source: sasmodels/sasmodels/models/core_shell_cylinder.py @ da1c8d1

r"""
Definition
----------

The output of the 2D scattering intensity function for oriented core-shell
cylinders is given by (Kline, 2006 [#kline]_). The form factor is normalized
by the particle volume.

.. math::

    I(q,\alpha) = \frac{\text{scale}}{V_s} F^2(q,\alpha).sin(\alpha) + \text{background}

where

.. math::

    F(q,\alpha) = &\ (\rho_c - \rho_s) V_c
           \frac{\sin \left( q \tfrac12 L\cos\alpha \right)}
                {q \tfrac12 L\cos\alpha}
           \frac{2 J_1 \left( qR\sin\alpha \right)}
                {qR\sin\alpha} \\
         &\ + (\rho_s - \rho_\text{solv}) V_s
           \frac{\sin \left( q \left(\tfrac12 L+T\right) \cos\alpha \right)}
                {q \left(\tfrac12 L +T \right) \cos\alpha}
           \frac{ 2 J_1 \left( q(R+T)\sin\alpha \right)}
                {q(R+T)\sin\alpha}

and

.. math::

    V_s = \pi (R + T)^2 (L + 2T)

and $\alpha$ is the angle between the axis of the cylinder and $\vec q$,
$V_s$ is the volume of the outer shell (i.e. the total volume, including
the shell), $V_c$ is the volume of the core, $L$ is the length of the core,
$R$ is the radius of the core, $T$ is the thickness of the shell, $\rho_c$
is the scattering length density of the core, $\rho_s$ is the scattering
length density of the shell, $\rho_\text{solv}$ is the scattering length
density of the solvent, and *background* is the background level.  The outer
radius of the shell is given by $R+T$ and the total length of the outer
shell is given by $L+2T$. $J1$ is the first order Bessel function.

.. _core-shell-cylinder-geometry:

.. figure:: img/core_shell_cylinder_geometry.jpg

    Core shell cylinder schematic.

To provide easy access to the orientation of the core-shell cylinder, we
define the axis of the cylinder using two angles $\theta$ and $\phi$.
(see :ref:`cylinder model <cylinder-angle-definition>`)

NB: The 2nd virial coefficient of the cylinder is calculated based on
the radius and 2 length values, and used as the effective radius for
$S(q)$ when $P(q) \cdot S(q)$ is applied.

The $\theta$ and $\phi$ parameters are not used for the 1D output.

Reference
---------

.. [#] see, for example, Ian Livsey  J. Chem. Soc., Faraday Trans. 2, 1987,83,
   1445-1452
.. [#kline] S R Kline, *J Appl. Cryst.*, 39 (2006) 895

Authorship and Verification
----------------------------

* **Author:** NIST IGOR/DANSE **Date:** pre 2010
* **Last Modified by:** Paul Kienzle **Date:** Aug 8, 2016
* **Last Reviewed by:** Richard Heenan **Date:** March 18, 2016
"""

import numpy as np
from numpy import pi, inf, sin, cos

name = "core_shell_cylinder"
title = "Right circular cylinder with a core-shell scattering length density profile."
description = """
P(q,alpha)= scale/Vs*f(q)^(2) + background,
      where: f(q)= 2(sld_core - solvant_sld)
        * Vc*sin[qLcos(alpha/2)]
        /[qLcos(alpha/2)]*J1(qRsin(alpha))
        /[qRsin(alpha)]+2(sld_shell-sld_solvent)
        *Vs*sin[q(L+T)cos(alpha/2)][[q(L+T)
        *cos(alpha/2)]*J1(q(R+T)sin(alpha))
        /q(R+T)sin(alpha)]

    alpha:is the angle between the axis of
        the cylinder and the q-vector
    Vs: the volume of the outer shell
    Vc: the volume of the core
    L: the length of the core
        sld_shell: the scattering length density of the shell
    sld_solvent: the scattering length density of the solvent
    background: the background
    T: the thickness
        R+T: is the outer radius
     L+2T: The total length of the outershell
    J1: the first order Bessel function
     theta: axis_theta of the cylinder
     phi: the axis_phi of the cylinder
"""
category = "shape:cylinder"

#             ["name", "units", default, [lower, upper], "type", "description"],
parameters = [["sld_core", "1e-6/Ang^2", 4, [-inf, inf], "sld",
               "Cylinder core scattering length density"],
              ["sld_shell", "1e-6/Ang^2", 4, [-inf, inf], "sld",
               "Cylinder shell scattering length density"],
              ["sld_solvent", "1e-6/Ang^2", 1, [-inf, inf], "sld",
               "Solvent scattering length density"],
              ["radius", "Ang", 20, [0, inf], "volume",
               "Cylinder core radius"],
              ["thickness", "Ang", 20, [0, inf], "volume",
               "Cylinder shell thickness"],
              ["length", "Ang", 400, [0, inf], "volume",
               "Cylinder length"],
              ["theta", "degrees", 60, [-360, 360], "orientation",
               "cylinder axis to beam angle"],
              ["phi", "degrees", 60, [-360, 360], "orientation",
               "rotation about beam"],
             ]

source = ["lib/polevl.c", "lib/sas_J1.c", "lib/gauss76.c", "core_shell_cylinder.c"]

def ER(radius, thickness, length):
    """
    Returns the effective radius used in the S*P calculation
    """
    print("radius")
    radius = radius + thickness
    length = length + 2 * thickness
    ddd = 0.75 * radius * (2 * radius * length + (length + radius) * (length + pi * radius))
    return 0.5 * (ddd) ** (1. / 3.)

def random():
    outer_radius = 10**np.random.uniform(1, 4.7)
    # Use a distribution with a preference for thin shell or thin core
    # Avoid core,shell radii < 1
    radius = np.random.beta(0.5, 0.5)*(outer_radius-2) + 1
    thickness = outer_radius - radius
    length = np.random.uniform(1, 4.7)
    pars = dict(
        radius=radius,
        thickness=thickness,
        length=length,
    )
    return pars

demo = dict(scale=1, background=0,
            sld_core=6, sld_shell=8, sld_solvent=1,
            radius=45, thickness=25, length=340,
            theta=30, phi=15,
            radius_pd=.2, radius_pd_n=1,
            length_pd=.2, length_pd_n=10,
            thickness_pd=.2, thickness_pd_n=10,
            theta_pd=15, theta_pd_n=45,
            phi_pd=15, phi_pd_n=1)
q = 0.1
# april 6 2017, rkh add unit tests, NOT compared with any other calc method, assume correct!
qx = q*cos(pi/6.0)
qy = q*sin(pi/6.0)
tests = [
    [{}, 0.075, 10.8552692237],
    [{}, (qx, qy), 0.444618752741],
]
del qx, qy  # not necessary to delete, but cleaner