def test_imex_linear_diffusion():
# advection with linear diffusion
# (q_t + q_x = q_xx + s(x, t))
exact_solution = xt_functions.AdvectingSine(offset=2.0)
problem = convection_diffusion.ConvectionDiffusion.manufactured_solution(
exact_solution)
t_initial = 0.0
bc = boundary.Periodic()
error_dict = dict()
cfl_list = [0.9, 0.3, 0.1]
for num_basis_cpts in range(1, 4):
imex = imex_runge_kutta.get_time_stepper(num_basis_cpts)
cfl = cfl_list[num_basis_cpts - 1]
# take 10 timesteps at coarsest time interval
n = 20
t_final = cfl * (1.0 / n) / exact_solution.wavespeed
exact_solution_final = lambda x: exact_solution(x, t_final)
for basis_class in basis.BASIS_LIST:
basis_ = basis_class(num_basis_cpts)
error_list = []
for num_elems in [n, 2 * n]:
mesh_ = mesh.Mesh1DUniform(0.0, 1.0, num_elems)
delta_t = cfl * mesh_.delta_x / exact_solution.wavespeed
dg_solution = basis_.project(problem.initial_condition, mesh_)
# weak dg form with flux_function and source term
explicit_operator = problem.get_explicit_operator(bc)
# ldg discretization of diffusion_function
implicit_operator = problem.get_implicit_operator(
bc, bc, include_source=False)
# this is a constant matrix case
(matrix, vector) = problem.ldg_matrix(dg_solution,
t_initial,
bc,
bc,
include_source=False)
solve_operator = time_stepping.get_solve_function_constant_matrix(
matrix, vector)
final_solution = time_stepping.time_step_loop_imex(
dg_solution,
t_initial,
t_final,
delta_t,
imex,
explicit_operator,
implicit_operator,
solve_operator,
)
dg_error = math_utils.compute_dg_error(final_solution,
exact_solution_final)
error = dg_error.norm()
error_list.append(error)
# plot.plot_dg_1d(final_solution, function=exact_solution_final)
# plot.plot_dg_1d(dg_error)
error_dict[num_basis_cpts] = error_list
order = utils.convergence_order(error_list)
assert order >= num_basis_cpts
def single_run(
problem, basis_, mesh_, bc, t_final, delta_t, num_picard_iterations=None
):
if num_picard_iterations is None:
num_picard_iterations = basis_.num_basis_cpts
imex = imex_runge_kutta.get_time_stepper(basis_.num_basis_cpts)
dg_solution = basis_.project(problem.initial_condition, mesh_)
# weak dg form with flux_function and source term
explicit_operator = problem.get_explicit_operator(bc)
# ldg discretization of diffusion_function
implicit_operator = problem.get_implicit_operator(
bc, bc, bc, bc, include_source=False
)
matrix_function = lambda t, q: problem.ldg_matrix(
q, t, bc, bc, bc, bc, include_source=False
)
solve_operator = time_stepping.get_solve_function_picard(
matrix_function, num_picard_iterations, mesh_.num_elems * basis_.num_basis_cpts
)
error_dict = dict()
# def after_step_hook(dg_solution, time):
# error = math_utils.compute_error(
# dg_solution, lambda x: problem.exact_solution(x, time)
# )
# error_dict[round(time, 8)] = error
final_solution = time_stepping.time_step_loop_imex(
dg_solution,
0.0,
t_final,
delta_t,
imex,
explicit_operator,
implicit_operator,
solve_operator,
# after_step_hook
)
exact_solution_final = x_functions.FrozenT(problem.exact_solution, t_final)
error = math_utils.compute_error(final_solution, exact_solution_final)
return (final_solution, error, error_dict)
def test_imex_linearized_mms():
# advection with linearized diffusion
# (q_t + q_x = (f(x, t) q_xx + s(x, t))
exact_solution = flux_functions.AdvectingSine(amplitude=0.1, offset=0.15)
p_class = convection_hyper_diffusion.ConvectionHyperDiffusion
p_func = p_class.linearized_manufactured_solution
t_initial = 0.0
bc = boundary.Periodic()
for diffusion_function in [squared]:
problem = p_func(exact_solution, None, diffusion_function)
cfl_list = [0.9, 0.15, 0.1]
for num_basis_cpts in range(2, 4):
imex = imex_runge_kutta.get_time_stepper(num_basis_cpts)
cfl = cfl_list[num_basis_cpts - 1]
n = 20
t_final = cfl * (1.0 / n) / exact_solution.wavespeed
exact_solution_final = lambda x: exact_solution(x, t_final)
for basis_class in [basis.LegendreBasis1D]:
basis_ = basis_class(num_basis_cpts)
error_list = []
for num_elems in [n, 2 * n]:
mesh_ = mesh.Mesh1DUniform(0.0, 1.0, num_elems)
delta_t = cfl * mesh_.delta_x / exact_solution.wavespeed
dg_solution = basis_.project(problem.initial_condition,
mesh_)
# weak dg form with flux_function and source term
explicit_operator = problem.get_explicit_operator(bc)
# ldg discretization of diffusion_function
implicit_operator = problem.get_implicit_operator(
bc, bc, bc, bc, include_source=False)
# this is a constant matrix case
matrix_function = lambda t: problem.ldg_matrix(
dg_solution, t, bc, bc, bc, bc, include_source=False)
solve_operator = time_stepping.get_solve_function_matrix(
matrix_function)
final_solution = time_stepping.time_step_loop_imex(
dg_solution,
t_initial,
t_final,
delta_t,
imex,
explicit_operator,
implicit_operator,
solve_operator,
)
error = math_utils.compute_error(final_solution,
exact_solution_final)
error_list.append(error)
# plot.plot_dg_1d(final_solution, function=exact_solution_final)
order = utils.convergence_order(error_list)
with open("hyper_diffusion_linearized_mms_test.yml",
"a") as file:
dict_ = dict()
subdict = dict()
subdict["cfl"] = cfl
subdict["n"] = n
subdict["error0"] = float(error_list[0])
subdict["error1"] = float(error_list[1])
subdict["order"] = float(
np.log2(error_list[0] / error_list[1]))
dict_[num_basis_cpts] = subdict
yaml.dump(dict_, file, default_flow_style=False)
assert order >= num_basis_cpts
def test_imex_nonlinear_mms():
wavenumber = 1.0 / 20.0
x_left = 0.0
x_right = 40.0
exact_solution = flux_functions.AdvectingSine(
amplitude=0.1, wavenumber=wavenumber, offset=0.15
)
p_func = thin_film.ThinFilm.manufactured_solution
t_initial = 0.0
bc = boundary.Periodic()
problem = p_func(exact_solution)
cfl_list = [0.5, 0.1, 0.1]
n = 40
for num_basis_cpts in range(3, 4):
imex = imex_runge_kutta.get_time_stepper(num_basis_cpts)
cfl = cfl_list[num_basis_cpts - 1]
t_final = 10 * cfl * ((x_right - x_left) / n) / exact_solution.wavespeed
exact_solution_final = lambda x: exact_solution(x, t_final)
for basis_class in [basis.LegendreBasis1D]:
basis_ = basis_class(num_basis_cpts)
error_list = []
for num_elems in [n, 2 * n]:
mesh_ = mesh.Mesh1DUniform(x_left, x_right, num_elems)
delta_t = cfl * mesh_.delta_x / exact_solution.wavespeed
dg_solution = basis_.project(problem.initial_condition, mesh_)
# weak dg form with flux_function and source term
explicit_operator = problem.get_explicit_operator(bc)
# ldg discretization of diffusion_function
implicit_operator = problem.get_implicit_operator(
bc, bc, bc, bc, include_source=False
)
matrix_function = lambda t, q: problem.ldg_matrix(
q, t, bc, bc, bc, bc, include_source=False
)
solve_operator = time_stepping.get_solve_function_picard(
matrix_function, num_basis_cpts, num_elems * num_basis_cpts
)
final_solution = time_stepping.time_step_loop_imex(
dg_solution,
t_initial,
t_final,
delta_t,
imex,
explicit_operator,
implicit_operator,
solve_operator,
)
error = math_utils.compute_error(final_solution, exact_solution_final)
error_list.append(error)
# plot.plot_dg_1d(final_solution, function=exact_solution_final)
with open("thin_film_nonlinear_mms_test.yml", "a") as file:
dict_ = dict()
subdict = dict()
subdict["cfl"] = cfl
subdict["n"] = n
subdict["error0"] = float(error_list[0])
subdict["error1"] = float(error_list[1])
subdict["order"] = float(np.log2(error_list[0] / error_list[1]))
dict_[num_basis_cpts] = subdict
yaml.dump(dict_, file, default_flow_style=False)
order = utils.convergence_order(error_list)
assert order >= num_basis_cpts
