Definition

cylinders is given by (Kline, 20_). The form factor is normalized

The output of the 2D scattering intensity function for oriented core-shell by the particle volume. Note that in this model the shell envelops the entire core so that besides a "sleeve" around the core, the shell also provides two flat end caps of thickness = shell thickness. In other words the length of the total cyclinder is the length of the core cylinder plus twice the thickness of the shell. If no end caps are desired one should use the `core-shell-bicelle` and set the thickness of the end caps (in this case the "thick_face") to zero.

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

$$

where

$$ 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

$$ 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 total volume (i.e. including both the core and the outer 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 $L+2T$. $J_1$ is the first order Bessel function.

.. _core-shell-cylinder-geometry:

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 `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,

S R Kline, *J Appl. Cryst.*, 39 (2006) 895

L. Onsager, *Ann. New York Acad. Sci.*, 51 (1949) 627-659

1445-1452

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

Created By |
sasview |

Uploaded |
Sept. 8, 2016, 9:33 a.m. |

Category |
Cylinder |

Score |
1 |

Verified |
Verified by Lewis O'Driscoll on 08 Sep 2016 |

In Library |
This model is included in the SasView library by default |

Files |
core_shell_cylinder.py core_shell_cylinder.c |

No comments yet.

Please log in to add a comment.