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Advection diffusion with a potent sink term
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# %% | ||
# %load_ext autoreload | ||
# %autoreload 2 | ||
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# %% | ||
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""" | ||
Test of the Updec package on the Advection-Diffusion equation with RBFs: | ||
PDE here: https://en.wikipedia.org/wiki/Convection%E2%80%93diffusion_equation | ||
""" | ||
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import time | ||
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import jax | ||
import jax.numpy as jnp | ||
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# jax.config.update('jax_platform_name', 'cpu') | ||
jax.config.update("jax_enable_x64", True) | ||
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from updes import * | ||
# key = jax.random.PRNGKey(13) | ||
key = None | ||
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# from torch.utils.tensorboard import SummaryWriter | ||
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RUN_NAME = "TempFolder" | ||
DATAFOLDER = "./data/" + RUN_NAME +"/" | ||
# DATAFOLDER = "demos/Advection/data/"+RUN_NAME+"/" | ||
make_dir(DATAFOLDER) | ||
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RBF = partial(polyharmonic, a=1) | ||
# RBF = gaussian | ||
MAX_DEGREE = 0 | ||
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DT = 1e-4 | ||
NB_TIMESTEPS = 30 | ||
PLOT_EVERY = 10 | ||
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## Diffusive constant | ||
K = 0.0 | ||
VEL = jnp.array([500.0, 0.0]) | ||
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Nx = 35 | ||
Ny = 35 | ||
SUPPORT_SIZE = "max" | ||
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# facet_types={"South":"p1", "North":"p1", "West":"p2", "East":"p2"} | ||
facet_types={"South":"p1", "North":"p1", "West":"p2", "East":"p2"} | ||
cloud = SquareCloud(Nx=Nx, Ny=Ny, facet_types=facet_types, noise_key=key, support_size=SUPPORT_SIZE) | ||
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cloud.visualize_cloud(s=0.1, figsize=(7,3)); | ||
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# %% | ||
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def my_diff_operator(x, center=None, rbf=None, monomial=None, fields=None): | ||
val = nodal_value(x, center, rbf, monomial) | ||
grad = nodal_gradient(x, center, rbf, monomial) | ||
lap = nodal_laplacian(x, center, rbf, monomial) | ||
return (val/DT) + jnp.dot(VEL, grad) - K*lap + fields[0]*val | ||
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def my_rhs_operator(x, centers=None, rbf=None, fields=None): | ||
val = value(x, fields[:,0], centers, rbf) | ||
return (val/DT) | ||
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d_zero = lambda x: 0. | ||
boundary_conditions = {"South":d_zero, "West":d_zero, "North":d_zero, "East":d_zero} | ||
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## u0 is zero everywhere except at a point in the middle | ||
# u0 = jnp.zeros(cloud.N) | ||
# source_id = int(cloud.N*0.71) | ||
# source_neighbors = jnp.array(cloud.local_supports[source_id][:cloud.N//40]) | ||
# # source_id = 0 | ||
# # source_neighbors = jnp.array(cloud.local_supports[source_id][:1]) | ||
# u0 = u0.at[source_neighbors].set(0.95) | ||
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def gaussian(x, y, x0, y0, sigma): | ||
return jnp.exp(-((x-x0)**2 + (y-y0)**2) / (2*sigma**2)) | ||
xy = cloud.sorted_nodes | ||
u0 = gaussian(xy[:,0], xy[:,1], 0.35, 0.5, 1/20) | ||
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u_sink = 0e-5*gaussian(xy[:,0], xy[:,1], 0.85, 0.5, 1/100) | ||
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## Begin timestepping for 100 steps | ||
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# fig = plt.figure(figsize=(6,3)) | ||
# ax1= fig.add_subplot(1, 1, 1, projection='3d') | ||
# ax = fig.add_subplot(1, 1, 1) | ||
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u = u0.copy() | ||
ulist = [u] | ||
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start = time.time() | ||
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for i in range(1, NB_TIMESTEPS+1): | ||
ufield = pde_solver_jit(diff_operator=my_diff_operator, | ||
rhs_operator = my_rhs_operator, | ||
diff_args=[u_sink], | ||
rhs_args=[u], | ||
cloud = cloud, | ||
boundary_conditions = boundary_conditions, | ||
rbf=RBF, | ||
max_degree=MAX_DEGREE,) | ||
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u = ufield.vals | ||
ulist.append(u) | ||
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# if i<=3 or i%PLOT_EVERY==0: | ||
# print(f"Step {i}") | ||
# # plt.cla() | ||
# # cloud.visualize_field(u, cmap="jet", projection="3d", title=f"Step {i}") | ||
# ax, _ = cloud.visualize_field(u, cmap="jet", title=f"Step {i}", vmin=0, vmax=1, figsize=(6*10,3*10), colorbar=False, levels=200) | ||
# plt.show() | ||
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walltime = time.time() - start | ||
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minutes = walltime // 60 % 60 | ||
seconds = walltime % 60 | ||
print(f"Walltime: {minutes} minutes {seconds:.2f} seconds") | ||
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# %% | ||
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filename = DATAFOLDER + "adv_diff_sink.gif" | ||
cloud.animate_fields([ulist], cmaps="jet", filename=filename, figsize=(7,3), titles=["Advection-Diffusion with Sink"]); | ||
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# %% | ||
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