1 | r""" |
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2 | Definition |
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3 | ---------- |
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4 | |
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5 | Calculates the form factor for a rectangular solid with a core-shell structure. |
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6 | The thickness and the scattering length density of the shell or |
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7 | "rim" can be different on each (pair) of faces. |
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8 | |
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9 | The form factor is normalized by the particle volume $V$ such that |
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10 | |
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11 | .. math:: |
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12 | |
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13 | I(q) = \text{scale}\frac{\langle f^2 \rangle}{V} + \text{background} |
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14 | |
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15 | where $\langle \ldots \rangle$ is an average over all possible orientations |
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16 | of the rectangular solid. |
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17 | |
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18 | The function calculated is the form factor of the rectangular solid below. |
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19 | The core of the solid is defined by the dimensions $A$, $B$, $C$ such that |
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20 | $A < B < C$. |
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21 | |
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22 | .. image:: img/core_shell_parallelepiped_geometry.jpg |
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23 | |
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24 | There are rectangular "slabs" of thickness $t_A$ that add to the $A$ dimension |
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25 | (on the $BC$ faces). There are similar slabs on the $AC$ $(=t_B)$ and $AB$ |
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26 | $(=t_C)$ faces. The projection in the $AB$ plane is then |
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27 | |
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28 | .. image:: img/core_shell_parallelepiped_projection.jpg |
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29 | |
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30 | The volume of the solid is |
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31 | |
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32 | .. math:: |
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33 | |
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34 | V = ABC + 2t_ABC + 2t_BAC + 2t_CAB |
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35 | |
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36 | **meaning that there are "gaps" at the corners of the solid.** |
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37 | |
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38 | The intensity calculated follows the :ref:`parallelepiped` model, with the |
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39 | core-shell intensity being calculated as the square of the sum of the |
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40 | amplitudes of the core and the slabs on the edges. |
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41 | |
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42 | the scattering amplitude is computed for a particular orientation of the |
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43 | core-shell parallelepiped with respect to the scattering vector and then |
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44 | averaged over all possible orientations, where $\alpha$ is the angle between |
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45 | the $z$ axis and the $C$ axis of the parallelepiped, $\beta$ is |
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46 | the angle between projection of the particle in the $xy$ detector plane |
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47 | and the $y$ axis. |
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48 | |
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49 | .. math:: |
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50 | |
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51 | F(Q) |
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52 | &= (\rho_\text{core}-\rho_\text{solvent}) |
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53 | S(Q_A, A) S(Q_B, B) S(Q_C, C) \\ |
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54 | &+ (\rho_\text{A}-\rho_\text{solvent}) |
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55 | \left[S(Q_A, A+2t_A) - S(Q_A, Q)\right] S(Q_B, B) S(Q_C, C) \\ |
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56 | &+ (\rho_\text{B}-\rho_\text{solvent}) |
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57 | S(Q_A, A) \left[S(Q_B, B+2t_B) - S(Q_B, B)\right] S(Q_C, C) \\ |
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58 | &+ (\rho_\text{C}-\rho_\text{solvent}) |
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59 | S(Q_A, A) S(Q_B, B) \left[S(Q_C, C+2t_C) - S(Q_C, C)\right] |
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60 | |
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61 | with |
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62 | |
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63 | .. math:: |
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64 | |
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65 | S(Q, L) = L \frac{\sin \tfrac{1}{2} Q L}{\tfrac{1}{2} Q L} |
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66 | |
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67 | and |
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68 | |
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69 | .. math:: |
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70 | |
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71 | Q_A &= \sin\alpha \sin\beta \\ |
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72 | Q_B &= \sin\alpha \cos\beta \\ |
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73 | Q_C &= \cos\alpha |
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74 | |
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75 | |
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76 | where $\rho_\text{core}$, $\rho_\text{A}$, $\rho_\text{B}$ and $\rho_\text{C}$ |
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77 | are the scattering length of the parallelepiped core, and the rectangular |
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78 | slabs of thickness $t_A$, $t_B$ and $t_C$, respectively. $\rho_\text{solvent}$ |
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79 | is the scattering length of the solvent. |
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80 | |
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81 | FITTING NOTES |
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82 | ~~~~~~~~~~~~~ |
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83 | |
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84 | If the scale is set equal to the particle volume fraction, $\phi$, the returned |
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85 | value is the scattered intensity per unit volume, $I(q) = \phi P(q)$. However, |
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86 | **no interparticle interference effects are included in this calculation.** |
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87 | |
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88 | There are many parameters in this model. Hold as many fixed as possible with |
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89 | known values, or you will certainly end up at a solution that is unphysical. |
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90 | |
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91 | The returned value is in units of |cm^-1|, on absolute scale. |
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92 | |
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93 | NB: The 2nd virial coefficient of the core_shell_parallelepiped is calculated |
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94 | based on the the averaged effective radius $(=\sqrt{(A+2t_A)(B+2t_B)/\pi})$ |
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95 | and length $(C+2t_C)$ values, after appropriately sorting the three dimensions |
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96 | to give an oblate or prolate particle, to give an effective radius, |
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97 | for $S(Q)$ when $P(Q) * S(Q)$ is applied. |
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98 | |
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99 | For 2d data the orientation of the particle is required, described using |
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100 | angles $\theta$, $\phi$ and $\Psi$ as in the diagrams below, for further |
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101 | details of the calculation and angular dispersions see :ref:`orientation`. |
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102 | The angle $\Psi$ is the rotational angle around the *long_c* axis. For example, |
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103 | $\Psi = 0$ when the *short_b* axis is parallel to the *x*-axis of the detector. |
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104 | |
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105 | For 2d, constraints must be applied during fitting to ensure that the |
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106 | inequality $A < B < C$ is not violated, and hence the correct definition |
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107 | of angles is preserved. The calculation will not report an error, |
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108 | but the results may be not correct. |
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109 | |
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110 | .. figure:: img/parallelepiped_angle_definition.png |
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111 | |
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112 | Definition of the angles for oriented core-shell parallelepipeds. |
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113 | Note that rotation $\theta$, initially in the $xz$ plane, is carried |
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114 | out first, then rotation $\phi$ about the $z$ axis, finally rotation |
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115 | $\Psi$ is now around the axis of the cylinder. The neutron or X-ray |
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116 | beam is along the $z$ axis. |
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117 | |
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118 | .. figure:: img/parallelepiped_angle_projection.png |
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119 | |
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120 | Examples of the angles for oriented core-shell parallelepipeds against the |
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121 | detector plane. |
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122 | |
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123 | References |
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124 | ---------- |
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125 | |
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126 | .. [#] P Mittelbach and G Porod, *Acta Physica Austriaca*, 14 (1961) 185-211 |
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127 | Equations (1), (13-14). (in German) |
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128 | .. [#] D Singh (2009). *Small angle scattering studies of self assembly in |
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129 | lipid mixtures*, Johns Hopkins University Thesis (2009) 223-225. `Available |
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130 | from Proquest <http://search.proquest.com/docview/304915826?accountid |
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131 | =26379>`_ |
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132 | |
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133 | Authorship and Verification |
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134 | ---------------------------- |
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135 | |
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136 | * **Author:** NIST IGOR/DANSE **Date:** pre 2010 |
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137 | * **Converted to sasmodels by:** Miguel Gonzales **Date:** February 26, 2016 |
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138 | * **Last Modified by:** Paul Kienzle **Date:** October 17, 2017 |
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139 | * Cross-checked against hollow rectangular prism and rectangular prism for |
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140 | equal thickness overlapping sides, and by Monte Carlo sampling of points |
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141 | within the shape for non-uniform, non-overlapping sides. |
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142 | """ |
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143 | |
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144 | import numpy as np |
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145 | from numpy import pi, inf, sqrt, cos, sin |
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146 | |
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147 | name = "core_shell_parallelepiped" |
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148 | title = "Rectangular solid with a core-shell structure." |
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149 | description = """ |
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150 | P(q)= |
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151 | """ |
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152 | category = "shape:parallelepiped" |
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153 | |
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154 | # ["name", "units", default, [lower, upper], "type","description"], |
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155 | parameters = [["sld_core", "1e-6/Ang^2", 1, [-inf, inf], "sld", |
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156 | "Parallelepiped core scattering length density"], |
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157 | ["sld_a", "1e-6/Ang^2", 2, [-inf, inf], "sld", |
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158 | "Parallelepiped A rim scattering length density"], |
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159 | ["sld_b", "1e-6/Ang^2", 4, [-inf, inf], "sld", |
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160 | "Parallelepiped B rim scattering length density"], |
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161 | ["sld_c", "1e-6/Ang^2", 2, [-inf, inf], "sld", |
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162 | "Parallelepiped C rim scattering length density"], |
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163 | ["sld_solvent", "1e-6/Ang^2", 6, [-inf, inf], "sld", |
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164 | "Solvent scattering length density"], |
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165 | ["length_a", "Ang", 35, [0, inf], "volume", |
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166 | "Shorter side of the parallelepiped"], |
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167 | ["length_b", "Ang", 75, [0, inf], "volume", |
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168 | "Second side of the parallelepiped"], |
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169 | ["length_c", "Ang", 400, [0, inf], "volume", |
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170 | "Larger side of the parallelepiped"], |
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171 | ["thick_rim_a", "Ang", 10, [0, inf], "volume", |
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172 | "Thickness of A rim"], |
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173 | ["thick_rim_b", "Ang", 10, [0, inf], "volume", |
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174 | "Thickness of B rim"], |
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175 | ["thick_rim_c", "Ang", 10, [0, inf], "volume", |
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176 | "Thickness of C rim"], |
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177 | ["theta", "degrees", 0, [-360, 360], "orientation", |
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178 | "c axis to beam angle"], |
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179 | ["phi", "degrees", 0, [-360, 360], "orientation", |
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180 | "rotation about beam"], |
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181 | ["psi", "degrees", 0, [-360, 360], "orientation", |
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182 | "rotation about c axis"], |
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183 | ] |
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184 | |
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185 | source = ["lib/gauss76.c", "core_shell_parallelepiped.c"] |
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186 | |
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187 | |
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188 | def ER(length_a, length_b, length_c, thick_rim_a, thick_rim_b, thick_rim_c): |
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189 | """ |
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190 | Return equivalent radius (ER) |
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191 | """ |
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192 | from .parallelepiped import ER as ER_p |
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193 | |
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194 | a = length_a + 2*thick_rim_a |
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195 | b = length_b + 2*thick_rim_b |
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196 | c = length_c + 2*thick_rim_c |
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197 | return ER_p(a, b, c) |
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198 | |
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199 | # VR defaults to 1.0 |
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200 | |
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201 | def random(): |
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202 | outer = 10**np.random.uniform(1, 4.7, size=3) |
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203 | thick = np.random.beta(0.5, 0.5, size=3)*(outer-2) + 1 |
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204 | length = outer - thick |
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205 | pars = dict( |
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206 | length_a=length[0], |
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207 | length_b=length[1], |
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208 | length_c=length[2], |
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209 | thick_rim_a=thick[0], |
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210 | thick_rim_b=thick[1], |
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211 | thick_rim_c=thick[2], |
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212 | ) |
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213 | return pars |
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214 | |
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215 | # parameters for demo |
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216 | demo = dict(scale=1, background=0.0, |
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217 | sld_core=1, sld_a=2, sld_b=4, sld_c=2, sld_solvent=6, |
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218 | length_a=35, length_b=75, length_c=400, |
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219 | thick_rim_a=10, thick_rim_b=10, thick_rim_c=10, |
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220 | theta=0, phi=0, psi=0, |
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221 | length_a_pd=0.1, length_a_pd_n=1, |
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222 | length_b_pd=0.1, length_b_pd_n=1, |
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223 | length_c_pd=0.1, length_c_pd_n=1, |
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224 | thick_rim_a_pd=0.1, thick_rim_a_pd_n=1, |
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225 | thick_rim_b_pd=0.1, thick_rim_b_pd_n=1, |
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226 | thick_rim_c_pd=0.1, thick_rim_c_pd_n=1, |
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227 | theta_pd=10, theta_pd_n=1, |
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228 | phi_pd=10, phi_pd_n=1, |
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229 | psi_pd=10, psi_pd_n=1) |
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230 | |
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231 | # rkh 7/4/17 add random unit test for 2d, note make all params different, |
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232 | # 2d values not tested against other codes or models |
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233 | if 0: # pak: model rewrite; need to update tests |
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234 | qx, qy = 0.2 * cos(pi/6.), 0.2 * sin(pi/6.) |
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235 | tests = [[{}, 0.2, 0.533149288477], |
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236 | [{}, [0.2], [0.533149288477]], |
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237 | [{'theta':10.0, 'phi':20.0}, (qx, qy), 0.0853299803222], |
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238 | [{'theta':10.0, 'phi':20.0}, [(qx, qy)], [0.0853299803222]], |
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239 | ] |
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240 | del qx, qy # not necessary to delete, but cleaner |
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