Changes in src/sas/models/media/model_functions.rst [7072ce6:cd06a5f] 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
@@ -19 +20 @@
 .. ZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZ
 
-
-.. note::  The contents of this document are awaiting proof reading. Feb2015
 
 
@@ -170 +169 @@
 - RaspBerryModel_
 - CoreShellModel_ (including magnetic 2D version)
-- MicelleSphCoreModel_
 - CoreMultiShellModel_ (including magnetic 2D version)
 - Core2ndMomentModel_
@@ -2446 +2444 @@
 
 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). The total thickness is 2(H+T).
+|drho|\ H = SLD(headgroup) - SLD(solvent), and |drho|\ T = SLD(tail) - SLD(solvent).
 
 The 2D scattering intensity is calculated in the same way as 1D, where the *q* vector is defined as
@@ -3374 +3372 @@
 
 
-.. _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
 -------------------------------