source: sasmodels/sasmodels/models/sphere.py @ 71b751d

core_shell_microgelsmagnetic_modelticket-1257-vesicle-productticket_1156ticket_1265_superballticket_822_more_unit_tests
Last change on this file since 71b751d was 71b751d, checked in by Paul Kienzle <pkienzle@…>, 6 years ago

update remaining form factors to use Fq interface

  • Property mode set to 100644
File size: 3.1 KB
Line 
1r"""
2For information about polarised and magnetic scattering, see
3the :ref:`magnetism` documentation.
4
5Definition
6----------
7
8The 1D scattering intensity is calculated in the following way (Guinier, 1955)
9
10.. math::
11
12    I(q) = \frac{\text{scale}}{V} \cdot \left[
13        3V(\Delta\rho) \cdot \frac{\sin(qr) - qr\cos(qr))}{(qr)^3}
14        \right]^2 + \text{background}
15
16where *scale* is a volume fraction, $V$ is the volume of the scatterer,
17$r$ is the radius of the sphere and *background* is the background level.
18*sld* and *sld_solvent* are the scattering length densities (SLDs) of the
19scatterer and the solvent respectively, whose difference is $\Delta\rho$.
20
21Note that if your data is in absolute scale, the *scale* should represent
22the volume fraction (which is unitless) if you have a good fit. If not,
23it should represent the volume fraction times a factor (by which your data
24might need to be rescaled).
25
26The 2D scattering intensity is the same as above, regardless of the
27orientation of $\vec q$.
28
29Validation
30----------
31
32Validation of our code was done by comparing the output of the 1D model
33to the output of the software provided by the NIST (Kline, 2006).
34
35
36References
37----------
38
39A Guinier and G. Fournet, *Small-Angle Scattering of X-Rays*,
40John Wiley and Sons, New York, (1955)
41
42* **Last Reviewed by:** S King and P Parker **Date:** 2013/09/09 and 2014/01/06
43"""
44
45import numpy as np
46from numpy import inf
47
48name = "sphere"
49title = "Spheres with uniform scattering length density"
50description = """\
51P(q)=(scale/V)*[3V(sld-sld_solvent)*(sin(qr)-qr cos(qr))
52                /(qr)^3]^2 + background
53    r: radius of sphere
54    V: The volume of the scatter
55    sld: the SLD of the sphere
56    sld_solvent: the SLD of the solvent
57"""
58category = "shape:sphere"
59
60#             ["name", "units", default, [lower, upper], "type","description"],
61parameters = [["sld", "1e-6/Ang^2", 1, [-inf, inf], "sld",
62               "Layer scattering length density"],
63              ["sld_solvent", "1e-6/Ang^2", 6, [-inf, inf], "sld",
64               "Solvent scattering length density"],
65              ["radius", "Ang", 50, [0, inf], "volume",
66               "Sphere radius"],
67             ]
68
69source = ["lib/sas_3j1x_x.c"]
70have_Fq = True
71
72c_code = """
73static double form_volume(double radius)
74{
75    return M_4PI_3*cube(radius);
76}
77
78static void Fq(double q, double *f1, double *f2, double sld, double sld_solvent, double radius)
79{
80    const double bes = sas_3j1x_x(q*radius);
81    const double contrast = (sld - sld_solvent);
82    const double form = contrast * form_volume(radius) * bes;
83    *f1 = 1.0e-2*form;
84    *f2 = 1.0e-4*form*form;
85}
86"""
87
88def ER(radius):
89    """
90    Return equivalent radius (ER)
91    """
92    return radius
93
94# VR defaults to 1.0
95
96def random():
97    radius = 10**np.random.uniform(1.3, 4)
98    pars = dict(
99        radius=radius,
100    )
101    return pars
102
103tests = [
104    [{}, 0.2, 0.726362],
105    [{"scale": 1., "background": 0., "sld": 6., "sld_solvent": 1.,
106      "radius": 120., "radius_pd": 0.2, "radius_pd_n":45},
107     0.2, 0.228843],
108    [{"radius": 120., "radius_pd": 0.2, "radius_pd_n":45}, "ER", 120.],
109    [{"radius": 120., "radius_pd": 0.2, "radius_pd_n":45}, "VR", 1.],
110]
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