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Peano
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Variables | |
int | dimensions = 2 |
int | patch_size = 16 |
int | depth = 5 |
float | end_time = 1.0 |
list | size = [10.0, 10.0, 10.0] |
list | offset = [0.0, 0.0, 0.0] |
float | time_in_between_two_snapshots = end_time / 10 |
string | compile_mode = "Release" |
my_project | |
my_solver | |
my_pde | |
p = my_pde.name_Q_entry(0, "p") | |
v = my_pde.name_Q_entries(1, dimensions, "v") | |
rho = sympy.symbols("rho") | |
c = sympy.symbols("c") | |
K0 = rho * c * c | |
sigma = sympy.symbols("sigma") | |
t0 = sympy.symbols("t0") | |
M0 = sympy.symbols("M0") | |
t = sympy.symbols("t") | |
max_h = sympy.symbols("MaxAdmissibleVolumeH") | |
force = M0 * sympy.exp(-((t - t0) * (t - t0)) / (2.0 * sigma * sigma)) | |
point_source = sympy.sqrt((5 - my_pde.x[0]) ** 2 + (5 - my_pde.x[1]) ** 2) | |
initial_conditions | |
boundary_conditions | |
flux | |
max_eigenvalue | |
source_term | |
plot_description | |
min_end_time | |
max_end_time | |
first_plot_time_stamp | |
time_in_between_plots | |
periodic_BC | |
mode | |
make | |
True | |
make_clean_first | |
throw_away_data_after_build | |
acoustic.boundary_conditions |
Definition at line 187 of file acoustic.py.
acoustic.c = sympy.symbols("c") |
Definition at line 89 of file acoustic.py.
Referenced by airfoilSymmetric(), TP::TwoPunctures.C_To_c(), TP::Utilities.chder(), TP::Utilities.chebev(), TP::Utilities.chebft_Extremes(), TP::Utilities.chebft_Zeros(), Numerics.computeParameters(), Numerics.getStiffnessTensor(), TP::error.incase(), TP::TwoPunctures.interpol(), TP::TwoPunctures.PunctTaylorExpandAtArbitPosition(), and TP::error.unless().
string acoustic.compile_mode = "Release" |
Definition at line 51 of file acoustic.py.
int acoustic.depth = 5 |
Definition at line 29 of file acoustic.py.
Referenced by applyBoundaryConditionsToAxis(), TP::Utilities.d3tensor(), and benchmarks::exahype2::kernelbenchmarks::DataRepository::Indexing.linearise().
acoustic.dimensions = 2 |
Definition at line 19 of file acoustic.py.
float acoustic.end_time = 1.0 |
Definition at line 34 of file acoustic.py.
acoustic.first_plot_time_stamp |
Definition at line 213 of file acoustic.py.
acoustic.flux |
Definition at line 188 of file acoustic.py.
Definition at line 158 of file acoustic.py.
acoustic.initial_conditions |
Definition at line 186 of file acoustic.py.
Definition at line 90 of file acoustic.py.
Referenced by examples::exahype2::mgccz4.source().
acoustic.M0 = sympy.symbols("M0") |
Definition at line 154 of file acoustic.py.
acoustic.make |
Definition at line 251 of file acoustic.py.
acoustic.make_clean_first |
Definition at line 251 of file acoustic.py.
acoustic.max_eigenvalue |
Definition at line 189 of file acoustic.py.
acoustic.max_end_time |
Definition at line 212 of file acoustic.py.
acoustic.max_h = sympy.symbols("MaxAdmissibleVolumeH") |
Definition at line 157 of file acoustic.py.
acoustic.min_end_time |
Definition at line 211 of file acoustic.py.
acoustic.mode |
Definition at line 235 of file acoustic.py.
acoustic.my_pde |
Definition at line 82 of file acoustic.py.
acoustic.my_project |
Definition at line 57 of file acoustic.py.
acoustic.my_solver |
Definition at line 69 of file acoustic.py.
acoustic.offset = [0.0, 0.0, 0.0] |
Definition at line 40 of file acoustic.py.
acoustic.p = my_pde.name_Q_entry(0, "p") |
Definition at line 85 of file acoustic.py.
Referenced by TP::TwoPunctures.bicgstab(), ContextCurvilinear< Shortcuts, basisSize, numberOfData, T >.correctPointSourceLocation(), TP::TwoPunctures.Derivatives_AB3(), ellipsoidTransform(), ellipsoidTransformInverse(), projection::albers_equal_area::ellipsoid.forward(), projection::albers_equal_area::sphere.forward(), TP::TwoPunctures.Interpolate(), projection::albers_equal_area::ellipsoid.inverse(), projection::albers_equal_area::sphere.inverse(), TP::TwoPunctures.PunctEvalAtArbitPosition(), TP::TwoPunctures.PunctEvalAtArbitPositionFast(), TP::TwoPunctures.PunctEvalAtArbitPositionFaster(), TP::TwoPunctures.PunctEvalAtArbitPositionFasterLowRes(), riemannSolver.riemannSolver_BC0(), riemannSolver.riemannSolver_Nodal(), Numerics.riemannSolverBC0(), Numerics.riemannSolverNodal(), TP::TwoPunctures.SpecCoef(), sphereTransform(), and sphereTransformInverse().
int acoustic.patch_size = 16 |
Definition at line 24 of file acoustic.py.
acoustic.periodic_BC |
Definition at line 215 of file acoustic.py.
acoustic.plot_description |
Definition at line 197 of file acoustic.py.
acoustic.point_source = sympy.sqrt((5 - my_pde.x[0]) ** 2 + (5 - my_pde.x[1]) ** 2) |
Definition at line 161 of file acoustic.py.
acoustic.rho = sympy.symbols("rho") |
Definition at line 88 of file acoustic.py.
Referenced by TP::TwoPunctures.bicgstab(), and Numerics.computeParameters().
acoustic.sigma = sympy.symbols("sigma") |
Definition at line 152 of file acoustic.py.
Referenced by Numerics.computeTractions(), Numerics.riemannSolver(), ContextDynamicRupture< Shortcuts, basisSize, numberOfVariables, numberOfParameters, T >.riemannSolver(), riemannSolver.riemannSolver_BC0(), riemannSolver.riemannSolver_BCn(), Numerics.riemannSolverBC0(), and Numerics.riemannSolverBCn().
acoustic.size = [10.0, 10.0, 10.0] |
Definition at line 39 of file acoustic.py.
acoustic.source_term |
Definition at line 190 of file acoustic.py.
acoustic.t = sympy.symbols("t") |
Definition at line 155 of file acoustic.py.
Referenced by examples::exahype2::mgccz4::FiniteVolumeMGCCZ4.adjustSolution(), examples::exahype2::mgccz4::ADERDGMGCCZ4.adjustSolution(), airfoilSymmetric(), examples::exahype2::mgccz4::ADERDGMGCCZ4.algebraicSource(), applyBoundaryConditions(), applyBoundaryConditionsToAxis(), TP::TwoPunctures.bicgstab(), applications::exahype2::ccz4::CCZ4.boundaryConditions(), examples::exahype2::mgccz4::FiniteVolumeMGCCZ4.boundaryConditions(), benchmarks::exahype2::ccz4::CCZ4.boundaryConditions(), examples::exahype2::mgccz4::ADERDGMGCCZ4.boundaryConditions(), applications::exahype2::ccz4.diagonal_gaugeWave(), examples::exahype2::mgccz4.forcedflat(), TP::Utilities.free_d3tensor(), applications::exahype2::ccz4.gaugeWave(), examples::exahype2::mgccz4.gaugeWave(), ContextCurvilinear< Shortcuts, basisSize, numberOfData, T >.initUnknownsPatch(), invokeFVSolverBoundaryConditions(), applications::exahype2::ccz4.linearWave(), examples::exahype2::mgccz4.linearWave(), applications::exahype2::ccz4::CCZ4.maxEigenvalue(), benchmarks::exahype2::ccz4::CCZ4.maxEigenvalue(), applications::exahype2::ccz4::CCZ4.nonconservativeProduct(), benchmarks::exahype2::ccz4::CCZ4.nonconservativeProduct(), examples::exahype2::mgccz4::FiniteVolumeMGCCZ4.nonconservativeProduct(), examples::exahype2::mgccz4::ADERDGMGCCZ4.nonconservativeProduct(), math::differentiation::numeric_3D::central_difference.partialT(), math::differentiation::numeric_3D::central_difference.partialX(), math::differentiation::numeric_3D::central_difference.partialY(), applications::exahype2::ccz4::CCZ4.refinementCriterion(), ContextDynamicRupture< Shortcuts, basisSize, numberOfVariables, numberOfParameters, T >.riemannSolver(), ContextDynamicRupture< Shortcuts, basisSize, numberOfVariables, numberOfParameters, T >.slipWeakeningFriction(), examples::exahype2::mgccz4::FiniteVolumeMGCCZ4.sourceTerm(), applications::exahype2::ccz4::CCZ4.sourceTerm(), benchmarks::exahype2::ccz4::CCZ4.sourceTerm(), ContextDynamicRupture< Shortcuts, basisSize, numberOfVariables, numberOfParameters, T >.tauStrength(), exahype2::CellFaceData< inType, outType >.toString(), exahype2::FaceData< inType, outType >.toString(), exahype2::CellFaceData< inType, outType >.~CellFaceData(), and exahype2::FaceData< inType, outType >.~FaceData().
acoustic.t0 = sympy.symbols("t0") |
Definition at line 153 of file acoustic.py.
acoustic.throw_away_data_after_build |
Definition at line 251 of file acoustic.py.
acoustic.time_in_between_plots |
Definition at line 214 of file acoustic.py.
float acoustic.time_in_between_two_snapshots = end_time / 10 |
Definition at line 45 of file acoustic.py.
acoustic.True |
Definition at line 251 of file acoustic.py.
acoustic.v = my_pde.name_Q_entries(1, dimensions, "v") |
Definition at line 86 of file acoustic.py.
Referenced by TP::TwoPunctures.bicgstab(), TP::TwoPunctures.calculate_derivs(), Numerics.computeFluctuationsLeft(), Numerics.computeFluctuationsRight(), TP::TwoPunctures.Derivatives_AB3(), TP::TwoPunctures.F_of_v(), TP::Utilities.free_dvector(), TP::Utilities.free_ivector(), riemannSolver.generate_fluctuations_left(), riemannSolver.generate_fluctuations_right(), Numerics.getVelocities(), TP::TwoPunctures.interpol(), TP::TwoPunctures.Interpolate(), TP::TwoPunctures.Newton(), TP::Utilities.norm1(), TP::Utilities.norm2(), TP::TwoPunctures.PunctEvalAtArbitPosition(), TP::TwoPunctures.PunctEvalAtArbitPositionFast(), TP::TwoPunctures.PunctIntPolAtArbitPosition(), TP::TwoPunctures.PunctTaylorExpandAtArbitPosition(), Numerics.riemannSolver(), ContextDynamicRupture< Shortcuts, basisSize, numberOfVariables, numberOfParameters, T >.riemannSolver(), riemannSolver.riemannSolver_BC0(), riemannSolver.riemannSolver_BCn(), Numerics.riemannSolverBC0(), Numerics.riemannSolverBCn(), TP::TwoPunctures.Run(), TP::Utilities.scalarproduct(), TP::TwoPunctures.set_initial_guess(), TP::TwoPunctures.SpecCoef(), and TP::TwoPunctures.TestRelax().