[400155b] | 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.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 CCoreShellModel |
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| 28 | |
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| 29 | def create_CoreShellModel(): |
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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 = CoreShellModel() |
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| 34 | # CCoreShellModel.__init__(obj) is called by |
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| 35 | # the CoreShellModel constructor |
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| 36 | return obj |
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| 37 | |
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| 38 | class CoreShellModel(CCoreShellModel, BaseComponent): |
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| 39 | """ |
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| 40 | Class that evaluates a CoreShellModel model. |
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| 41 | This file was auto-generated from src\sans\models\include\core_shell.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 = 60.0 [A] |
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| 48 | * scale = 1.0 |
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| 49 | * thickness = 10.0 [A] |
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| 50 | * core_sld = 1e-06 [1/A^(2)] |
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| 51 | * shell_sld = 2e-06 [1/A^(2)] |
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| 52 | * solvent_sld = 3e-06 [1/A^(2)] |
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| 53 | * background = 0.0 [1/cm] |
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| 54 | * M0_sld_shell = 0.0 [1/A^(2)] |
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| 55 | * M_theta_shell = 0.0 [deg] |
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| 56 | * M_phi_shell = 0.0 [deg] |
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| 57 | * M0_sld_core = 0.0 [1/A^(2)] |
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| 58 | * M_theta_core = 0.0 [deg] |
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| 59 | * M_phi_core = 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(CCoreShellModel.__init__, (self,)) |
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| 76 | |
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| 77 | CCoreShellModel.__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 = "CoreShellModel" |
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| 82 | ## Model description |
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| 83 | self.description = """ |
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| 84 | Form factor for a monodisperse spherical particle with particle |
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| 85 | with a core-shell structure: |
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| 86 | |
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| 87 | The form factor is normalized by the |
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| 88 | total particle volume. |
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| 89 | |
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| 90 | radius: core radius, thickness: shell thickness |
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| 91 | |
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| 92 | Ref: Guinier, A. and G. Fournet, |
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| 93 | John Wiley and Sons, New York, 1955. |
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| 94 | """ |
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| 95 | |
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| 96 | ## Parameter details [units, min, max] |
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| 97 | self.details = {} |
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| 98 | self.details['radius'] = ['[A]', None, None] |
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| 99 | self.details['scale'] = ['', None, None] |
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| 100 | self.details['thickness'] = ['[A]', None, None] |
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| 101 | self.details['core_sld'] = ['[1/A^(2)]', None, None] |
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| 102 | self.details['shell_sld'] = ['[1/A^(2)]', None, None] |
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| 103 | self.details['solvent_sld'] = ['[1/A^(2)]', None, None] |
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| 104 | self.details['background'] = ['[1/cm]', None, None] |
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| 105 | self.details['M0_sld_shell'] = ['[1/A^(2)]', None, None] |
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| 106 | self.details['M_theta_shell'] = ['[deg]', None, None] |
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| 107 | self.details['M_phi_shell'] = ['[deg]', None, None] |
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| 108 | self.details['M0_sld_core'] = ['[1/A^(2)]', None, None] |
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| 109 | self.details['M_theta_core'] = ['[deg]', None, None] |
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| 110 | self.details['M_phi_core'] = ['[deg]', None, None] |
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| 111 | self.details['M0_sld_solv'] = ['[1/A^(2)]', None, None] |
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| 112 | self.details['M_theta_solv'] = ['[deg]', None, None] |
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| 113 | self.details['M_phi_solv'] = ['[deg]', None, None] |
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| 114 | self.details['Up_frac_i'] = ['[u/(u+d)]', None, None] |
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| 115 | self.details['Up_frac_f'] = ['[u/(u+d)]', None, None] |
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| 116 | self.details['Up_theta'] = ['[deg]', None, None] |
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| 117 | |
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| 118 | ## fittable parameters |
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| 119 | self.fixed = ['thickness.width', |
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| 120 | 'radius.width'] |
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| 121 | |
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| 122 | ## non-fittable parameters |
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| 123 | self.non_fittable = [] |
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| 124 | |
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| 125 | ## parameters with orientation |
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| 126 | self.orientation_params = ['M0_sld_shell', |
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| 127 | 'M_theta_shell', |
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| 128 | 'M_phi_shell', |
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| 129 | 'M0_sld_core', |
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| 130 | 'M_theta_core', |
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| 131 | 'M_phi_core', |
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| 132 | 'M0_sld_solv', |
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| 133 | 'M_theta_solv', |
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| 134 | 'M_phi_solv', |
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| 135 | 'Up_frac_i', |
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| 136 | 'Up_frac_f', |
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| 137 | 'Up_theta'] |
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| 138 | |
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| 139 | ## parameters with magnetism |
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| 140 | self.magnetic_params = ['M0_sld_shell', 'M_theta_shell', 'M_phi_shell', 'M0_sld_core', 'M_theta_core', 'M_phi_core', 'M0_sld_solv', 'M_theta_solv', 'M_phi_solv', 'Up_frac_i', 'Up_frac_f', 'Up_theta'] |
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| 141 | |
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| 142 | self.category = None |
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| 143 | self.multiplicity_info = None |
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| 144 | |
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| 145 | def __setstate__(self, state): |
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| 146 | """ |
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| 147 | restore the state of a model from pickle |
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| 148 | """ |
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| 149 | self.__dict__, self.params, self.dispersion = state |
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| 150 | |
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| 151 | def __reduce_ex__(self, proto): |
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| 152 | """ |
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| 153 | Overwrite the __reduce_ex__ of PyTypeObject *type call in the init of |
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| 154 | c model. |
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| 155 | """ |
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| 156 | state = (self.__dict__, self.params, self.dispersion) |
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| 157 | return (create_CoreShellModel, tuple(), state, None, None) |
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| 158 | |
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| 159 | def clone(self): |
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| 160 | """ Return a identical copy of self """ |
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| 161 | return self._clone(CoreShellModel()) |
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| 162 | |
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| 163 | def run(self, x=0.0): |
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| 164 | """ |
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| 165 | Evaluate the model |
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| 166 | |
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| 167 | :param x: input q, or [q,phi] |
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| 168 | |
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| 169 | :return: scattering function P(q) |
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| 170 | |
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| 171 | """ |
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| 172 | return CCoreShellModel.run(self, x) |
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| 173 | |
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| 174 | def runXY(self, x=0.0): |
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| 175 | """ |
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| 176 | Evaluate the model in cartesian coordinates |
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| 177 | |
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| 178 | :param x: input q, or [qx, qy] |
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| 179 | |
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| 180 | :return: scattering function P(q) |
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| 181 | |
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| 182 | """ |
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| 183 | return CCoreShellModel.runXY(self, x) |
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| 184 | |
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| 185 | def evalDistribution(self, x): |
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| 186 | """ |
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| 187 | Evaluate the model in cartesian coordinates |
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| 188 | |
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| 189 | :param x: input q[], or [qx[], qy[]] |
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| 190 | |
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| 191 | :return: scattering function P(q[]) |
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| 192 | |
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| 193 | """ |
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| 194 | return CCoreShellModel.evalDistribution(self, x) |
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| 195 | |
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| 196 | def calculate_ER(self): |
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| 197 | """ |
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| 198 | Calculate the effective radius for P(q)*S(q) |
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| 199 | |
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| 200 | :return: the value of the effective radius |
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| 201 | |
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| 202 | """ |
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| 203 | return CCoreShellModel.calculate_ER(self) |
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| 204 | |
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| 205 | def calculate_VR(self): |
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| 206 | """ |
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| 207 | Calculate the volf ratio for P(q)*S(q) |
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| 208 | |
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| 209 | :return: the value of the volf ratio |
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| 210 | |
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| 211 | """ |
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| 212 | return CCoreShellModel.calculate_VR(self) |
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| 213 | |
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| 214 | def set_dispersion(self, parameter, dispersion): |
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| 215 | """ |
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| 216 | Set the dispersion object for a model parameter |
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| 217 | |
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| 218 | :param parameter: name of the parameter [string] |
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| 219 | :param dispersion: dispersion object of type DispersionModel |
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| 220 | |
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| 221 | """ |
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| 222 | return CCoreShellModel.set_dispersion(self, |
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| 223 | parameter, dispersion.cdisp) |
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| 224 | |
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| 225 | |
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| 226 | # End of file |
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| 227 | |
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