1 | ############################################################################## |
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2 | # This software was developed by the University of Tennessee as part of the |
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3 | # Distributed Data Analysis of Neutron Scattering Experiments (DANSE) |
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4 | # project funded by the US National Science Foundation. |
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5 | # |
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6 | # If you use DANSE applications to do scientific research that leads to |
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7 | # publication, we ask that you acknowledge the use of the software with the |
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8 | # following sentence: |
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9 | # |
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10 | # This work benefited from DANSE software developed under NSF award DMR-0520547 |
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11 | # |
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12 | # Copyright 2008-2011, University of Tennessee |
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13 | ############################################################################## |
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14 | |
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15 | """ |
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16 | Provide functionality for a C extension model |
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17 | |
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18 | .. WARNING:: |
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19 | |
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20 | THIS FILE WAS GENERATED BY WRAPPERGENERATOR.PY |
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21 | DO NOT MODIFY THIS FILE, MODIFY |
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22 | src\sans\models\include\masssurfacefractal.h |
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23 | AND RE-RUN THE GENERATOR SCRIPT |
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24 | """ |
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25 | |
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26 | from sans.models.BaseComponent import BaseComponent |
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27 | from sans.models.sans_extension.c_models import CMassSurfaceFractal |
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28 | |
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29 | def create_MassSurfaceFractal(): |
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30 | """ |
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31 | Create a model instance |
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32 | """ |
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33 | obj = MassSurfaceFractal() |
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34 | # CMassSurfaceFractal.__init__(obj) is called by |
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35 | # the MassSurfaceFractal constructor |
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36 | return obj |
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37 | |
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38 | class MassSurfaceFractal(CMassSurfaceFractal, BaseComponent): |
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39 | """ |
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40 | Class that evaluates a MassSurfaceFractal model. |
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41 | This file was auto-generated from src\sans\models\include\masssurfacefractal.h. |
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42 | Refer to that file and the structure it contains |
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43 | for details of the model. |
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44 | |
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45 | List of default parameters: |
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46 | |
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47 | * scale = 1.0 |
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48 | * mass_dim = 1.8 |
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49 | * surface_dim = 2.3 |
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50 | * cluster_rg = 86.7 [A] |
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51 | * primary_rg = 4000.0 [A] |
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52 | * background = 0.0 |
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53 | |
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54 | """ |
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55 | |
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56 | def __init__(self, multfactor=1): |
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57 | """ Initialization """ |
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58 | self.__dict__ = {} |
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59 | |
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60 | # Initialize BaseComponent first, then sphere |
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61 | BaseComponent.__init__(self) |
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62 | #apply(CMassSurfaceFractal.__init__, (self,)) |
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63 | |
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64 | CMassSurfaceFractal.__init__(self) |
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65 | self.is_multifunc = False |
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66 | |
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67 | ## Name of the model |
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68 | self.name = "MassSurfaceFractal" |
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69 | ## Model description |
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70 | self.description = """ |
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71 | The scattering intensity I(x) = scale*P(x) + background, |
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72 | p(x)= {[1+(x^2*a)]^(Dm/2) * [1+(x^2*b)]^(6-Ds-Dm)/2}^(-1) |
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73 | a = Rg^2/(3*Dm/2) |
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74 | b = rg^2/(3*(6-Ds-Dm)/2) |
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75 | scale = scale factor * N*Volume^2*contrast^2 |
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76 | mass_dim = Dm (mass fractal dimension) |
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77 | surface_dim = Ds |
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78 | cluster_rg = Rg |
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79 | primary_rg = rg |
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80 | background = background |
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81 | Ref: Schmidt, J Appl Cryst, eq(19), (1991), 24, 414-435 |
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82 | : Hurd, Schaefer, Martin, Phys Rev A, eq(2),(1987),35, 2361-2364 |
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83 | Note that 0 < Ds< 6 and 0 < Dm < 6. |
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84 | """ |
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85 | |
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86 | ## Parameter details [units, min, max] |
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87 | self.details = {} |
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88 | self.details['scale'] = ['', None, None] |
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89 | self.details['mass_dim'] = ['', None, None] |
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90 | self.details['surface_dim'] = ['', None, None] |
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91 | self.details['cluster_rg'] = ['[A]', None, None] |
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92 | self.details['primary_rg'] = ['[A]', None, None] |
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93 | self.details['background'] = ['', None, None] |
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94 | |
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95 | ## fittable parameters |
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96 | self.fixed = [] |
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97 | |
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98 | ## non-fittable parameters |
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99 | self.non_fittable = [] |
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100 | |
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101 | ## parameters with orientation |
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102 | self.orientation_params = [] |
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103 | |
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104 | ## parameters with magnetism |
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105 | self.magnetic_params = [] |
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106 | |
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107 | self.category = None |
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108 | self.multiplicity_info = None |
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109 | |
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110 | def __setstate__(self, state): |
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111 | """ |
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112 | restore the state of a model from pickle |
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113 | """ |
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114 | self.__dict__, self.params, self.dispersion = state |
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115 | |
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116 | def __reduce_ex__(self, proto): |
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117 | """ |
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118 | Overwrite the __reduce_ex__ of PyTypeObject *type call in the init of |
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119 | c model. |
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120 | """ |
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121 | state = (self.__dict__, self.params, self.dispersion) |
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122 | return (create_MassSurfaceFractal, tuple(), state, None, None) |
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123 | |
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124 | def clone(self): |
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125 | """ Return a identical copy of self """ |
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126 | return self._clone(MassSurfaceFractal()) |
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127 | |
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128 | def run(self, x=0.0): |
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129 | """ |
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130 | Evaluate the model |
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131 | |
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132 | :param x: input q, or [q,phi] |
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133 | |
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134 | :return: scattering function P(q) |
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135 | |
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136 | """ |
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137 | return CMassSurfaceFractal.run(self, x) |
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138 | |
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139 | def runXY(self, x=0.0): |
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140 | """ |
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141 | Evaluate the model in cartesian coordinates |
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142 | |
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143 | :param x: input q, or [qx, qy] |
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144 | |
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145 | :return: scattering function P(q) |
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146 | |
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147 | """ |
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148 | return CMassSurfaceFractal.runXY(self, x) |
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149 | |
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150 | def evalDistribution(self, x): |
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151 | """ |
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152 | Evaluate the model in cartesian coordinates |
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153 | |
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154 | :param x: input q[], or [qx[], qy[]] |
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155 | |
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156 | :return: scattering function P(q[]) |
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157 | |
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158 | """ |
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159 | return CMassSurfaceFractal.evalDistribution(self, x) |
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160 | |
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161 | def calculate_ER(self): |
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162 | """ |
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163 | Calculate the effective radius for P(q)*S(q) |
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164 | |
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165 | :return: the value of the effective radius |
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166 | |
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167 | """ |
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168 | return CMassSurfaceFractal.calculate_ER(self) |
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169 | |
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170 | def calculate_VR(self): |
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171 | """ |
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172 | Calculate the volf ratio for P(q)*S(q) |
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173 | |
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174 | :return: the value of the volf ratio |
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175 | |
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176 | """ |
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177 | return CMassSurfaceFractal.calculate_VR(self) |
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178 | |
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179 | def set_dispersion(self, parameter, dispersion): |
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180 | """ |
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181 | Set the dispersion object for a model parameter |
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182 | |
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183 | :param parameter: name of the parameter [string] |
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184 | :param dispersion: dispersion object of type DispersionModel |
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185 | |
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186 | """ |
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187 | return CMassSurfaceFractal.set_dispersion(self, |
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188 | parameter, dispersion.cdisp) |
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189 | |
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190 | |
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191 | # End of file |
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192 | |
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