| |
| |
| r""" |
| Two-dimensional variable-coefficient acoustics |
| ============================================== |
| |
| Solve the variable-coefficient acoustics equations in 2D: |
| |
| .. math:: |
| p_t + K(x,y) (u_x + v_y) & = 0 \\ |
| u_t + p_x / \rho(x,y) & = 0 \\ |
| v_t + p_y / \rho(x,y) & = 0. |
| |
| Here p is the pressure, (u,v) is the velocity, :math:`K(x,y)` is the bulk modulus, |
| and :math:`\rho(x,y)` is the density. |
| |
| This example shows how to solve a problem with variable coefficients. |
| The left and right halves of the domain consist of different materials. |
| """ |
|
|
| from functools import partial |
|
|
| import matplotlib.pyplot as plt |
| import numpy as np |
| from skimage.transform import resize |
|
|
|
|
| def create_maze(dim, seed): |
| |
| maze = np.ones((dim * 2 + 1, dim * 2 + 1)) |
|
|
| |
| x, y = (0, 0) |
| maze[2 * x + 1, 2 * y + 1] = 0 |
|
|
| |
| stack = [(x, y)] |
| while len(stack) > 0: |
| x, y = stack[-1] |
|
|
| |
| directions = [(0, 1), (1, 0), (0, -1), (-1, 0)] |
| directions = seed.permutation(directions) |
|
|
| for dx, dy in directions: |
| nx, ny = x + dx, y + dy |
| if ( |
| nx >= 0 |
| and ny >= 0 |
| and nx < dim |
| and ny < dim |
| and maze[2 * nx + 1, 2 * ny + 1] == 1 |
| ): |
| maze[2 * nx + 1, 2 * ny + 1] = 0 |
| maze[2 * x + 1 + dx, 2 * y + 1 + dy] = 0 |
| stack.append((nx, ny)) |
| break |
| else: |
| stack.pop() |
|
|
| |
| maze[1, 0] = 0 |
| maze[-2, -1] = 0 |
|
|
| return maze |
|
|
|
|
| def setup( |
| kernel_language="Fortran", |
| use_petsc=False, |
| outdir="./_output", |
| solver_type="classic", |
| time_integrator="SSP104", |
| lim_type=2, |
| disable_output=False, |
| num_cells=(256, 256), |
| seed=None, |
| T_max=4.0, |
| num_steps=201, |
| ): |
| """ |
| Example python script for solving the 2d acoustics equations. |
| """ |
| from clawpack import riemann |
|
|
| if seed is None: |
| seed = np.random.default_rng() |
| if use_petsc: |
| import clawpack.petclaw as pyclaw |
| else: |
| from clawpack import pyclaw |
|
|
| if solver_type == "classic": |
| solver = pyclaw.ClawSolver2D(riemann.vc_acoustics_2D) |
| solver.dimensional_split = False |
| solver.limiters = pyclaw.limiters.tvd.MC |
| elif solver_type == "sharpclaw": |
| solver = pyclaw.SharpClawSolver2D(riemann.vc_acoustics_2D) |
| solver.time_integrator = time_integrator |
| if time_integrator == "SSPLMMk2": |
| solver.lmm_steps = 3 |
| solver.cfl_max = 0.25 |
| solver.cfl_desired = 0.24 |
|
|
| solver.bc_lower[0] = pyclaw.BC.wall |
| solver.bc_upper[0] = pyclaw.BC.extrap |
| solver.bc_lower[1] = pyclaw.BC.wall |
| solver.bc_upper[1] = pyclaw.BC.extrap |
| solver.aux_bc_lower[0] = pyclaw.BC.wall |
| solver.aux_bc_upper[0] = pyclaw.BC.extrap |
| solver.aux_bc_lower[1] = pyclaw.BC.wall |
| solver.aux_bc_upper[1] = pyclaw.BC.extrap |
|
|
| x = pyclaw.Dimension(-1.0, 1.0, num_cells[0], name="x") |
| y = pyclaw.Dimension(-1.0, 1.0, num_cells[1], name="y") |
| domain = pyclaw.Domain([x, y]) |
|
|
| num_eqn = 3 |
| num_aux = 2 |
| state = pyclaw.State(domain, num_eqn, num_aux) |
|
|
| grid = state.grid |
| X, Y = grid.p_centers |
|
|
| def construct_maze_background(aux, seed, base_maze_low=3, base_maze_high=8): |
| maze_size = seed.integers(base_maze_low, base_maze_high + 1) |
| maze = create_maze(maze_size, seed) |
| maze = resize(maze, (aux[0].shape[-2], aux[0].shape[-1]), order=0) |
| rho = maze * 1e6 + 3 |
| return rho |
|
|
| rho = construct_maze_background(state.aux, seed) |
| c = np.sqrt(4.0 / rho) |
| state.aux[0, :, :] = rho |
| state.aux[1, :, :] = c |
|
|
| state.q[0, :, :] = 0.0 |
| state.q[1, :, :] = 0.0 |
| state.q[2, :, :] = 0.0 |
| |
| n_waves = seed.integers(1, 6) |
| mask = rho < 100 |
| for i in range(n_waves): |
| center_pixel = seed.choice(rho[mask].shape[0]) |
| x0 = X[mask][center_pixel] |
| y0 = Y[mask][center_pixel] |
| width = seed.uniform(0.01, 0.02) |
| rad = seed.uniform(0.01, 0.04) |
| intensity = seed.uniform(3.0, 5.0) |
| |
| r = np.sqrt((X - x0) ** 2 + (Y - y0) ** 2) |
| |
| state.q[0, :, :] += (np.abs(r - rad) <= width) * ( |
| intensity + np.cos(np.pi * (r - rad) / width) |
| ) |
|
|
| state.q[0][~mask] = 0.0 |
|
|
| claw = pyclaw.Controller() |
| claw.keep_copy = True |
| if disable_output: |
| claw.output_format = None |
| claw.solution = pyclaw.Solution(state, domain) |
| claw.solver = solver |
| claw.outdir = outdir |
| claw.tfinal = T_max |
| claw.num_output_times = num_steps |
| claw.write_aux_init = True |
| claw.setplot = setplot |
| claw.output_options = {"format": "binary"} |
| if use_petsc: |
| claw.output_options = {"format": "binary"} |
|
|
| return claw |
|
|
|
|
| def setplot(plotdata): |
| """ |
| Plot solution using VisClaw. |
| |
| This example shows how to mark an internal boundary on a 2D plot. |
| """ |
|
|
| from clawpack.visclaw import colormaps |
|
|
| plotdata.clearfigures() |
|
|
| |
| plotfigure = plotdata.new_plotfigure(name="Pressure", figno=0) |
|
|
| |
| plotaxes = plotfigure.new_plotaxes() |
| plotaxes.title = "Pressure" |
| plotaxes.scaled = True |
| plotaxes.afteraxes = mark_interface |
|
|
| |
| plotitem = plotaxes.new_plotitem(plot_type="2d_pcolor") |
| plotitem.plot_var = 0 |
| plotitem.pcolor_cmap = colormaps.yellow_red_blue |
| plotitem.add_colorbar = True |
| plotitem.pcolor_cmin = 0.0 |
| plotitem.pcolor_cmax = 1.0 |
|
|
| |
| plotfigure = plotdata.new_plotfigure(name="x-Velocity", figno=1) |
|
|
| |
| plotaxes = plotfigure.new_plotaxes() |
| plotaxes.title = "u" |
| plotaxes.afteraxes = mark_interface |
|
|
| plotitem = plotaxes.new_plotitem(plot_type="2d_pcolor") |
| plotitem.plot_var = 1 |
| plotitem.pcolor_cmap = colormaps.yellow_red_blue |
| plotitem.add_colorbar = True |
| plotitem.pcolor_cmin = -0.3 |
| plotitem.pcolor_cmax = 0.3 |
|
|
| return plotdata |
|
|
|
|
| def mark_interface(current_data): |
| plt.plot((0.0, 0.0), (-1.0, 1.0), "-k", linewidth=2) |
|
|
|
|
| if __name__ == "__main__": |
| from clawpack.pyclaw.util import run_app_from_main |
|
|
| setup_wrapped = partial(setup, seed=np.random.default_rng(1)) |
| output = run_app_from_main(setup_wrapped, setplot) |
|
|