Changeset 02d7952 in sasview for src/sas/models/media
- Timestamp:
- Mar 20, 2016 9:39:04 AM (9 years ago)
- Branches:
- master, ESS_GUI, ESS_GUI_Docs, ESS_GUI_batch_fitting, ESS_GUI_bumps_abstraction, ESS_GUI_iss1116, ESS_GUI_iss879, ESS_GUI_iss959, ESS_GUI_opencl, ESS_GUI_ordering, ESS_GUI_sync_sascalc, costrafo411, magnetic_scatt, release-4.1.1, release-4.1.2, release-4.2.2, release_4.0.1, ticket-1009, ticket-1094-headless, ticket-1242-2d-resolution, ticket-1243, ticket-1249, ticket885, unittest-saveload
- Children:
- 558d64e, 1e81bc8
- Parents:
- e565eaf
- File:
-
- 1 edited
Legend:
- Unmodified
- Added
- Removed
-
src/sas/models/media/olddocs/model_functions.rst
rad25dc2 r02d7952 3981 3981 3982 3982 This is based on the generalized Guinier law for such elongated objects (see the Glatter reference below). For 3D 3983 globular objects (such as spheres), *s* = 0 and one recovers the standard Guinier _ formula. For 2D symmetry (such as3983 globular objects (such as spheres), *s* = 0 and one recovers the standard GuinierLaw_ formula. For 2D symmetry (such as 3984 3984 for rods) *s* = 1, and for 1D symmetry (such as for lamellae or platelets) *s* = 2. A dimensionality parameter (3-*s*) 3985 3985 is thus defined, and is 3 for spherical objects, 2 for rods, and 1 for plates.
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