Changes in src/sas/models/media/model_functions.rst [cd06a5f:7072ce6] in sasview

File:

• src/sas/models/media/model_functions.rst (modified) (5 diffs)

src/sas/models/media/model_functions.rst

@@ -10 +10 @@
 
 .. To do:
-.. Remove the 'This is xi' & 'This is zeta' lines before release!
 .. Add example parameters/plots for the CoreShellEllipsoidXTModel
 .. Add example parameters/plots for the RectangularPrism models
@@ -20 +19 @@
 .. ZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZ
 
+
+.. note::  The contents of this document are awaiting proof reading. Feb2015
 
 
@@ -169 +170 @@
 - RaspBerryModel_
 - CoreShellModel_ (including magnetic 2D version)
+- MicelleSphCoreModel_
 - CoreMultiShellModel_ (including magnetic 2D version)
 - Core2ndMomentModel_
@@ -2444 +2446 @@
 
 where |delta|\ T = tail length (or *t_length*), |delta|\ H = head thickness (or *h_thickness*),
-|drho|\ H = SLD(headgroup) - SLD(solvent), and |drho|\ T = SLD(tail) - SLD(solvent).
+|drho|\ H = SLD(headgroup) - SLD(solvent), and |drho|\ T = SLD(tail) - SLD(solvent). The total thickness is 2(H+T).
 
 The 2D scattering intensity is calculated in the same way as 1D, where the *q* vector is defined as
@@ -3372 +3374 @@
 
 
+.. _MicelleSphCoreModel:
+
+**2.1.42. MicelleSphCoreModel**
+
+This model provides the form factor, *P(q)*, for a micelle with a spherical core 
+and Gaussian polymer chains attached to the surface.
+
+*2.1.42.1. Definition*
+
+The 1D scattering intensity for this model is calculated according to the equations given by Pedersen
+(Pedersen, 2000).
+
+*2.1.42.2. Validation of the MicelleSphCoreModel*
+
+This model has not yet been validated. Feb2015
+
+REFERENCES
+
+J Pedersen, *J. Appl. Cryst.*, 33 (2000) 637-640
+
+
+
 2.2 Shape-independent Functions
 -------------------------------