1 #include "h_refinement_study_isentropic_vortex.h" 2 #include "flow_solver/flow_solver_factory.h" 3 #include "flow_solver/flow_solver_cases/periodic_1D_unsteady.h" 4 #include "flow_solver/flow_solver_cases/periodic_entropy_tests.h" 5 #include "physics/exact_solutions/exact_solution.h" 6 #include "physics/euler.h" 13 template <
int dim,
int nstate>
16 const dealii::ParameterHandler ¶meter_handler_input)
18 parameter_handler(parameter_handler_input),
19 n_calculations(parameters_input->time_refinement_study_param.number_of_times_to_solve),
20 refine_ratio(parameters_input->time_refinement_study_param.refinement_ratio)
25 template <
int dim,
int nstate>
35 template <
int dim,
int nstate>
37 double &Lp_error_pressure,
44 std::shared_ptr<ExactSolutionFunction<dim,nstate,double>> exact_solution_function;
46 int overintegrate = 10;
53 double Lp_error_density_local = 0;
54 double Lp_error_pressure_local = 0;
58 dealii::QGauss<dim> quad_extra(dg->max_degree+1+overintegrate);
59 dealii::FEValues<dim,dim> fe_values_extra(*(dg->high_order_grid->mapping_fe_field), dg->fe_collection[dg->max_degree], quad_extra,
60 dealii::update_values | dealii::update_gradients | dealii::update_JxW_values | dealii::update_quadrature_points);
62 const unsigned int n_quad_pts = fe_values_extra.n_quadrature_points;
63 std::array<double,nstate> soln_at_q;
65 std::vector<dealii::types::global_dof_index> dofs_indices (fe_values_extra.dofs_per_cell);
66 for (
auto cell : dg->dof_handler.active_cell_iterators()) {
67 if (!cell->is_locally_owned())
continue;
68 fe_values_extra.reinit (cell);
69 cell->get_dof_indices (dofs_indices);
71 for (
unsigned int iquad=0; iquad<n_quad_pts; ++iquad) {
73 std::fill(soln_at_q.begin(), soln_at_q.end(), 0.0);
75 for (
unsigned int idof=0; idof<fe_values_extra.dofs_per_cell; ++idof) {
76 const unsigned int istate = fe_values_extra.get_fe().system_to_component_index(idof).first;
77 soln_at_q[istate] += dg->solution[dofs_indices[idof]] * fe_values_extra.shape_value_component(idof, iquad, istate);
80 const dealii::Point<dim> qpoint = (fe_values_extra.quadrature_point(iquad));
83 std::array<double,nstate> exact_soln_at_q;
84 for (
unsigned int istate = 0; istate < nstate; ++istate) {
85 exact_soln_at_q[istate] = exact_solution_function->value(qpoint, istate);
88 const double exact_pressure = euler_physics->compute_pressure(exact_soln_at_q);
89 const double pressure = euler_physics->compute_pressure(soln_at_q);
92 Lp_error_density_local += pow(abs(soln_at_q[0] - exact_soln_at_q[0]), norm_p) * fe_values_extra.JxW(iquad);
93 Lp_error_pressure_local += pow(abs(pressure-exact_pressure), norm_p) * fe_values_extra.JxW(iquad);
96 Lp_error_density_local = std::max(abs(soln_at_q[0]-exact_soln_at_q[0]), Lp_error_density_local);
97 Lp_error_pressure_local = std::max(abs(pressure-exact_pressure), Lp_error_pressure_local);
104 Lp_error_density= dealii::Utilities::MPI::sum(Lp_error_density_local, this->
mpi_communicator);
105 Lp_error_density= pow(Lp_error_density, 1.0/((
double)norm_p));
106 Lp_error_pressure = dealii::Utilities::MPI::sum(Lp_error_pressure_local, this->
mpi_communicator);
107 Lp_error_pressure= pow(Lp_error_pressure, 1.0/((
double)norm_p));
110 Lp_error_density = dealii::Utilities::MPI::max(Lp_error_density_local, this->
mpi_communicator);
111 Lp_error_pressure = dealii::Utilities::MPI::max(Lp_error_pressure_local, this->
mpi_communicator);
116 template <
int dim,
int nstate>
122 const int n_steps = floor(final_time/initial_time_step);
123 if (n_steps * initial_time_step != final_time){
124 pcout <<
"WARNING: final_time is not evenly divisible by initial_time_step!" << std::endl
125 <<
"Remainder is " << fmod(final_time, initial_time_step)
126 <<
". Consider modifying parameters." << std::endl;
131 dealii::ConvergenceTable convergence_table_density;
132 dealii::ConvergenceTable convergence_table_pressure;
133 double L2_error_pressure_old = 0;
134 double L2_error_pressure_conv_rate=0;
137 for (
int refinement = 0; refinement <
n_calculations; ++refinement){
139 pcout <<
"\n\n---------------------------------------------" << std::endl;
140 pcout <<
"Refinement number " << refinement <<
" of " << n_calculations - 1 << std::endl;
141 pcout <<
"---------------------------------------------" << std::endl;
145 std::unique_ptr<FlowSolver::PeriodicEntropyTests<dim, nstate>> flow_solver_case = std::make_unique<FlowSolver::PeriodicEntropyTests<dim,nstate>>(¶ms);
147 static_cast<void>(flow_solver->run());
148 pcout <<
"Finished flowsolver " << std::endl;
150 const double final_time_actual = flow_solver->ode_solver->current_time;
152 double L1_error_density=0;
153 double L1_error_pressure=0;
155 double L2_error_density =0;
156 double L2_error_pressure=0;
158 double Linfty_error_density = 0;
159 double Linfty_error_pressure = 0;
161 pcout <<
"Computed density errors are: " << std::endl
162 <<
" L1: " << L1_error_density << std::endl
163 <<
" L2: " << L2_error_density << std::endl
164 <<
" Linfty: " << Linfty_error_density << std::endl;
166 const double dt = flow_solver_case->get_constant_time_step(flow_solver->dg);
168 pcout <<
" at dt = " << dt << std::endl;
171 convergence_table_density.add_value(
"refinement", refinement);
172 convergence_table_density.add_value(
"dt", dt );
173 convergence_table_density.set_precision(
"dt", 16);
174 convergence_table_density.set_scientific(
"dt",
true);
175 convergence_table_density.add_value(
"n_cells",n_cells);
176 convergence_table_density.add_value(
"L1_error_density",L1_error_density);
177 convergence_table_density.set_precision(
"L1_error_density", 16);
178 convergence_table_density.evaluate_convergence_rates(
"L1_error_density",
"n_cells", dealii::ConvergenceTable::reduction_rate_log2, PHILIP_DIM);
179 convergence_table_density.add_value(
"L2_error_density",L2_error_density);
180 convergence_table_density.set_precision(
"L2_error_density", 16);
181 convergence_table_density.evaluate_convergence_rates(
"L2_error_density",
"n_cells", dealii::ConvergenceTable::reduction_rate_log2, PHILIP_DIM);
182 convergence_table_density.add_value(
"Linfty_error_density",Linfty_error_density);
183 convergence_table_density.set_precision(
"Linfty_error_density", 16);
184 convergence_table_density.evaluate_convergence_rates(
"Linfty_error_density",
"n_cells", dealii::ConvergenceTable::reduction_rate_log2, PHILIP_DIM);
187 const double gamma_agg = final_time_actual / (dt * flow_solver->ode_solver->current_iteration);
189 convergence_table_density.add_value(
"gamma_agg",gamma_agg-1.0);
190 convergence_table_density.set_precision(
"gamma_agg", 16);
191 convergence_table_density.evaluate_convergence_rates(
"gamma_agg",
"n_cells", dealii::ConvergenceTable::reduction_rate_log2, PHILIP_DIM);
195 convergence_table_pressure.add_value(
"refinement", refinement);
196 convergence_table_pressure.add_value(
"dt", dt );
197 convergence_table_pressure.set_precision(
"dt", 16);
198 convergence_table_pressure.set_scientific(
"dt",
true);
199 convergence_table_pressure.add_value(
"n_cells",n_cells);
200 convergence_table_pressure.add_value(
"L1_error_pressure",L1_error_pressure);
201 convergence_table_pressure.set_precision(
"L1_error_pressure", 16);
202 convergence_table_pressure.evaluate_convergence_rates(
"L1_error_pressure",
"n_cells", dealii::ConvergenceTable::reduction_rate_log2, PHILIP_DIM);
203 convergence_table_pressure.add_value(
"L2_error_pressure",L2_error_pressure);
204 convergence_table_pressure.set_precision(
"L2_error_pressure", 16);
205 convergence_table_pressure.evaluate_convergence_rates(
"L2_error_pressure",
"n_cells", dealii::ConvergenceTable::reduction_rate_log2, PHILIP_DIM);
206 convergence_table_pressure.add_value(
"Linfty_error_pressure",Linfty_error_pressure);
207 convergence_table_pressure.set_precision(
"Linfty_error_pressure", 16);
208 convergence_table_pressure.evaluate_convergence_rates(
"Linfty_error_pressure",
"n_cells", dealii::ConvergenceTable::reduction_rate_log2, PHILIP_DIM);
213 const double order_tolerance = 1.0;
214 if (refinement > 0) {
215 L2_error_pressure_conv_rate = -log(L2_error_pressure_old/L2_error_pressure)/log(
refine_ratio);
216 pcout <<
"Order for L2 pressure at " << refinement <<
" is " << L2_error_pressure_conv_rate << std::endl;
217 if (abs(L2_error_pressure_conv_rate - expected_order) > order_tolerance){
219 pcout <<
"Expected convergence order for L2 pressure was not reached at refinement " << refinement <<std::endl;
221 if (refinement < n_calculations-1 &&
pcout.is_active()){
223 convergence_table_density.write_text(
pcout.get_stream());
224 convergence_table_pressure.write_text(
pcout.get_stream());
227 L2_error_pressure_old = L2_error_pressure;
232 if (
pcout.is_active()){
233 convergence_table_density.write_text(
pcout.get_stream());
234 convergence_table_pressure.write_text(
pcout.get_stream());
236 std::ofstream conv_tab_file;
237 const std::string fname =
"convergence_tables.txt";
238 conv_tab_file.open(fname);
239 convergence_table_density.write_text(conv_tab_file);
240 convergence_table_pressure.write_text(conv_tab_file);
241 conv_tab_file.close();
double final_time
Final solution time.
int run_test() const override
Run test.
unsigned int number_of_grid_elements_per_dimension
Number of grid elements per dimension for hyper_cube mesh based cases.
h refinement test for the isentropic vortex advection test case.
FlowSolverParam flow_solver_param
Contains the parameters for simulation cases (flow solver test)
const double refine_ratio
Ratio to refine by.
const MPI_Comm mpi_communicator
MPI communicator.
const int n_calculations
Number of times to solve for convergence summary.
Files for the baseline physics.
static std::shared_ptr< ExactSolutionFunction< dim, nstate, real > > create_ExactSolutionFunction(const Parameters::FlowSolverParam &flow_solver_parameters, const double time_compare)
Construct ExactSolutionFunction object from global parameter file.
unsigned int poly_degree
Polynomial order (P) of the basis functions for DG.
Main parameter class that contains the various other sub-parameter classes.
ODESolverParam ode_solver_param
Contains parameters for ODE solver.
const dealii::ParameterHandler & parameter_handler
Parameter handler for storing the .prm file being ran.
double initial_time_step
Time step used in ODE solver.
static std::unique_ptr< FlowSolver< dim, nstate > > select_flow_case(const Parameters::AllParameters *const parameters_input, const dealii::ParameterHandler ¶meter_handler_input)
Factory to return the correct flow solver given input file.
const Parameters::AllParameters *const all_parameters
Pointer to all parameters.
Parameters::AllParameters reinit_params_and_refine(int refinement) const
Reinitialize parameters while refining the timestep. Necessary because all_parameters is constant...
Euler equations. Derived from PhysicsBase.
static std::shared_ptr< PhysicsBase< dim, nstate, real > > create_Physics(const Parameters::AllParameters *const parameters_input, std::shared_ptr< ModelBase< dim, nstate, real > > model_input=nullptr)
Factory to return the correct physics given input file.
ODESolverEnum ode_solver_type
ODE solver type.
std::string unsteady_data_table_filename
dealii::ConditionalOStream pcout
ConditionalOStream.
DGBase is independent of the number of state variables.
void calculate_Lp_error_at_final_time_wrt_function(double &Lp_error_density, double &Lp_error_pressure, std::shared_ptr< DGBase< dim, double >> dg, const Parameters::AllParameters parameters, double final_time, int norm_p) const
Base class of all the tests.
HRefinementStudyIsentropicVortex(const Parameters::AllParameters *const parameters_input, const dealii::ParameterHandler ¶meter_handler_input)
Constructor.