based on
* this iteration's current approximation to the scalar flux. A
* residual for the source with respect to the source compute on
* the previous iteration is computed and returned. The residual
* is determined as follows:
* /f$ res = \sqrt{\frac{\displaystyle\sum \displaystyle\sum
* \left(\frac{Q^i - Q^{i-1}{Q^i}\right)^2}{\# FSRs}}} \f$
*
* @return the residual between this source and the previous source
*/
FP_PRECISION CPUSolver::computeFSRSources() {
int tid;
Material* material;
FP_PRECISION scatter_source;
FP_PRECISION fission_source;
FP_PRECISION* nu_sigma_f;
FP_PRECISION* sigma_s;
FP_PRECISION* sigma_t;
FP_PRECISION* chi;
FP_PRECISION source_residual = 0.0;
FP_PRECISION inverse_k_eff = 1.0 / _k_eff;
/* For all FSRs, find the source */
#pragma omp parallel for private(tid, material, nu_sigma_f, chi, \
sigma_s, sigma_t, fission_source, scatter_source) schedule(guided)
for (int r=0; r < _num_FSRs; r++) {
tid = omp_get_thread_num();
material = _FSR_materials[r];
nu_sigma_f = material->getNuSigmaF();
chi = material->getChi();
sigma_s = material->getSigmaS();
sigma_t = material->getSigmaT();
/* Initialize the source residual to zero */
_source_residuals[r] = 0.;
/* Compute fission source for each group */
if (material->isFissionable()) {
for (int e=0; e < _num_groups; e++)
_fission_sources(r,e) = _scalar_flux(r,e) * nu_sigma_f[e];
fission_source = pairwise_sum<FP_PRECISION>(&_fission_sources(r,0),
_num_groups);
fission_source *= inverse_k_eff;
}
else
fission_source = 0.0;
/* Compute total scattering source for group G */
for (int G=0; G < _num_groups; G++) {
scatter_source = 0;
for (int g=0; g < _num_groups; g++)
_scatter_sources(tid,g) = sigma_s[G*_num_groups+g] * _scalar_flux(r,g);
scatter_source=pairwise_sum<FP_PRECISION>(&_scatter_sources(tid,0),
_num_groups);
/* Set the total source for FSR r in group G */
_source(r,G) = (fission_source * chi[G] + scatter_source) *
ONE_OVER_FOUR_PI;
_reduced_source(r,G) = _source(r,G) / sigma_t[G];
/* Compute the norm of residual of the source in the FSR */
if (fabs(_source(r,G)) > 1E-10)
_source_residuals[r] += pow((_source(r,G) - _old_source(r,G))
/ _source(r,G), 2);
/* Update the old source */
_old_source(r,G) = _source(r,G);
}
}
/* Sum up the residuals from each FSR */
source_residual = pairwise_sum<FP_PRECISION>(_source_residuals, _num_FSRs);
source_residual = sqrt(source_residual / (_num_FSRs * _num_groups));
return source_residual;
}
/**
* @brief Computes the total source (fission and scattering) in each FSR.
* @details This method computes the total source in each FSR based on
* this iteration's current approximation to the scalar flux. A
* residual for the source with respect to the source compute on
* the previous iteration is computed and returned. The residual
* is determined as follows:
* /f$ res = \sqrt{\frac{\displaystyle\sum \displaystyle\sum
* \left(\frac{Q^i - Q^{i-1}{Q^i}\right)^2}{# FSRs}}} \f$
*
* @return the residual between this source and the previous source
*/
FP_PRECISION VectorizedSolver::computeFSRSources() {
int tid;
FP_PRECISION scatter_source;
FP_PRECISION fission_source;
FP_PRECISION* nu_sigma_f;
FP_PRECISION* sigma_s;
FP_PRECISION* sigma_t;
FP_PRECISION* chi;
Material* material;
FP_PRECISION source_residual = 0.0;
FP_PRECISION inverse_k_eff = 1.0 / _k_eff;
/* For all FSRs, find the source */
#pragma omp parallel for private(material, nu_sigma_f, chi, \
sigma_s, sigma_t, fission_source, scatter_source) schedule(guided)
for (int r=0; r < _num_FSRs; r++) {
tid = omp_get_thread_num();
material = _FSR_materials[r];
nu_sigma_f = material->getNuSigmaF();
chi = material->getChi();
sigma_s = material->getSigmaS();
sigma_t = material->getSigmaT();
/* Initialize the source residual to zero */
_source_residuals[r] = 0.;
/* Compute fission source for each group */
if (material->isFissionable()) {
for (int v=0; v < _num_vector_lengths; v++) {
/* Compute fission source for each group */
#pragma simd vectorlength(VEC_LENGTH)
for (int e=v*VEC_LENGTH; e < (v+1)*VEC_LENGTH; e++)
_fission_sources(r,e) = _scalar_flux(r,e) * nu_sigma_f[e];
}
#ifdef SINGLE
fission_source = cblas_sasum(_num_groups, &_fission_sources(r,0),1);
#else
fission_source = cblas_dasum(_num_groups, &_fission_sources(r,0),1);
#endif
fission_source *= inverse_k_eff;
}
else
fission_source = 0.0;
/* Compute total scattering source for group G */
for (int G=0; G < _num_groups; G++) {
scatter_source = 0;
for (int v=0; v < _num_vector_lengths; v++) {
#pragma simd vectorlength(VEC_LENGTH)
for (int g=v*VEC_LENGTH; g < (v+1)*VEC_LENGTH; g++)
_scatter_sources(tid,g) = sigma_s[G*_num_groups+g] *
_scalar_flux(r,g);
}
#ifdef SINGLE
scatter_source=cblas_sasum(_num_groups,&_scatter_sources(tid,0),1);
#else
scatter_source=cblas_dasum(_num_groups,&_scatter_sources(tid,0),1);
#endif
/* Set the total source for FSR r in group G */
_source(r,G) = (fission_source * chi[G] + scatter_source)
* ONE_OVER_FOUR_PI;
_reduced_source(r,G) = _source(r,G) / sigma_t[G];
/* Compute the norm of residual of the source in the FSR */
if (fabs(_source(r,G)) > 1E-10)
_source_residuals[r] += pow((_source(r,G) - _old_source(r,G))
/ _source(r,G), 2);
/* Update the old source */
_old_source(r,G) = _source(r,G);
}
}
/* Sum up the residuals from each group and in each FSR */
#ifdef SINGLE
source_residual = cblas_sasum(_num_FSRs,_source_residuals,1);
#else
source_residual = cblas_dasum(_num_FSRs,_source_residuals,1);
#endif
source_residual = sqrt(source_residual / (_num_groups * _num_FSRs));
return source_residual;
}
