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Peano
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Variables | |
int | patch_size = 16 |
int | depth = 5 |
float | end_time = 1.0 |
list | size = [2.0, 2.0] |
list | offset = [0.0, 0.0] |
float | time_in_between_two_snapshots = end_time / 10 |
string | compile_mode = "Release" |
my_project | |
my_solver | |
my_pde | |
h = my_pde.name_Q_entry(0, "h") | |
hu = my_pde.name_Q_entry(1, "hu") | |
hv = my_pde.name_Q_entry(2, "hv") | |
b = my_pde.name_auxiliary_variable(0, "b") | |
g = sympy.symbols("g") | |
u = hu / h | |
v = hv / h | |
delta_b = my_pde.grad(b) | |
volume_centre = sympy.sqrt((1.0 - my_pde.x[0]) ** 2 + (1.0 - my_pde.x[1]) ** 2) | |
initial_conditions | |
boundary_conditions | |
flux | |
max_eigenvalue | |
ncp | |
plot_description | |
dimensions | |
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 | |
swe.b = my_pde.name_auxiliary_variable(0, "b") |
Definition at line 82 of file swe.py.
Referenced by TP::Utilities.chebev(), TP::Utilities.fourft(), TP::TwoPunctures.interpol(), TP::TwoPunctures.LineRelax_al(), TP::TwoPunctures.LineRelax_be(), and TP::TwoPunctures.PunctTaylorExpandAtArbitPosition().
swe.h = my_pde.name_Q_entry(0, "h") |
Definition at line 79 of file swe.py.
Referenced by examples::regulargridupscaling::MyObserver.beginTraversal(), examples::regulargridupscaling::MyObserver.endTraversal(), invokeFVSolverBoundaryConditions(), main(), math::differentiation::numeric_3D::central_difference.partialT(), math::differentiation::numeric_3D::central_difference.partialX(), math::differentiation::numeric_3D::central_difference.partialY(), and runParallel().
swe.my_pde |
swe.my_project |
swe.my_solver |