Changes in / [737679d:3fd0499] in sasmodels
- Location:
- sasmodels/models
- Files:
-
- 2 added
- 5 edited
Legend:
- Unmodified
- Added
- Removed
-
sasmodels/models/bcc_paracrystal.py
r1f65db5 re2d6e3b 79 79 be accurate. 80 80 81 .. figure:: img/ parallelepiped_angle_definition.png81 .. figure:: img/bcc_angle_definition.png 82 82 83 Orientation of the crystal with respect to the scattering plane, when 84 $\theta = \phi = 0$ the $c$ axis is along the beam direction (the $z$ axis). 83 Orientation of the crystal with respect to the scattering plane. 85 84 86 85 References -
sasmodels/models/core_shell_parallelepiped.py
r1f65db5 r1916c52 6 6 The thickness and the scattering length density of the shell or 7 7 "rim" can be different on each (pair) of faces. However at this time 8 the 1D calculationdoes **NOT** actually calculate a c face rim despite the presence of9 the parameter. Some other aspects of the 1D calculation may be wrong.8 the model does **NOT** actually calculate a c face rim despite the presence of 9 the parameter. 10 10 11 11 .. note:: -
sasmodels/models/fcc_paracrystal.py
r1f65db5 re2d6e3b 76 76 2D model computation. 77 77 78 .. figure:: img/ parallelepiped_angle_definition.png78 .. figure:: img/bcc_angle_definition.png 79 79 80 Orientation of the crystal with respect to the scattering plane, when 81 $\theta = \phi = 0$ the $c$ axis is along the beam direction (the $z$ axis). 80 Orientation of the crystal with respect to the scattering plane. 82 81 83 82 References -
sasmodels/models/sc_paracrystal.py
r1f65db5 r3330bb4 83 83 model computation. 84 84 85 <<<<<<< HEAD86 .. figure:: img/parallelepiped_angle_definition.png87 88 Orientation of the crystal with respect to the scattering plane, when89 $\theta = \phi = 0$ the $c$ axis is along the beam direction (the $z$ axis).90 =======91 85 .. figure:: img/sc_crystal_angle_definition.jpg 92 >>>>>>> 3fd04991e2575b02401723d8534c376cd9b6630593 86 94 87 Reference -
sasmodels/models/triaxial_ellipsoid.py
r1f65db5 r3330bb4 113 113 * **Author:** NIST IGOR/DANSE **Date:** pre 2010 114 114 * **Last Modified by:** Paul Kienzle (improved calculation) **Date:** April 4, 2017 115 <<<<<<< HEAD116 * **Last Reviewed by:** Paul Kienzle &Richard Heenan **Date:** April 4, 2017117 =======118 115 * **Last Reviewed by:** Paul Kienzle & Richard Heenan **Date:** April 4, 2017 119 >>>>>>> 3fd04991e2575b02401723d8534c376cd9b66305120 116 121 117 """
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