lamellar_hg¶
Random lamellar phase with Head and Tail Groups
Parameter |
Description |
Units |
Default value |
---|---|---|---|
scale |
Scale factor or Volume fraction |
None |
1 |
background |
Source background |
cm-1 |
0.001 |
length_tail |
Tail thickness ( total = H+T+T+H) |
Å |
15 |
length_head |
Head thickness |
Å |
10 |
sld |
Tail scattering length density |
10-6Å-2 |
0.4 |
sld_head |
Head scattering length density |
10-6Å-2 |
3 |
sld_solvent |
Solvent scattering length density |
10-6Å-2 |
6 |
The returned value is scaled to units of cm-1 sr-1, absolute scale.
This model provides the scattering intensity, \(I(q)\), for a lyotropic lamellar phase where a random distribution in solution are assumed. The SLD of the head region is taken to be different from the SLD of the tail region.
Definition
The scattering intensity \(I(q)\) is
The form factor \(P(q)\) is
where \(\delta_T\) is length_tail, \(\delta_H\) is length_head, \(\Delta\rho_H\) is the head contrast (sld_head \(-\) sld_solvent), and \(\Delta\rho_T\) is tail contrast (sld \(-\) sld_solvent).
The total thickness of the lamellar sheet is a_H + delta_T + delta_T + delta_H$. Note that in a non aqueous solvent the chemical “head” group may be the “Tail region” and vice-versa.
The 2D scattering intensity is calculated in the same way as 1D, where the \(q\) vector is defined as
Source
References
F Nallet, R Laversanne, and D Roux, J. Phys. II France, 3, (1993) 487-502
J Berghausen, J Zipfel, P Lindner, W Richtering, J. Phys. Chem. B, 105, (2001) 11081-11088
Authorship and Verification
Author:
Last Modified by:
Last Reviewed by: S King and P Butler Date April 17, 2014