1 | #!/usr/bin/env python |
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2 | |
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3 | ############################################################################## |
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4 | # This software was developed by the University of Tennessee as part of the |
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5 | # Distributed Data Analysis of Neutron Scattering Experiments (DANSE) |
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6 | # project funded by the US National Science Foundation. |
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7 | # |
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8 | # If you use DANSE applications to do scientific research that leads to |
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9 | # publication, we ask that you acknowledge the use of the software with the |
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10 | # following sentence: |
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11 | # |
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12 | # "This work benefited from DANSE software developed under NSF award DMR-0520547." |
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13 | # |
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14 | # copyright 2008, University of Tennessee |
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15 | ############################################################################## |
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16 | |
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17 | |
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18 | """ |
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19 | Provide functionality for a C extension model |
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20 | |
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21 | :WARNING: THIS FILE WAS GENERATED BY WRAPPERGENERATOR.PY |
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22 | DO NOT MODIFY THIS FILE, MODIFY ..\c_extensions\fractal.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 | |
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27 | from sans.models.BaseComponent import BaseComponent |
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28 | from sans_extension.c_models import CFractalModel |
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29 | import copy |
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30 | |
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31 | class FractalModel(CFractalModel, BaseComponent): |
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32 | """ |
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33 | Class that evaluates a FractalModel model. |
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34 | This file was auto-generated from ..\c_extensions\fractal.h. |
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35 | Refer to that file and the structure it contains |
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36 | for details of the model. |
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37 | List of default parameters: |
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38 | scale = 0.05 |
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39 | radius = 5.0 [A] |
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40 | fractal_dim = 2.0 |
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41 | cor_length = 100.0 [A] |
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42 | sldBlock = 2e-006 [1/A^(2)] |
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43 | sldSolv = 6.35e-006 [1/A^(2)] |
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44 | background = 0.0 [1/cm] |
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45 | |
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46 | """ |
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47 | |
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48 | def __init__(self): |
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49 | """ Initialization """ |
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50 | |
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51 | # Initialize BaseComponent first, then sphere |
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52 | BaseComponent.__init__(self) |
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53 | CFractalModel.__init__(self) |
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54 | |
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55 | ## Name of the model |
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56 | self.name = "FractalModel" |
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57 | ## Model description |
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58 | self.description =""" The scattering intensity I(x) = P(|x|)*S(|x|) + background, where |
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59 | p(x)= scale * V * delta^(2)* F(x*radius)^(2) |
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60 | F(x) = 3*[sin(x)-x cos(x)]/x**3 |
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61 | where delta = sldBlock -sldSolv. |
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62 | scale = scale factor * Volume fraction |
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63 | radius = Block radius |
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64 | fractal_dim = Fractal dimension |
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65 | cor_length = Correlation Length |
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66 | sldBlock = SDL block |
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67 | sldSolv = SDL solvent |
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68 | background = background""" |
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69 | |
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70 | ## Parameter details [units, min, max] |
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71 | self.details = {} |
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72 | self.details['scale'] = ['', None, None] |
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73 | self.details['radius'] = ['[A]', None, None] |
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74 | self.details['fractal_dim'] = ['', None, None] |
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75 | self.details['cor_length'] = ['[A]', None, None] |
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76 | self.details['sldBlock'] = ['[1/A^(2)]', None, None] |
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77 | self.details['sldSolv'] = ['[1/A^(2)]', None, None] |
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78 | self.details['background'] = ['[1/cm]', None, None] |
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79 | |
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80 | ## fittable parameters |
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81 | self.fixed=[] |
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82 | |
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83 | ## parameters with orientation |
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84 | self.orientation_params =[] |
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85 | |
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86 | def clone(self): |
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87 | """ Return a identical copy of self """ |
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88 | return self._clone(FractalModel()) |
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89 | |
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90 | def __getstate__(self): |
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91 | """ |
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92 | return object state for pickling and copying |
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93 | """ |
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94 | model_state = {'params': self.params, 'dispersion': self.dispersion, 'log': self.log} |
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95 | |
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96 | return self.__dict__, model_state |
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97 | |
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98 | def __setstate__(self, state): |
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99 | """ |
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100 | create object from pickled state |
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101 | |
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102 | :param state: the state of the current model |
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103 | |
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104 | """ |
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105 | |
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106 | self.__dict__, model_state = state |
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107 | self.params = model_state['params'] |
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108 | self.dispersion = model_state['dispersion'] |
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109 | self.log = model_state['log'] |
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110 | |
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111 | |
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112 | def run(self, x=0.0): |
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113 | """ |
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114 | Evaluate the model |
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115 | |
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116 | :param x: input q, or [q,phi] |
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117 | |
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118 | :return: scattering function P(q) |
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119 | |
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120 | """ |
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121 | |
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122 | return CFractalModel.run(self, x) |
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123 | |
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124 | def runXY(self, x=0.0): |
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125 | """ |
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126 | Evaluate the model in cartesian coordinates |
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127 | |
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128 | :param x: input q, or [qx, qy] |
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129 | |
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130 | :return: scattering function P(q) |
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131 | |
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132 | """ |
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133 | |
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134 | return CFractalModel.runXY(self, x) |
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135 | |
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136 | def evalDistribution(self, x=[]): |
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137 | """ |
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138 | Evaluate the model in cartesian coordinates |
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139 | |
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140 | :param x: input q[], or [qx[], qy[]] |
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141 | |
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142 | :return: scattering function P(q[]) |
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143 | |
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144 | """ |
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145 | return CFractalModel.evalDistribution(self, x) |
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146 | |
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147 | def calculate_ER(self): |
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148 | """ |
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149 | Calculate the effective radius for P(q)*S(q) |
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150 | |
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151 | :return: the value of the effective radius |
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152 | |
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153 | """ |
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154 | return CFractalModel.calculate_ER(self) |
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155 | |
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156 | def set_dispersion(self, parameter, dispersion): |
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157 | """ |
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158 | Set the dispersion object for a model parameter |
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159 | |
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160 | :param parameter: name of the parameter [string] |
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161 | :param dispersion: dispersion object of type DispersionModel |
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162 | |
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163 | """ |
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164 | return CFractalModel.set_dispersion(self, parameter, dispersion.cdisp) |
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165 | |
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166 | |
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167 | # End of file |
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