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\core_shell_bicelle.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 CCoreShellBicelleModel |
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28 | |
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29 | def create_CoreShellBicelleModel(): |
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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 = CoreShellBicelleModel() |
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34 | # CCoreShellBicelleModel.__init__(obj) is called by |
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35 | # the CoreShellBicelleModel constructor |
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36 | return obj |
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37 | |
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38 | class CoreShellBicelleModel(CCoreShellBicelleModel, BaseComponent): |
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39 | """ |
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40 | Class that evaluates a CoreShellBicelleModel model. |
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41 | This file was auto-generated from src\sans\models\include\core_shell_bicelle.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 | * radius = 20.0 [A] |
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48 | * scale = 1.0 |
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49 | * rim_thick = 10.0 [A] |
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50 | * face_thick = 10.0 [A] |
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51 | * length = 400.0 [A] |
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52 | * core_sld = 1e-06 [1/A^(2)] |
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53 | * face_sld = 4e-06 [1/A^(2)] |
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54 | * rim_sld = 4e-06 [1/A^(2)] |
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55 | * solvent_sld = 1e-06 [1/A^(2)] |
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56 | * background = 0.0 [1/cm] |
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57 | * axis_theta = 90.0 [deg] |
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58 | * axis_phi = 0.0 [deg] |
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59 | |
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60 | """ |
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61 | |
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62 | def __init__(self, multfactor=1): |
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63 | """ Initialization """ |
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64 | self.__dict__ = {} |
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65 | |
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66 | # Initialize BaseComponent first, then sphere |
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67 | BaseComponent.__init__(self) |
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68 | #apply(CCoreShellBicelleModel.__init__, (self,)) |
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69 | |
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70 | CCoreShellBicelleModel.__init__(self) |
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71 | self.is_multifunc = False |
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72 | |
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73 | ## Name of the model |
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74 | self.name = "CoreShellBicelleModel" |
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75 | ## Model description |
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76 | self.description = """ |
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77 | P(q,alpha)= scale/Vs*f(q)^(2) + bkg, where: f(q)= 2(core_sld |
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78 | - solvant_sld)* Vc*sin[qLcos(alpha/2)] |
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79 | /[qLcos(alpha/2)]*J1(qRsin(alpha)) |
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80 | /[qRsin(alpha)]+2(shell_sld-solvent_sld) |
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81 | *Vs*sin[q(L+T)cos(alpha/2)][[q(L+T) |
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82 | *cos(alpha/2)]*J1(q(R+T)sin(alpha)) |
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83 | /q(R+T)sin(alpha)] |
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84 | |
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85 | alpha:is the angle between the axis of |
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86 | the cylinder and the q-vector |
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87 | Vs: the volume of the outer shell |
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88 | Vc: the volume of the core |
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89 | L: the length of the core |
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90 | shell_sld: the scattering length density |
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91 | of the shell |
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92 | solvent_sld: the scattering length density |
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93 | of the solvent |
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94 | bkg: the background |
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95 | T: the thickness |
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96 | R+T: is the outer radius |
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97 | L+2T: The total length of the outershell |
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98 | J1: the first order Bessel function |
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99 | theta: axis_theta of the cylinder |
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100 | phi: the axis_phi of the cylinder... |
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101 | """ |
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102 | |
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103 | ## Parameter details [units, min, max] |
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104 | self.details = {} |
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105 | self.details['radius'] = ['[A]', None, None] |
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106 | self.details['scale'] = ['', None, None] |
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107 | self.details['rim_thick'] = ['[A]', None, None] |
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108 | self.details['face_thick'] = ['[A]', None, None] |
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109 | self.details['length'] = ['[A]', None, None] |
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110 | self.details['core_sld'] = ['[1/A^(2)]', None, None] |
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111 | self.details['face_sld'] = ['[1/A^(2)]', None, None] |
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112 | self.details['rim_sld'] = ['[1/A^(2)]', None, None] |
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113 | self.details['solvent_sld'] = ['[1/A^(2)]', None, None] |
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114 | self.details['background'] = ['[1/cm]', None, None] |
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115 | self.details['axis_theta'] = ['[deg]', None, None] |
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116 | self.details['axis_phi'] = ['[deg]', None, None] |
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117 | |
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118 | ## fittable parameters |
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119 | self.fixed = ['axis_phi.width', |
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120 | 'axis_theta.width', |
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121 | 'length.width', |
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122 | 'radius.width', |
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123 | 'rim_thick.width', |
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124 | 'face_thick.width'] |
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125 | |
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126 | ## non-fittable parameters |
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127 | self.non_fittable = [] |
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128 | |
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129 | ## parameters with orientation |
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130 | self.orientation_params = ['axis_phi', |
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131 | 'axis_theta', |
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132 | 'axis_phi.width', |
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133 | 'axis_theta.width'] |
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134 | |
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135 | ## parameters with magnetism |
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136 | self.magnetic_params = [] |
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137 | |
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138 | self.category = None |
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139 | self.multiplicity_info = None |
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140 | |
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141 | def __setstate__(self, state): |
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142 | """ |
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143 | restore the state of a model from pickle |
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144 | """ |
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145 | self.__dict__, self.params, self.dispersion = state |
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146 | |
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147 | def __reduce_ex__(self, proto): |
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148 | """ |
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149 | Overwrite the __reduce_ex__ of PyTypeObject *type call in the init of |
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150 | c model. |
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151 | """ |
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152 | state = (self.__dict__, self.params, self.dispersion) |
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153 | return (create_CoreShellBicelleModel, tuple(), state, None, None) |
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154 | |
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155 | def clone(self): |
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156 | """ Return a identical copy of self """ |
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157 | return self._clone(CoreShellBicelleModel()) |
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158 | |
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159 | def run(self, x=0.0): |
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160 | """ |
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161 | Evaluate the model |
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162 | |
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163 | :param x: input q, or [q,phi] |
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164 | |
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165 | :return: scattering function P(q) |
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166 | |
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167 | """ |
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168 | return CCoreShellBicelleModel.run(self, x) |
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169 | |
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170 | def runXY(self, x=0.0): |
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171 | """ |
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172 | Evaluate the model in cartesian coordinates |
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173 | |
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174 | :param x: input q, or [qx, qy] |
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175 | |
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176 | :return: scattering function P(q) |
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177 | |
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178 | """ |
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179 | return CCoreShellBicelleModel.runXY(self, x) |
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180 | |
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181 | def evalDistribution(self, x): |
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182 | """ |
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183 | Evaluate the model in cartesian coordinates |
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184 | |
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185 | :param x: input q[], or [qx[], qy[]] |
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186 | |
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187 | :return: scattering function P(q[]) |
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188 | |
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189 | """ |
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190 | return CCoreShellBicelleModel.evalDistribution(self, x) |
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191 | |
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192 | def calculate_ER(self): |
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193 | """ |
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194 | Calculate the effective radius for P(q)*S(q) |
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195 | |
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196 | :return: the value of the effective radius |
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197 | |
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198 | """ |
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199 | return CCoreShellBicelleModel.calculate_ER(self) |
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200 | |
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201 | def calculate_VR(self): |
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202 | """ |
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203 | Calculate the volf ratio for P(q)*S(q) |
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204 | |
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205 | :return: the value of the volf ratio |
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206 | |
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207 | """ |
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208 | return CCoreShellBicelleModel.calculate_VR(self) |
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209 | |
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210 | def set_dispersion(self, parameter, dispersion): |
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211 | """ |
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212 | Set the dispersion object for a model parameter |
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213 | |
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214 | :param parameter: name of the parameter [string] |
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215 | :param dispersion: dispersion object of type DispersionModel |
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216 | |
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217 | """ |
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218 | return CCoreShellBicelleModel.set_dispersion(self, |
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219 | parameter, dispersion.cdisp) |
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220 | |
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221 | |
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222 | # End of file |
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223 | |
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