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Peano
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Data Structures | |
| class | SolverVariant |
Functions | |
| create_abstract_solver_declarations (flux_implementation, ncp_implementation, eigenvalues_implementation, source_term_implementation, point_source_implementation, pde_terms_without_state) | |
| create_abstract_solver_definitions (flux_implementation, ncp_implementation, eigenvalues_implementation, source_term_implementation, point_source_implementation, pde_terms_without_state) | |
| create_solver_declarations (flux_implementation, ncp_implementation, eigenvalues_implementation, source_term_implementation, point_source_implementation, pde_terms_without_state) | |
| create_solver_definitions (flux_implementation, ncp_implementation, eigenvalues_implementation, source_term_implementation, point_source_implementation, pde_terms_without_state) | |
| get_face_merge_implementation (patch_overlap) | |
| create_start_time_step_implementation_for_fixed_time_stepping (normalised_time_step_size) | |
| We roll over all reduced data after the last time step, and we plot status info in the first step. | |
| create_volumetric_solver_call (polynomial_basis, solver_variant) | |
| A set of default volumetric kernel calls. | |
| create_add_solver_contributions_call (polynomial_basis) | |
| create_multiply_with_inverted_mass_matrix_call (polynomial_basis) | |
| exahype2.solvers.rkdg.kernels.create_abstract_solver_declarations | ( | flux_implementation, | |
| ncp_implementation, | |||
| eigenvalues_implementation, | |||
| source_term_implementation, | |||
| point_source_implementation, | |||
| pde_terms_without_state ) |
Definition at line 19 of file kernels.py.
| exahype2.solvers.rkdg.kernels.create_abstract_solver_definitions | ( | flux_implementation, | |
| ncp_implementation, | |||
| eigenvalues_implementation, | |||
| source_term_implementation, | |||
| point_source_implementation, | |||
| pde_terms_without_state ) |
Definition at line 218 of file kernels.py.
| exahype2.solvers.rkdg.kernels.create_add_solver_contributions_call | ( | polynomial_basis | ) |
Definition at line 1039 of file kernels.py.
| exahype2.solvers.rkdg.kernels.create_multiply_with_inverted_mass_matrix_call | ( | polynomial_basis | ) |
Definition at line 1068 of file kernels.py.
| exahype2.solvers.rkdg.kernels.create_solver_declarations | ( | flux_implementation, | |
| ncp_implementation, | |||
| eigenvalues_implementation, | |||
| source_term_implementation, | |||
| point_source_implementation, | |||
| pde_terms_without_state ) |
Definition at line 428 of file kernels.py.
| exahype2.solvers.rkdg.kernels.create_solver_definitions | ( | flux_implementation, | |
| ncp_implementation, | |||
| eigenvalues_implementation, | |||
| source_term_implementation, | |||
| point_source_implementation, | |||
| pde_terms_without_state ) |
Definition at line 673 of file kernels.py.
| exahype2.solvers.rkdg.kernels.create_start_time_step_implementation_for_fixed_time_stepping | ( | normalised_time_step_size | ) |
We roll over all reduced data after the last time step, and we plot status info in the first step.
Definition at line 892 of file kernels.py.
| exahype2.solvers.rkdg.kernels.create_volumetric_solver_call | ( | polynomial_basis, | |
| solver_variant ) |
A set of default volumetric kernel calls.
You might want to use different solver calls in your code depending on the context.
In the FV code base, I need the implementation routines as argument: As we work with FV, the generic FV class does not know which implementations are around. If you work with a domain-specific Rusanov solver, e.g., then there is no such thing as an ncp.
For the DG schemes, things are different: Every DG solver in ExaHyPE 2 in principle supports the ncp. So the base Python class already instantiates the corresponding dictionary entries, and we can use them straightaway.
solver_variant: SolverVariant Picks different implementation variants
Definition at line 921 of file kernels.py.
| exahype2.solvers.rkdg.kernels.get_face_merge_implementation | ( | patch_overlap | ) |
Definition at line 858 of file kernels.py.