1 | #!/usr/bin/env python |
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2 | """ |
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3 | Application to explore the difference between sasview 3.x orientation |
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4 | dispersity and possible replacement algorithms. |
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5 | """ |
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6 | from __future__ import division, print_function |
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7 | |
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8 | import sys, os |
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9 | sys.path.insert(0, os.path.dirname(os.path.dirname(os.path.realpath(__file__)))) |
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10 | |
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11 | import mpl_toolkits.mplot3d # Adds projection='3d' option to subplot |
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12 | import matplotlib.pyplot as plt |
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13 | from matplotlib.widgets import Slider, CheckButtons |
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14 | from matplotlib import cm |
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15 | import numpy as np |
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16 | from numpy import pi, cos, sin, sqrt, exp, degrees, radians |
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17 | |
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18 | def draw_beam(ax, view=(0, 0)): |
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19 | """ |
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20 | Draw the beam going from source at (0, 0, 1) to detector at (0, 0, -1) |
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21 | """ |
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22 | #ax.plot([0,0],[0,0],[1,-1]) |
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23 | #ax.scatter([0]*100,[0]*100,np.linspace(1, -1, 100), alpha=0.8) |
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24 | |
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25 | steps = 25 |
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26 | u = np.linspace(0, 2 * np.pi, steps) |
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27 | v = np.linspace(-1, 1, steps) |
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28 | |
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29 | r = 0.02 |
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30 | x = r*np.outer(np.cos(u), np.ones_like(v)) |
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31 | y = r*np.outer(np.sin(u), np.ones_like(v)) |
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32 | z = 1.3*np.outer(np.ones_like(u), v) |
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33 | |
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34 | theta, phi = view |
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35 | shape = x.shape |
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36 | points = np.matrix([x.flatten(), y.flatten(), z.flatten()]) |
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37 | points = Rz(phi)*Ry(theta)*points |
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38 | x, y, z = [v.reshape(shape) for v in points] |
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39 | |
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40 | ax.plot_surface(x, y, z, rstride=4, cstride=4, color='y', alpha=0.5) |
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41 | |
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42 | def draw_jitter(ax, view, jitter, dist='gaussian', size=(0.1, 0.4, 1.0)): |
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43 | """ |
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44 | Represent jitter as a set of shapes at different orientations. |
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45 | """ |
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46 | # set max diagonal to 0.95 |
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47 | scale = 0.95/sqrt(sum(v**2 for v in size)) |
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48 | size = tuple(scale*v for v in size) |
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49 | draw_shape = draw_parallelepiped |
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50 | #draw_shape = draw_ellipsoid |
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51 | |
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52 | #np.random.seed(10) |
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53 | #cloud = np.random.randn(10,3) |
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54 | cloud = [ |
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55 | [-1, -1, -1], |
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56 | [-1, -1, 0], |
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57 | [-1, -1, 1], |
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58 | [-1, 0, -1], |
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59 | [-1, 0, 0], |
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60 | [-1, 0, 1], |
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61 | [-1, 1, -1], |
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62 | [-1, 1, 0], |
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63 | [-1, 1, 1], |
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64 | [ 0, -1, -1], |
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65 | [ 0, -1, 0], |
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66 | [ 0, -1, 1], |
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67 | [ 0, 0, -1], |
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68 | [ 0, 0, 0], |
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69 | [ 0, 0, 1], |
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70 | [ 0, 1, -1], |
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71 | [ 0, 1, 0], |
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72 | [ 0, 1, 1], |
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73 | [ 1, -1, -1], |
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74 | [ 1, -1, 0], |
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75 | [ 1, -1, 1], |
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76 | [ 1, 0, -1], |
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77 | [ 1, 0, 0], |
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78 | [ 1, 0, 1], |
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79 | [ 1, 1, -1], |
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80 | [ 1, 1, 0], |
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81 | [ 1, 1, 1], |
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82 | ] |
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83 | dtheta, dphi, dpsi = jitter |
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84 | if dtheta == 0: |
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85 | cloud = [v for v in cloud if v[0] == 0] |
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86 | if dphi == 0: |
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87 | cloud = [v for v in cloud if v[1] == 0] |
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88 | if dpsi == 0: |
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89 | cloud = [v for v in cloud if v[2] == 0] |
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90 | draw_shape(ax, size, view, [0, 0, 0], steps=100, alpha=0.8) |
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91 | scale = 1/sqrt(3) if dist == 'rectangle' else 1 |
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92 | for point in cloud: |
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93 | delta = [scale*dtheta*point[0], scale*dphi*point[1], scale*dpsi*point[2]] |
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94 | draw_shape(ax, size, view, delta, alpha=0.8) |
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95 | for v in 'xyz': |
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96 | a, b, c = size |
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97 | lim = np.sqrt(a**2+b**2+c**2) |
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98 | getattr(ax, 'set_'+v+'lim')([-lim, lim]) |
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99 | getattr(ax, v+'axis').label.set_text(v) |
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100 | |
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101 | def draw_ellipsoid(ax, size, view, jitter, steps=25, alpha=1): |
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102 | """Draw an ellipsoid.""" |
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103 | a,b,c = size |
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104 | u = np.linspace(0, 2 * np.pi, steps) |
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105 | v = np.linspace(0, np.pi, steps) |
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106 | x = a*np.outer(np.cos(u), np.sin(v)) |
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107 | y = b*np.outer(np.sin(u), np.sin(v)) |
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108 | z = c*np.outer(np.ones_like(u), np.cos(v)) |
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109 | x, y, z = transform_xyz(view, jitter, x, y, z) |
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110 | |
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111 | ax.plot_surface(x, y, z, rstride=4, cstride=4, color='w', alpha=alpha) |
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112 | |
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113 | draw_labels(ax, view, jitter, [ |
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114 | ('c+', [ 0, 0, c], [ 1, 0, 0]), |
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115 | ('c-', [ 0, 0,-c], [ 0, 0,-1]), |
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116 | ('a+', [ a, 0, 0], [ 0, 0, 1]), |
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117 | ('a-', [-a, 0, 0], [ 0, 0,-1]), |
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118 | ('b+', [ 0, b, 0], [-1, 0, 0]), |
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119 | ('b-', [ 0,-b, 0], [-1, 0, 0]), |
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120 | ]) |
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121 | |
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122 | def draw_parallelepiped(ax, size, view, jitter, steps=None, alpha=1): |
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123 | """Draw a parallelepiped.""" |
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124 | a,b,c = size |
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125 | x = a*np.array([ 1,-1, 1,-1, 1,-1, 1,-1]) |
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126 | y = b*np.array([ 1, 1,-1,-1, 1, 1,-1,-1]) |
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127 | z = c*np.array([ 1, 1, 1, 1,-1,-1,-1,-1]) |
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128 | tri = np.array([ |
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129 | # counter clockwise triangles |
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130 | # z: up/down, x: right/left, y: front/back |
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131 | [0,1,2], [3,2,1], # top face |
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132 | [6,5,4], [5,6,7], # bottom face |
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133 | [0,2,6], [6,4,0], # right face |
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134 | [1,5,7], [7,3,1], # left face |
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135 | [2,3,6], [7,6,3], # front face |
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136 | [4,1,0], [5,1,4], # back face |
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137 | ]) |
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138 | |
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139 | x, y, z = transform_xyz(view, jitter, x, y, z) |
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140 | ax.plot_trisurf(x, y, triangles=tri, Z=z, color='w', alpha=alpha) |
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141 | |
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142 | draw_labels(ax, view, jitter, [ |
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143 | ('c+', [ 0, 0, c], [ 1, 0, 0]), |
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144 | ('c-', [ 0, 0,-c], [ 0, 0,-1]), |
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145 | ('a+', [ a, 0, 0], [ 0, 0, 1]), |
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146 | ('a-', [-a, 0, 0], [ 0, 0,-1]), |
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147 | ('b+', [ 0, b, 0], [-1, 0, 0]), |
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148 | ('b-', [ 0,-b, 0], [-1, 0, 0]), |
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149 | ]) |
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150 | |
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151 | def draw_sphere(ax, radius=10., steps=100): |
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152 | """Draw a sphere""" |
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153 | u = np.linspace(0, 2 * np.pi, steps) |
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154 | v = np.linspace(0, np.pi, steps) |
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155 | |
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156 | x = radius * np.outer(np.cos(u), np.sin(v)) |
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157 | y = radius * np.outer(np.sin(u), np.sin(v)) |
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158 | z = radius * np.outer(np.ones(np.size(u)), np.cos(v)) |
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159 | ax.plot_surface(x, y, z, rstride=4, cstride=4, color='w') |
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160 | |
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161 | def draw_mesh(ax, view, jitter, radius=1.2, n=11, dist='gaussian'): |
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162 | """ |
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163 | Draw the dispersion mesh showing the theta-phi orientations at which |
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164 | the model will be evaluated. |
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165 | """ |
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166 | theta, phi, psi = view |
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167 | dtheta, dphi, dpsi = jitter |
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168 | |
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169 | if dist == 'gaussian': |
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170 | t = np.linspace(-3, 3, n) |
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171 | weights = exp(-0.5*t**2) |
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172 | elif dist == 'rectangle': |
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173 | # Note: uses sasmodels ridiculous definition of rectangle width |
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174 | t = np.linspace(-1, 1, n)*sqrt(3) |
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175 | weights = np.ones_like(t) |
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176 | else: |
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177 | raise ValueError("expected dist to be 'gaussian' or 'rectangle'") |
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178 | |
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179 | # mesh in theta, phi formed by rotating z |
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180 | z = np.matrix([[0], [0], [radius]]) |
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181 | points = np.hstack([Rx(phi_i)*Ry(theta_i)*z |
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182 | for theta_i in dtheta*t |
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183 | for phi_i in dphi*t]) |
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184 | # rotate relative to beam |
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185 | points = orient_relative_to_beam(view, points) |
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186 | |
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187 | w = np.outer(weights*cos(radians(dtheta*t)), weights) |
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188 | |
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189 | x, y, z = [np.array(v).flatten() for v in points] |
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190 | ax.scatter(x, y, z, c=w.flatten(), marker='o', vmin=0., vmax=1.) |
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191 | |
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192 | def draw_labels(ax, view, jitter, text): |
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193 | """ |
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194 | Draw text at a particular location. |
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195 | """ |
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196 | labels, locations, orientations = zip(*text) |
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197 | px, py, pz = zip(*locations) |
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198 | dx, dy, dz = zip(*orientations) |
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199 | |
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200 | px, py, pz = transform_xyz(view, jitter, px, py, pz) |
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201 | dx, dy, dz = transform_xyz(view, jitter, dx, dy, dz) |
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202 | |
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203 | # TODO: zdir for labels is broken, and labels aren't appearing. |
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204 | for label, p, zdir in zip(labels, zip(px, py, pz), zip(dx, dy, dz)): |
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205 | zdir = np.asarray(zdir).flatten() |
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206 | ax.text(p[0], p[1], p[2], label, zdir=zdir) |
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207 | |
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208 | # Definition of rotation matrices comes from wikipedia: |
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209 | # https://en.wikipedia.org/wiki/Rotation_matrix#Basic_rotations |
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210 | def Rx(angle): |
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211 | """Construct a matrix to rotate points about *x* by *angle* degrees.""" |
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212 | a = radians(angle) |
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213 | R = [[1, 0, 0], |
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214 | [0, +cos(a), -sin(a)], |
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215 | [0, +sin(a), +cos(a)]] |
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216 | return np.matrix(R) |
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217 | |
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218 | def Ry(angle): |
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219 | """Construct a matrix to rotate points about *y* by *angle* degrees.""" |
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220 | a = radians(angle) |
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221 | R = [[+cos(a), 0, +sin(a)], |
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222 | [0, 1, 0], |
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223 | [-sin(a), 0, +cos(a)]] |
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224 | return np.matrix(R) |
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225 | |
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226 | def Rz(angle): |
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227 | """Construct a matrix to rotate points about *z* by *angle* degrees.""" |
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228 | a = radians(angle) |
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229 | R = [[+cos(a), -sin(a), 0], |
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230 | [+sin(a), +cos(a), 0], |
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231 | [0, 0, 1]] |
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232 | return np.matrix(R) |
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233 | |
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234 | def transform_xyz(view, jitter, x, y, z): |
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235 | """ |
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236 | Send a set of (x,y,z) points through the jitter and view transforms. |
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237 | """ |
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238 | x, y, z = [np.asarray(v) for v in (x, y, z)] |
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239 | shape = x.shape |
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240 | points = np.matrix([x.flatten(),y.flatten(),z.flatten()]) |
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241 | points = apply_jitter(jitter, points) |
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242 | points = orient_relative_to_beam(view, points) |
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243 | x, y, z = [np.array(v).reshape(shape) for v in points] |
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244 | return x, y, z |
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245 | |
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246 | def apply_jitter(jitter, points): |
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247 | """ |
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248 | Apply the jitter transform to a set of points. |
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249 | |
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250 | Points are stored in a 3 x n numpy matrix, not a numpy array or tuple. |
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251 | """ |
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252 | dtheta, dphi, dpsi = jitter |
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253 | points = Rx(dphi)*Ry(dtheta)*Rz(dpsi)*points |
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254 | return points |
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255 | |
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256 | def orient_relative_to_beam(view, points): |
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257 | """ |
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258 | Apply the view transform to a set of points. |
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259 | |
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260 | Points are stored in a 3 x n numpy matrix, not a numpy array or tuple. |
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261 | """ |
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262 | theta, phi, psi = view |
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263 | points = Rz(phi)*Ry(theta)*Rz(psi)*points |
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264 | return points |
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265 | |
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266 | # translate between number of dimension of dispersity and the number of |
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267 | # points along each dimension. |
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268 | PD_N_TABLE = { |
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269 | (0, 0, 0): (0, 0, 0), # 0 |
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270 | (1, 0, 0): (100, 0, 0), # 100 |
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271 | (0, 1, 0): (0, 100, 0), |
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272 | (0, 0, 1): (0, 0, 100), |
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273 | (1, 1, 0): (30, 30, 0), # 900 |
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274 | (1, 0, 1): (30, 0, 30), |
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275 | (0, 1, 1): (0, 30, 30), |
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276 | (1, 1, 1): (15, 15, 15), # 3375 |
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277 | } |
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278 | |
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279 | def clipped_range(data, portion=1.0, mode='central'): |
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280 | """ |
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281 | Determine range from data. |
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282 | |
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283 | If *portion* is 1, use full range, otherwise use the center of the range |
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284 | or the top of the range, depending on whether *mode* is 'central' or 'top'. |
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285 | """ |
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286 | if portion == 1.0: |
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287 | return data.min(), data.max() |
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288 | elif mode == 'central': |
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289 | data = np.sort(data.flatten()) |
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290 | offset = int(portion*len(data)/2 + 0.5) |
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291 | return data[offset], data[-offset] |
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292 | elif mode == 'top': |
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293 | data = np.sort(data.flatten()) |
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294 | offset = int(portion*len(data) + 0.5) |
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295 | return data[offset], data[-1] |
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296 | |
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297 | def draw_scattering(calculator, ax, view, jitter, dist='gaussian'): |
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298 | """ |
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299 | Plot the scattering for the particular view. |
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300 | |
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301 | *calculator* is returned from :func:`build_model`. *ax* are the 3D axes |
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302 | on which the data will be plotted. *view* and *jitter* are the current |
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303 | orientation and orientation dispersity. *dist* is one of the sasmodels |
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304 | weight distributions. |
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305 | """ |
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306 | ## Sasmodels use sqrt(3)*width for the rectangle range; scale to the |
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307 | ## proper width for comparison. Commented out since now using the |
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308 | ## sasmodels definition of width for rectangle. |
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309 | #scale = 1/sqrt(3) if dist == 'rectangle' else 1 |
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310 | scale = 1 |
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311 | |
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312 | # add the orientation parameters to the model parameters |
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313 | theta, phi, psi = view |
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314 | theta_pd, phi_pd, psi_pd = [scale*v for v in jitter] |
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315 | theta_pd_n, phi_pd_n, psi_pd_n = PD_N_TABLE[(theta_pd>0, phi_pd>0, psi_pd>0)] |
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316 | ## increase pd_n for testing jitter integration rather than simple viz |
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317 | #theta_pd_n, phi_pd_n, psi_pd_n = [5*v for v in (theta_pd_n, phi_pd_n, psi_pd_n)] |
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318 | |
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319 | pars = dict( |
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320 | theta=theta, theta_pd=theta_pd, theta_pd_type=dist, theta_pd_n=theta_pd_n, |
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321 | phi=phi, phi_pd=phi_pd, phi_pd_type=dist, phi_pd_n=phi_pd_n, |
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322 | psi=psi, psi_pd=psi_pd, psi_pd_type=dist, psi_pd_n=psi_pd_n, |
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323 | ) |
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324 | pars.update(calculator.pars) |
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325 | |
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326 | # compute the pattern |
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327 | qx, qy = calculator._data.x_bins, calculator._data.y_bins |
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328 | Iqxy = calculator(**pars).reshape(len(qx), len(qy)) |
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329 | |
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330 | # scale it and draw it |
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331 | Iqxy = np.log(Iqxy) |
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332 | if calculator.limits: |
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333 | # use limits from orientation (0,0,0) |
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334 | vmin, vmax = calculator.limits |
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335 | else: |
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336 | vmin, vmax = clipped_range(Iqxy, portion=0.95, mode='top') |
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337 | #print("range",(vmin,vmax)) |
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338 | #qx, qy = np.meshgrid(qx, qy) |
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339 | if 0: |
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340 | level = np.asarray(255*(Iqxy - vmin)/(vmax - vmin), 'i') |
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341 | level[level<0] = 0 |
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342 | colors = plt.get_cmap()(level) |
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343 | ax.plot_surface(qx, qy, -1.1, rstride=1, cstride=1, facecolors=colors) |
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344 | elif 1: |
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345 | ax.contourf(qx/qx.max(), qy/qy.max(), Iqxy, zdir='z', offset=-1.1, |
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346 | levels=np.linspace(vmin, vmax, 24)) |
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347 | else: |
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348 | ax.pcolormesh(qx, qy, Iqxy) |
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349 | |
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350 | def build_model(model_name, n=150, qmax=0.5, **pars): |
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351 | """ |
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352 | Build a calculator for the given shape. |
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353 | |
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354 | *model_name* is any sasmodels model. *n* and *qmax* define an n x n mesh |
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355 | on which to evaluate the model. The remaining parameters are stored in |
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356 | the returned calculator as *calculator.pars*. They are used by |
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357 | :func:`draw_scattering` to set the non-orientation parameters in the |
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358 | calculation. |
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359 | |
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360 | Returns a *calculator* function which takes a dictionary or parameters and |
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361 | produces Iqxy. The Iqxy value needs to be reshaped to an n x n matrix |
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362 | for plotting. See the :class:`sasmodels.direct_model.DirectModel` class |
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363 | for details. |
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364 | """ |
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365 | from sasmodels.core import load_model_info, build_model |
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366 | from sasmodels.data import empty_data2D |
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367 | from sasmodels.direct_model import DirectModel |
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368 | |
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369 | model_info = load_model_info(model_name) |
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370 | model = build_model(model_info) #, dtype='double!') |
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371 | q = np.linspace(-qmax, qmax, n) |
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372 | data = empty_data2D(q, q) |
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373 | calculator = DirectModel(data, model) |
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374 | |
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375 | # stuff the values for non-orientation parameters into the calculator |
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376 | calculator.pars = pars.copy() |
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377 | calculator.pars.setdefault('backgound', 1e-3) |
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378 | |
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379 | # fix the data limits so that we can see if the pattern fades |
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380 | # under rotation or angular dispersion |
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381 | Iqxy = calculator(theta=0, phi=0, psi=0, **calculator.pars) |
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382 | Iqxy = np.log(Iqxy) |
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383 | vmin, vmax = clipped_range(Iqxy, 0.95, mode='top') |
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384 | calculator.limits = vmin, vmax+1 |
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385 | |
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386 | return calculator |
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387 | |
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388 | def select_calculator(model_name, n=150): |
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389 | """ |
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390 | Create a model calculator for the given shape. |
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391 | |
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392 | *model_name* is one of sphere, cylinder, ellipsoid, triaxial_ellipsoid, |
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393 | parallelepiped or bcc_paracrystal. *n* is the number of points to use |
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394 | in the q range. *qmax* is chosen based on model parameters for the |
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395 | given model to show something intersting. |
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396 | |
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397 | Returns *calculator* and tuple *size* (a,b,c) giving minor and major |
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398 | equitorial axes and polar axis respectively. See :func:`build_model` |
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399 | for details on the returned calculator. |
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400 | """ |
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401 | a, b, c = 10, 40, 100 |
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402 | if model_name == 'sphere': |
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403 | calculator = build_model('sphere', n=n, radius=c) |
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404 | a = b = c |
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405 | elif model_name == 'bcc_paracrystal': |
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406 | calculator = build_model('bcc_paracrystal', n=n, dnn=c, |
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407 | d_factor=0.06, radius=40) |
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408 | a = b = c |
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409 | elif model_name == 'cylinder': |
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410 | calculator = build_model('cylinder', n=n, qmax=0.3, radius=b, length=c) |
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411 | a = b |
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412 | elif model_name == 'ellipsoid': |
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413 | calculator = build_model('ellipsoid', n=n, qmax=1.0, |
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414 | radius_polar=c, radius_equatorial=b) |
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415 | a = b |
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416 | elif model_name == 'triaxial_ellipsoid': |
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417 | calculator = build_model('triaxial_ellipsoid', n=n, qmax=0.5, |
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418 | radius_equat_minor=a, |
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419 | radius_equat_major=b, |
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420 | radius_polar=c) |
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421 | elif model_name == 'parallelepiped': |
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422 | calculator = build_model('parallelepiped', n=n, a=a, b=b, c=c) |
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423 | else: |
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424 | raise ValueError("unknown model %s"%model_name) |
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425 | |
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426 | return calculator, (a, b, c) |
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427 | |
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428 | def main(model_name='parallelepiped'): |
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429 | """ |
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430 | Show an interactive orientation and jitter demo. |
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431 | |
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432 | *model_name* is one of the models available in :func:`select_model`. |
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433 | """ |
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434 | # set up calculator |
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435 | calculator, size = select_calculator(model_name, n=150) |
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436 | |
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437 | ## uncomment to set an independent the colour range for every view |
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438 | ## If left commented, the colour range is fixed for all views |
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439 | calculator.limits = None |
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440 | |
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441 | ## use gaussian distribution unless testing integration |
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442 | #dist = 'rectangle' |
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443 | dist = 'gaussian' |
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444 | |
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445 | ## initial view |
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446 | #theta, dtheta = 70., 10. |
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447 | #phi, dphi = -45., 3. |
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448 | #psi, dpsi = -45., 3. |
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449 | theta, phi, psi = 0, 0, 0 |
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450 | dtheta, dphi, dpsi = 0, 0, 0 |
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451 | |
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452 | ## create the plot window |
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453 | #plt.hold(True) |
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454 | plt.set_cmap('gist_earth') |
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455 | plt.clf() |
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456 | #gs = gridspec.GridSpec(2,1,height_ratios=[4,1]) |
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457 | #ax = plt.subplot(gs[0], projection='3d') |
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458 | ax = plt.axes([0.0, 0.2, 1.0, 0.8], projection='3d') |
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459 | ax.axis('square') |
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460 | |
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461 | axcolor = 'lightgoldenrodyellow' |
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462 | |
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463 | ## add control widgets to plot |
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464 | axtheta = plt.axes([0.1, 0.15, 0.45, 0.04], axisbg=axcolor) |
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465 | axphi = plt.axes([0.1, 0.1, 0.45, 0.04], axisbg=axcolor) |
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466 | axpsi = plt.axes([0.1, 0.05, 0.45, 0.04], axisbg=axcolor) |
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467 | stheta = Slider(axtheta, 'Theta', -90, 90, valinit=theta) |
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468 | sphi = Slider(axphi, 'Phi', -180, 180, valinit=phi) |
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469 | spsi = Slider(axpsi, 'Psi', -180, 180, valinit=psi) |
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470 | |
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471 | axdtheta = plt.axes([0.75, 0.15, 0.15, 0.04], axisbg=axcolor) |
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472 | axdphi = plt.axes([0.75, 0.1, 0.15, 0.04], axisbg=axcolor) |
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473 | axdpsi= plt.axes([0.75, 0.05, 0.15, 0.04], axisbg=axcolor) |
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474 | # Note: using ridiculous definition of rectangle distribution, whose width |
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475 | # in sasmodels is sqrt(3) times the given width. Divide by sqrt(3) to keep |
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476 | # the maximum width to 90. |
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477 | dlimit = 30 if dist == 'gaussian' else 90/sqrt(3) |
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478 | sdtheta = Slider(axdtheta, 'dTheta', 0, dlimit, valinit=dtheta) |
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479 | sdphi = Slider(axdphi, 'dPhi', 0, 2*dlimit, valinit=dphi) |
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480 | sdpsi = Slider(axdpsi, 'dPsi', 0, 2*dlimit, valinit=dpsi) |
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481 | |
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482 | ## callback to draw the new view |
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483 | def update(val, axis=None): |
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484 | view = stheta.val, sphi.val, spsi.val |
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485 | jitter = sdtheta.val, sdphi.val, sdpsi.val |
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486 | # set small jitter as 0 if multiple pd dims |
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487 | dims = sum(v > 0 for v in jitter) |
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488 | limit = [0, 0, 2, 5][dims] |
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489 | jitter = [0 if v < limit else v for v in jitter] |
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490 | ax.cla() |
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491 | draw_beam(ax, (0, 0)) |
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492 | draw_jitter(ax, view, jitter, dist=dist, size=size) |
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493 | #draw_jitter(ax, view, (0,0,0)) |
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494 | draw_mesh(ax, view, jitter, dist=dist) |
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495 | draw_scattering(calculator, ax, view, jitter, dist=dist) |
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496 | plt.gcf().canvas.draw() |
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497 | |
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498 | ## bind control widgets to view updater |
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499 | stheta.on_changed(lambda v: update(v,'theta')) |
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500 | sphi.on_changed(lambda v: update(v, 'phi')) |
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501 | spsi.on_changed(lambda v: update(v, 'psi')) |
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502 | sdtheta.on_changed(lambda v: update(v, 'dtheta')) |
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503 | sdphi.on_changed(lambda v: update(v, 'dphi')) |
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504 | sdpsi.on_changed(lambda v: update(v, 'dpsi')) |
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505 | |
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506 | ## initialize view |
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507 | update(None, 'phi') |
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508 | |
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509 | ## go interactive |
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510 | plt.show() |
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511 | |
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512 | if __name__ == "__main__": |
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513 | model_name = sys.argv[1] if len(sys.argv) > 1 else 'parallelepiped' |
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514 | main(model_name) |
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