コード例 #1
0
ファイル: trajectory_io.py プロジェクト: zwicker-group/py-pde
r"""
Writing and reading trajectory data
===================================

This example illustrates how to store intermediate data to a file for later
post-processing. The storage frequency is an argument to the tracker. 
"""

from tempfile import NamedTemporaryFile

import pde

# define grid, state and pde
grid = pde.UnitGrid([32])
state = pde.FieldCollection([
    pde.ScalarField.random_uniform(grid),
    pde.VectorField.random_uniform(grid)
])
eq = pde.PDE({"s": "-0.1 * s", "v": "-v"})

# get a temporary file to write data to
path = NamedTemporaryFile(suffix=".hdf5")

# run a simulation and write the results
writer = pde.FileStorage(path.name, write_mode="truncate")
eq.solve(state, t_range=32, dt=0.01, tracker=writer.tracker(1))

# read the simulation back in again
reader = pde.FileStorage(path.name, write_mode="read_only")
pde.plot_kymographs(reader)
コード例 #2
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"""
Using simulation trackers
=========================

This example illustrates how trackers can be used to analyze simulations.
"""

import pde

grid = pde.UnitGrid([32, 32])  # generate grid
state = pde.ScalarField.random_uniform(grid)  # generate initial condition

storage = pde.MemoryStorage()

trackers = [
    "progress",  # show progress bar during simulation
    "steady_state",  # abort when steady state is reached
    storage.tracker(interval=1),  # store data every simulation time unit
    pde.PlotTracker(show=True),  # show images during simulation
    # print some output every 5 real seconds:
    pde.PrintTracker(interval=pde.RealtimeInterrupts(duration=5)),
]

eq = pde.DiffusionPDE(0.1)  # define the PDE
eq.solve(state, 3, dt=0.1, tracker=trackers)

for field in storage:
    print(field.integral)
コード例 #3
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ファイル: PDElib.py プロジェクト: FishermenOnTuesdays/dyns
import pde

grid = pde.UnitGrid([64, 64])  # generate grid
state = pde.ScalarField.random_uniform(grid)  # generate initial condition

#eq = pde.DiffusionPDE(diffusivity=0.1)        # define the pde
eq = pde.PDE({'c': 'laplace(c**3 - c - laplace(c))'})
result = eq.solve(state, t_range=[0, 10])  # solve the pde
result.plot()  # plot the resulting field
コード例 #4
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def main():
    grid = pde.UnitGrid([64, 64])
    field = pde.ScalarField.random_uniform(grid, label="Density")

    eq = pde.CahnHilliardPDE()
    eq.solve(field, t_range=1e3, dt=1e-3, tracker=["progress", "interactive"])
コード例 #5
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 def __init__(self, gridscale_x, gridscale_y, init_state_expression, t):
     self.grid = pde.UnitGrid([gridscale_x, gridscale_y])
     self.scale = np.array([gridscale_x, gridscale_y])
     self.t = t
     self.init_state = pde.ScalarField.from_expression(
         self.grid, init_state_expression)