Changeset bf227cd in sasmodels for sasmodels/models/mono_gauss_coil.py


Ignore:
Timestamp:
Mar 16, 2016 3:40:01 PM (8 years ago)
Author:
smk78
Branches:
master, core_shell_microgels, costrafo411, magnetic_model, release_v0.94, release_v0.95, ticket-1257-vesicle-product, ticket_1156, ticket_1265_superball, ticket_822_more_unit_tests
Children:
a1c91c2
Parents:
cb97bff
Message:

Improved

File:
1 edited

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  • sasmodels/models/mono_gauss_coil.py

    rcb97bff rbf227cd  
    88This model strictly describes the scattering from *monodisperse* polymer chains in theta solvents or polymer melts, conditions under which the distances between segments follow a Gaussian distribution. Provided the number of segments is large (ie, high molecular weight polymers) the single-chain form factor P(Q) is that described by Debye (1947). 
    99 
    10 To describe the scattering from *polydisperse* polymer chains, see the poly_gauss_coil model. 
     10To describe the scattering from *polydisperse* polymer chains, see the To describe the scattering from *monodisperse* polymer chains, see the :ref:`poly_gauss_coil <poly-gauss-coil>` model. 
    1111 
    1212Definition 
    1313---------- 
    1414 
    15      *I(q)* = *scale* |cdot| *P(q)* + *background* 
     15     *I(q)* = *scale* |cdot| *I* \ :sub:`0` |cdot| *P(q)* + *background* 
    1616          
    1717where 
    1818 
    19      *scale* = |phi|\ :sub:`poly` |cdot| *V* |cdot| (|rho|\ :sub:`poly` - |rho|\ :sub:`solv`)\  :sup:`2` 
     19     *I*\ :sub:`0` = |phi|\ :sub:`poly` |cdot| *V* |cdot| (|rho|\ :sub:`poly` - |rho|\ :sub:`solv`)\  :sup:`2` 
    2020 
    2121     *P(q)* = 2 [exp(-Z) + Z - 1] / Z \ :sup:`2` 
     
    2828          
    2929Here, |phi|\ :sub:`poly` is the volume fraction of polymer, *V* is the volume of a polymer coil, *M* is the molecular weight of the polymer, *N*\ :sub:`A` is Avogadro's Number, |delta| is the bulk density of the polymer, |rho|\ :sub:`poly` is the sld of the polymer, |rho|\ :sub:`solv` is the sld of the solvent, and *R*\ :sub:`g` is the radius of gyration of the polymer coil. 
    30  
    31 .. figure:: img/mono_gauss_coil_1d.jpg 
    32  
    33     1D plot using the default values. 
    3430 
    3531The 2D scattering intensity is calculated in the same way as the 1D, but where the *q* vector is redefined as 
     
    5955 
    6056#             ["name", "units", default, [lower, upper], "type", "description"], 
    61 parameters =  [["radius_gyration", "Ang", 50.0, [0.0, inf], "", "Radius of gyration"]] 
     57parameters =  [["i_zero", "1/cm", 1.0, [-inf, inf], "", "Intensity at q=0"], 
     58               ["radius_gyration", "Ang", 50.0, [0.0, inf], "", "Radius of gyration"]] 
    6259 
    6360# NB: Scale and Background are implicit parameters on every model 
     
    6865       inten = 1.0 
    6966    else: 
    70        inten = 2.0 * (exp(-z) + z - 1.0 ) / (z * z) 
     67       inten = i_zero * 2.0 * (exp(-z) + z - 1.0 ) / (z * z) 
    7168    return inten 
    7269Iq.vectorized =  True  # Iq accepts an array of q values 
     
    7875 
    7976demo =  dict(scale = 1.0, 
     77            i_zero = 1.0, 
    8078            radius_gyration = 50.0, 
    8179            background = 0.0) 
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