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March 14, 2016 08:32
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fdtd_3d_v1.py
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| #!coding:utf-8 | |
| """ | |
| fdtd_3d_v1.py | |
| OpenAcousticsのサンプルコード | |
| """ | |
| import os | |
| from time import sleep | |
| from scipy import * | |
| from mpl_toolkits.mplot3d import axes3d | |
| from matplotlib import cm | |
| import matplotlib.pyplot as plt | |
| # ************************************** # | |
| # * Paramater | |
| # ************************************** # | |
| X = 10 | |
| Y = 10 | |
| Z = 10 | |
| dx = 0.1 | |
| dy = 0.1 | |
| dz = 0.1 | |
| dt = 0.0001 | |
| Ro = 1.21 | |
| C = 343 | |
| K = Ro * C * C | |
| # ************************************** # | |
| # * Source | |
| # ************************************** # | |
| ang = arange(-pi, pi, 2 * pi / 50) | |
| sig = cos(ang) | |
| sig += 1 | |
| # 音響インピーダンス | |
| Z0 = Ro * C | |
| # ************************************** # | |
| # * Buffer | |
| # ************************************** # | |
| P1 = zeros((X, Y, Z), "float64") | |
| P2 = zeros((X, Y, Z), "float64") | |
| Ux1 = zeros((X + 1, Y, Z), "float64") | |
| Ux2 = zeros((X + 1, Y, Z), "float64") | |
| Uy1 = zeros((X, Y + 1, Z), "float64") | |
| Uy2 = zeros((X, Y + 1, Z), "float64") | |
| Uz1 = zeros((X, Y, Z + 1), "float64") | |
| Uz2 = zeros((X, Y, Z + 1), "float64") | |
| Rec = [] | |
| # ************************************** # | |
| # * Field Plot | |
| # ************************************** # | |
| plot_z = Z / 2 | |
| x = arange(0, dx * X, dx) | |
| y = arange(0, dy * Y, dy) | |
| xx, yy = meshgrid(y, x) | |
| fig = plt.figure() | |
| ax = axes3d.Axes3D(fig) | |
| surf = ax.plot_surface(xx, yy, P2[:, :, plot_z], rstride=1, cstride=1, cmap=cm.jet) | |
| oldsurf1 = surf | |
| surf = ax.plot_surface(xx, yy, P2[:, :, plot_z / 2] + 1, rstride=1, cstride=1, cmap=cm.jet) | |
| oldsurf2 = surf | |
| fig.show() | |
| # ************************************** # | |
| # * Iteration | |
| # ************************************** # | |
| for t in range(220): | |
| print t | |
| if t < len(sig): | |
| P1[X / 2, Y / 2, Z / 2] += sig[t] | |
| # ** 運動方程式 ** # | |
| # Inner Elements | |
| Ux2[1:X, :, :] = Ux1[1:X, :, :] - dt / Ro / dx * (P1[1:X, :, :] - P1[:X - 1, :, :]) | |
| Uy2[:, 1:Y, :] = Uy1[:, 1:Y, :] - dt / Ro / dy * (P1[:, 1:Y, :] - P1[:, :Y - 1, :]) | |
| Uz2[:, :, 1:Z] = Uz1[:, :, 1:Z] - dt / Ro / dz * (P1[:, :, 1:Z] - P1[:, :, :Z - 1]) | |
| # 振動解析により,構造振動ノードの変位から速度計算 | |
| # write code ... | |
| # BC | |
| Ux2[0, :, :] = P1[0, :, :] / -Z0 | |
| Ux2[-1, :, :] = P1[-1, :, :] / Z0 | |
| Uy2[:, 0, :] = P1[:, 0, :] / -Z0 | |
| Uy2[:, -1, :] = P1[:, -1, :] / Z0 | |
| Uz2[:, :, 0] = P1[:, :, 0] / -Z0 | |
| Uz2[:, :, -1] = P1[:, :, -1] / Z0 | |
| # ** 連続の式 ** # | |
| P2[:X, :Y, :Z] = P1[:X, :Y, :Z] \ | |
| - K * dt / dx * (Ux2[1:X + 1, :, :] - Ux2[:X, :, :]) \ | |
| - K * dt / dy * (Uy2[:, 1:Y + 1, :] - Uy2[:, :Y, :]) \ | |
| - K * dt / dz * (Uz2[:, :, 1:Z + 1] - Uz2[:, :, :Z]) | |
| # グラフプロット | |
| surf1 = ax.plot_surface(xx, yy, P2[:, :, plot_z], rstride=1, cstride=1, cmap=cm.jet) | |
| surf2 = ax.plot_surface(xx, yy, P2[:, :, plot_z / 2] + 1, rstride=1, cstride=1, cmap=cm.jet) | |
| ax.set_zlim3d(-1, 1) | |
| ax.collections.remove(oldsurf1) | |
| ax.collections.remove(oldsurf2) | |
| oldsurf1 = surf1 | |
| oldsurf2 = surf2 | |
| plt.pause(.01) | |
| # 変数の置き換え | |
| P1, P2 = P2, P1 | |
| Ux1, Ux2 = Ux2, Ux1 | |
| Uy1, Uy2 = Uy2, Uy1 | |
| Rec.append(P2[X / 4, Y / 4, Z / 4]) | |
| # output | |
| filename = "res_000.pp" | |
| basename = os.path.splitext(filename)[0] | |
| with open(basename + ".vtk", "w") as file: | |
| file.write("# vtk DataFile Version 2.0\n") | |
| file.write(basename + "\n") | |
| file.write("ASCII\n") | |
| file.write("DATASET UNSTRUCTURED_GRID\n") | |
| file.write("POINTS %d float\n" % len(x)) | |
| fig = plt.figure() | |
| plt.plot(Rec / max(Rec)) | |
| plt.plot(sig / max(sig)) | |
| plt.show() |
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