[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_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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