def my_rhs(t, state):
# check for some troublesome output types
inf_exists = not np.isfinite(discr.norm(state, np.inf))
if inf_exists:
if rank == 0:
logging.info(
"Non-finite values detected in simulation, exiting...")
# dump right now
sim_checkpoint(discr=discr,
visualizer=visualizer,
eos=eos,
q=state,
vizname=casename,
step=999999999,
t=t,
dt=current_dt,
nviz=1,
exittol=exittol,
constant_cfl=constant_cfl,
comm=comm,
vis_timer=vis_timer,
overwrite=True,
s0=s0_sc,
kappa=kappa_sc)
exit()
cv = split_conserved(dim=dim, q=state)
return (inviscid_operator(
discr, q=state, t=t, boundaries=boundaries, eos=eos) +
eos.get_species_source_terms(cv))
def test_lump_rhs(actx_factory, dim, order):
"""Tests the inviscid rhs using the non-trivial
1, 2, and 3D mass lump case against the analytic
expressions of the RHS. Checks several different
orders and refinement levels to check error behavior.
"""
actx = actx_factory()
tolerance = 1e-10
maxxerr = 0.0
from pytools.convergence import EOCRecorder
eoc_rec = EOCRecorder()
for nel_1d in [4, 8, 12]:
from meshmode.mesh.generation import (
generate_regular_rect_mesh, )
mesh = generate_regular_rect_mesh(
a=(-5, ) * dim,
b=(5, ) * dim,
n=(nel_1d, ) * dim,
)
logger.info(f"Number of elements: {mesh.nelements}")
discr = EagerDGDiscretization(actx, mesh, order=order)
nodes = thaw(actx, discr.nodes())
# Init soln with Lump and expected RHS = 0
center = np.zeros(shape=(dim, ))
velocity = np.zeros(shape=(dim, ))
lump = Lump(center=center, velocity=velocity)
lump_soln = lump(0, nodes)
boundaries = {BTAG_ALL: PrescribedBoundary(lump)}
inviscid_rhs = inviscid_operator(discr,
eos=IdealSingleGas(),
boundaries=boundaries,
q=lump_soln,
t=0.0)
expected_rhs = lump.exact_rhs(discr, lump_soln, 0)
err_max = discr.norm(inviscid_rhs - expected_rhs, np.inf)
if err_max > maxxerr:
maxxerr = err_max
eoc_rec.add_data_point(1.0 / nel_1d, err_max)
logger.info(f"Max error: {maxxerr}")
message = (f"Error for (dim,order) = ({dim},{order}):\n" f"{eoc_rec}")
logger.info(message)
assert (eoc_rec.order_estimate() >= order - 0.5
or eoc_rec.max_error() < tolerance)
def my_rhs(t, state):
#return inviscid_operator(discr, eos=eos, boundaries=boundaries, q=state, t=t)
return (inviscid_operator(
discr, q=state, t=t, boundaries=boundaries, eos=eos) +
artificial_viscosity(discr,
t=t,
r=state,
eos=eos,
boundaries=boundaries,
alpha=alpha_sc,
sigma=sigma_sc,
kappa=kappa_sc))
def test_vortex_rhs(actx_factory, order):
"""Tests the inviscid rhs using the non-trivial
2D isentropic vortex case configured to yield
rhs = 0. Checks several different orders
and refinement levels to check error
behavior.
"""
actx = actx_factory()
dim = 2
from pytools.convergence import EOCRecorder
eoc_rec = EOCRecorder()
from meshmode.mesh.generation import generate_regular_rect_mesh
for nel_1d in [16, 32, 64]:
mesh = generate_regular_rect_mesh(
a=(-5, ) * dim,
b=(5, ) * dim,
n=(nel_1d, ) * dim,
)
logger.info(f"Number of {dim}d elements: {mesh.nelements}")
discr = EagerDGDiscretization(actx, mesh, order=order)
nodes = thaw(actx, discr.nodes())
# Init soln with Vortex and expected RHS = 0
vortex = Vortex2D(center=[0, 0], velocity=[0, 0])
vortex_soln = vortex(0, nodes)
boundaries = {BTAG_ALL: PrescribedBoundary(vortex)}
inviscid_rhs = inviscid_operator(discr,
eos=IdealSingleGas(),
boundaries=boundaries,
q=vortex_soln,
t=0.0)
err_max = discr.norm(inviscid_rhs, np.inf)
eoc_rec.add_data_point(1.0 / nel_1d, err_max)
message = (f"Error for (dim,order) = ({dim},{order}):\n" f"{eoc_rec}")
logger.info(message)
assert (eoc_rec.order_estimate() >= order - 0.5
or eoc_rec.max_error() < 1e-11)
def my_rhs(t, state):
# check for some troublesome output types
inf_exists = not np.isfinite(discr.norm(state, np.inf))
if inf_exists:
if rank == 0:
logging.info("Non-finite values detected in simulation, exiting...")
# dump right now
viz_fields = [("sponge_sigma", gen_sponge())]
sim_checkpoint(discr=discr, visualizer=visualizer, eos=eos,
q=state, vizname=casename,
step=999999999, t=t, dt=current_dt,
nviz=1, exittol=exittol,
constant_cfl=constant_cfl, comm=comm, vis_timer=vis_timer,
overwrite=True,s0=s0_sc,kappa=kappa_sc,
viz_fields=viz_fields)
exit()
return ( inviscid_operator(discr, q=state, t=t,boundaries=boundaries, eos=eos)
+ artificial_viscosity(discr,t=t, r=state, eos=eos, boundaries=boundaries,
alpha=alpha_sc, s0=s0_sc, kappa=kappa_sc)
+ sponge(q=state, q_ref=ref_state, sigma=sponge_sigma))
def my_rhs(t, state):
return inviscid_operator(discr,
q=state,
t=t,
boundaries=boundaries,
eos=eos)
def rhs(t, q):
return inviscid_operator(discr,
eos=eos,
boundaries=boundaries,
q=q,
t=t)
def test_uniform_rhs(actx_factory, dim, order):
"""Tests the inviscid rhs using a trivial
constant/uniform state which should
yield rhs = 0 to FP. The test is performed
for 1, 2, and 3 dimensions.
"""
actx = actx_factory()
tolerance = 1e-9
maxxerr = 0.0
from pytools.convergence import EOCRecorder
eoc_rec0 = EOCRecorder()
eoc_rec1 = EOCRecorder()
# for nel_1d in [4, 8, 12]:
for nel_1d in [4, 8]:
from meshmode.mesh.generation import generate_regular_rect_mesh
mesh = generate_regular_rect_mesh(a=(-0.5, ) * dim,
b=(0.5, ) * dim,
n=(nel_1d, ) * dim)
logger.info(f"Number of {dim}d elements: {mesh.nelements}")
discr = EagerDGDiscretization(actx, mesh, order=order)
mass_input = discr.zeros(actx) + 1
energy_input = discr.zeros(actx) + 2.5
mom_input = make_obj_array(
[discr.zeros(actx) for i in range(discr.dim)])
fields = join_conserved(dim,
mass=mass_input,
energy=energy_input,
momentum=mom_input)
expected_rhs = make_obj_array(
[discr.zeros(actx) for i in range(len(fields))])
boundaries = {BTAG_ALL: DummyBoundary()}
inviscid_rhs = inviscid_operator(discr,
eos=IdealSingleGas(),
boundaries=boundaries,
q=fields,
t=0.0)
rhs_resid = inviscid_rhs - expected_rhs
resid_split = split_conserved(dim, rhs_resid)
rho_resid = resid_split.mass
rhoe_resid = resid_split.energy
mom_resid = resid_split.momentum
rhs_split = split_conserved(dim, inviscid_rhs)
rho_rhs = rhs_split.mass
rhoe_rhs = rhs_split.energy
rhov_rhs = rhs_split.momentum
message = (f"rho_rhs = {rho_rhs}\n"
f"rhoe_rhs = {rhoe_rhs}\n"
f"rhov_rhs = {rhov_rhs}")
logger.info(message)
assert discr.norm(rho_resid, np.inf) < tolerance
assert discr.norm(rhoe_resid, np.inf) < tolerance
for i in range(dim):
assert discr.norm(mom_resid[i], np.inf) < tolerance
err_max = discr.norm(rhs_resid[i], np.inf)
eoc_rec0.add_data_point(1.0 / nel_1d, err_max)
assert (err_max < tolerance)
if err_max > maxxerr:
maxxerr = err_max
# set a non-zero, but uniform velocity component
for i in range(len(mom_input)):
mom_input[i] = discr.zeros(actx) + (-1.0)**i
boundaries = {BTAG_ALL: DummyBoundary()}
inviscid_rhs = inviscid_operator(discr,
eos=IdealSingleGas(),
boundaries=boundaries,
q=fields,
t=0.0)
rhs_resid = inviscid_rhs - expected_rhs
resid_split = split_conserved(dim, rhs_resid)
rho_resid = resid_split.mass
rhoe_resid = resid_split.energy
mom_resid = resid_split.momentum
assert discr.norm(rho_resid, np.inf) < tolerance
assert discr.norm(rhoe_resid, np.inf) < tolerance
for i in range(dim):
assert discr.norm(mom_resid[i], np.inf) < tolerance
err_max = discr.norm(rhs_resid[i], np.inf)
eoc_rec1.add_data_point(1.0 / nel_1d, err_max)
assert (err_max < tolerance)
if err_max > maxxerr:
maxxerr = err_max
message = (f"V == 0 Errors:\n{eoc_rec0}" f"V != 0 Errors:\n{eoc_rec1}")
print(message)
assert (eoc_rec0.order_estimate() >= order - 0.5
or eoc_rec0.max_error() < 1e-9)
assert (eoc_rec1.order_estimate() >= order - 0.5
or eoc_rec1.max_error() < 1e-9)
