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\parallelepiped.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 CParallelepipedModel |
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28 | |
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29 | def create_ParallelepipedModel(): |
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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 = ParallelepipedModel() |
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34 | # CParallelepipedModel.__init__(obj) is called by |
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35 | # the ParallelepipedModel constructor |
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36 | return obj |
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37 | |
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38 | class ParallelepipedModel(CParallelepipedModel, BaseComponent): |
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39 | """ |
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40 | Class that evaluates a ParallelepipedModel model. |
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41 | This file was auto-generated from src\sans\models\include\parallelepiped.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 | * short_a = 35.0 [A] |
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49 | * short_b = 75.0 [A] |
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50 | * long_c = 400.0 [A] |
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51 | * sldPipe = 6.3e-06 [1/A^(2)] |
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52 | * sldSolv = 1e-06 [1/A^(2)] |
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53 | * background = 0.0 [1/cm] |
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54 | * parallel_theta = 0.0 [deg] |
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55 | * parallel_phi = 0.0 [deg] |
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56 | * parallel_psi = 0.0 [deg] |
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57 | * M0_sld_pipe = 0.0 [1/A^(2)] |
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58 | * M_theta_pipe = 0.0 [deg] |
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59 | * M_phi_pipe = 0.0 [deg] |
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60 | * M0_sld_solv = 0.0 [1/A^(2)] |
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61 | * M_theta_solv = 0.0 [deg] |
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62 | * M_phi_solv = 0.0 [deg] |
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63 | * Up_frac_i = 0.5 [u/(u+d)] |
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64 | * Up_frac_f = 0.5 [u/(u+d)] |
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65 | * Up_theta = 0.0 [deg] |
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66 | |
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67 | """ |
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68 | |
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69 | def __init__(self, multfactor=1): |
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70 | """ Initialization """ |
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71 | self.__dict__ = {} |
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72 | |
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73 | # Initialize BaseComponent first, then sphere |
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74 | BaseComponent.__init__(self) |
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75 | #apply(CParallelepipedModel.__init__, (self,)) |
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76 | |
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77 | CParallelepipedModel.__init__(self) |
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78 | self.is_multifunc = False |
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79 | |
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80 | ## Name of the model |
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81 | self.name = "ParallelepipedModel" |
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82 | ## Model description |
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83 | self.description = """ |
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84 | Form factor for a rectangular solid with uniform scattering length density. |
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85 | |
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86 | scale:Scale factor |
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87 | short_a: length of short edge [A] |
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88 | short_b: length of another short edge [A] |
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89 | long_c: length of long edge of the parallelepiped [A] |
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90 | sldPipe: Pipe_sld |
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91 | sldSolv: solvent_sld |
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92 | background:Incoherent Background [1/cm] |
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93 | """ |
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94 | |
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95 | ## Parameter details [units, min, max] |
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96 | self.details = {} |
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97 | self.details['scale'] = ['', None, None] |
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98 | self.details['short_a'] = ['[A]', None, None] |
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99 | self.details['short_b'] = ['[A]', None, None] |
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100 | self.details['long_c'] = ['[A]', None, None] |
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101 | self.details['sldPipe'] = ['[1/A^(2)]', None, None] |
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102 | self.details['sldSolv'] = ['[1/A^(2)]', None, None] |
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103 | self.details['background'] = ['[1/cm]', None, None] |
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104 | self.details['parallel_theta'] = ['[deg]', None, None] |
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105 | self.details['parallel_phi'] = ['[deg]', None, None] |
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106 | self.details['parallel_psi'] = ['[deg]', None, None] |
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107 | self.details['M0_sld_pipe'] = ['[1/A^(2)]', None, None] |
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108 | self.details['M_theta_pipe'] = ['[deg]', None, None] |
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109 | self.details['M_phi_pipe'] = ['[deg]', None, None] |
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110 | self.details['M0_sld_solv'] = ['[1/A^(2)]', None, None] |
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111 | self.details['M_theta_solv'] = ['[deg]', None, None] |
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112 | self.details['M_phi_solv'] = ['[deg]', None, None] |
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113 | self.details['Up_frac_i'] = ['[u/(u+d)]', None, None] |
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114 | self.details['Up_frac_f'] = ['[u/(u+d)]', None, None] |
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115 | self.details['Up_theta'] = ['[deg]', None, None] |
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116 | |
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117 | ## fittable parameters |
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118 | self.fixed = ['short_a.width', |
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119 | 'short_b.width', |
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120 | 'long_c.width', |
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121 | 'parallel_phi.width', |
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122 | 'parallel_psi.width', |
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123 | 'parallel_theta.width'] |
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124 | |
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125 | ## non-fittable parameters |
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126 | self.non_fittable = [] |
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127 | |
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128 | ## parameters with orientation |
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129 | self.orientation_params = ['parallel_phi', |
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130 | 'parallel_psi', |
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131 | 'parallel_theta', |
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132 | 'parallel_phi.width', |
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133 | 'parallel_psi.width', |
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134 | 'parallel_theta.width', |
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135 | 'M0_sld_pipe', |
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136 | 'M_theta_pipe', |
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137 | 'M_phi_pipe', |
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138 | 'M0_sld_solv', |
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139 | 'M_theta_solv', |
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140 | 'M_phi_solv', |
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141 | 'Up_frac_i', |
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142 | 'Up_frac_f', |
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143 | 'Up_theta'] |
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144 | |
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145 | ## parameters with magnetism |
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146 | self.magnetic_params = ['M0_sld_pipe', 'M_theta_pipe', 'M_phi_pipe', 'M0_sld_solv', 'M_theta_solv', 'M_phi_solv', 'Up_frac_i', 'Up_frac_f', 'Up_theta'] |
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147 | |
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148 | self.category = None |
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149 | self.multiplicity_info = None |
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150 | |
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151 | def __setstate__(self, state): |
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152 | """ |
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153 | restore the state of a model from pickle |
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154 | """ |
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155 | self.__dict__, self.params, self.dispersion = state |
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156 | |
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157 | def __reduce_ex__(self, proto): |
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158 | """ |
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159 | Overwrite the __reduce_ex__ of PyTypeObject *type call in the init of |
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160 | c model. |
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161 | """ |
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162 | state = (self.__dict__, self.params, self.dispersion) |
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163 | return (create_ParallelepipedModel, tuple(), state, None, None) |
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164 | |
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165 | def clone(self): |
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166 | """ Return a identical copy of self """ |
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167 | return self._clone(ParallelepipedModel()) |
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168 | |
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169 | def run(self, x=0.0): |
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170 | """ |
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171 | Evaluate the model |
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172 | |
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173 | :param x: input q, or [q,phi] |
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174 | |
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175 | :return: scattering function P(q) |
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176 | |
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177 | """ |
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178 | return CParallelepipedModel.run(self, x) |
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179 | |
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180 | def runXY(self, x=0.0): |
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181 | """ |
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182 | Evaluate the model in cartesian coordinates |
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183 | |
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184 | :param x: input q, or [qx, qy] |
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185 | |
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186 | :return: scattering function P(q) |
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187 | |
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188 | """ |
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189 | return CParallelepipedModel.runXY(self, x) |
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190 | |
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191 | def evalDistribution(self, x): |
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192 | """ |
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193 | Evaluate the model in cartesian coordinates |
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194 | |
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195 | :param x: input q[], or [qx[], qy[]] |
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196 | |
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197 | :return: scattering function P(q[]) |
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198 | |
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199 | """ |
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200 | return CParallelepipedModel.evalDistribution(self, x) |
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201 | |
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202 | def calculate_ER(self): |
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203 | """ |
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204 | Calculate the effective radius for P(q)*S(q) |
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205 | |
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206 | :return: the value of the effective radius |
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207 | |
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208 | """ |
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209 | return CParallelepipedModel.calculate_ER(self) |
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210 | |
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211 | def calculate_VR(self): |
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212 | """ |
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213 | Calculate the volf ratio for P(q)*S(q) |
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214 | |
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215 | :return: the value of the volf ratio |
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216 | |
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217 | """ |
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218 | return CParallelepipedModel.calculate_VR(self) |
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219 | |
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220 | def set_dispersion(self, parameter, dispersion): |
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221 | """ |
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222 | Set the dispersion object for a model parameter |
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223 | |
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224 | :param parameter: name of the parameter [string] |
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225 | :param dispersion: dispersion object of type DispersionModel |
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226 | |
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227 | """ |
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228 | return CParallelepipedModel.set_dispersion(self, |
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229 | parameter, dispersion.cdisp) |
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230 | |
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231 | |
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232 | # End of file |
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233 | |
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