Changeset c3ccaec in sasmodels for sasmodels/models/unified_power_Rg.py
- Timestamp:
- Feb 7, 2017 12:10:50 PM (7 years ago)
- Branches:
- master, core_shell_microgels, costrafo411, magnetic_model, ticket-1257-vesicle-product, ticket_1156, ticket_1265_superball, ticket_822_more_unit_tests
- Children:
- a90aa1c
- Parents:
- aa107ef (diff), fe8ff99 (diff)
Note: this is a merge changeset, the changes displayed below correspond to the merge itself.
Use the (diff) links above to see all the changes relative to each parent. - git-author:
- Paul Kienzle <pkienzle@…> (02/07/17 12:10:50)
- git-committer:
- GitHub <noreply@…> (02/07/17 12:10:50)
- File:
-
- 1 edited
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sasmodels/models/unified_power_Rg.py
r0542fe1 rc3ccaec 3 3 ---------- 4 4 5 Th e Beaucage model employs the empirical multiple level unified6 Exponential/Power-law fit method developed by G. Beaucage. Four functions 7 are included so that 1, 2, 3, or 4 levels can be used. In addition a 0 level 8 has been added which simplycalculates5 This model employs the empirical multiple level unified Exponential/Power-law 6 fit method developed by Beaucage. Four functions are included so that 1, 2, 3, 7 or 4 levels can be used. In addition a 0 level has been added which simply 8 calculates 9 9 10 10 .. math:: … … 15 15 many different types of particles, including fractal clusters, random coils 16 16 (Debye equation), ellipsoidal particles, etc. 17 18 The model works best for mass fractal systems characterized by Porod exponents 19 between 5/3 and 3. It should not be used for surface fractal systems. Hammouda 20 (2010) has pointed out a deficiency in the way this model handles the 21 transitioning between the Guinier and Porod regimes and which can create 22 artefacts that appear as kinks in the fitted model function. 23 24 Also see the Guinier_Porod model. 17 25 18 26 The empirical fit function is: … … 30 38 .. math:: 31 39 32 q_i^* = \frac{q}{\operatorname{erf}^3(q R_{gi}/\sqrt{6}} 40 q_i^* = q \left[\operatorname{erf} 41 \left(\frac{q R_{gi}}{\sqrt{6}}\right) 42 \right]^{-3} 33 43 34 44 … … 56 66 57 67 G Beaucage, *J. Appl. Cryst.*, 29 (1996) 134-146 68 69 B Hammouda, *Analysis of the Beaucage model, J. Appl. Cryst.*, (2010), 43, 1474-1478 58 70 59 71 """
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