Stereographic projection: Difference between revisions
(New page: A stereographic projection is often used to visualize a self-rotatation function. As explained in the [http://www.ccp4.ac.uk/html/polarrfn.html polarrfn documentation] the self-rotatation...) |
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Note: in the above, "theta" denotes the angle that is called "omega" in the [http://www.ccp4.ac.uk/html/polarrfn.html polarrfn documentation] | Note: in the above, "theta" denotes the angle that is called "omega" in the [http://www.ccp4.ac.uk/html/polarrfn.html polarrfn documentation] | ||
Example: see http://www.ccp4.ac.uk/dist/ccp4i/help/modules/appendices/mr-bathtutorial/mrbath5.html |
Revision as of 11:48, 24 April 2008
A stereographic projection is often used to visualize a self-rotatation function.
As explained in the polarrfn documentation the self-rotatation function always has the symmetry (180-theta, 180+phi, kappa) regardless of the crystallographic symmetry (i.e. even if it's P1). This relates one hemisphere (theta = 0 to 90) to the other (theta = 180 to 90) so there's no point plotting both hemispheres.
The self-rotatation function is plotted as a stereographic projection: if you imagine a sphere sitting on a horizontal flat piece of paper with the north pole at the top and the south pole in contact with the paper, then draw lines from the N pole through all the points making up the southern hemisphere until they hit the paper, that gives you the stereographic projection with the S pole in the middle and the equator projected onto the circumference. You could then turn the sphere upside down and draw lines from the S pole (now at the top) through all the points making up the northern hemisphere which gives you the other half of the projection, but as I said for self-rotatation functions they are the same so there's no point.
Note: in the above, "theta" denotes the angle that is called "omega" in the polarrfn documentation
Example: see http://www.ccp4.ac.uk/dist/ccp4i/help/modules/appendices/mr-bathtutorial/mrbath5.html