Difference between revisions of "Interpmat.m"
(Normalise sequential blank lines) |
|||
| Line 27: | Line 27: | ||
==See also== | ==See also== | ||
[[ppcs.m]], [[lpcs.m]], [[kpcs.m]], [[ipcs.m]], [[ilpcs.m]], [[xyz2pms.m]], [[hfc2pcs.m]], [[hfc2pms.m]], [[g2chi.m]] | [[ppcs.m]], [[lpcs.m]], [[kpcs.m]], [[ipcs.m]], [[ilpcs.m]], [[xyz2pms.m]], [[hfc2pcs.m]], [[hfc2pms.m]], [[g2chi.m]] | ||
| − | |||
''Version 2.3, authors: [[Ilya Kuprov]]'' | ''Version 2.3, authors: [[Ilya Kuprov]]'' | ||
Revision as of 12:26, 25 April 2026
Returns a matrix that acts on a stretched pseudocontact shift density cube and projects out the values of the PCS at the Cartesian coordinates given. Tricubic interpolation is used.
Syntax
P=interpmat(cube_dims,ranges,xyz)
Arguments
cube_dims - pseudocontact shift cube grid sizes, a vector of
three integers ordered as [X Y Z]
ranges - cartesian axis extents for the pseudocontact shift
cube as [xmin xmax ymin ymax zmin zmax] in Angstroms.
xyz - nuclear coordinates as [x y z] with multiple rows) at
which PCS is to be evaluated, in Angstroms.
Outputs
P - matrix projecting out PCS values at the specified
nuclear positions from the stretched PCS cube.
Notes
This function is a part of the PCS inverse problem solver module; it should not normally be called directly by the user.
See also
ppcs.m, lpcs.m, kpcs.m, ipcs.m, ilpcs.m, xyz2pms.m, hfc2pcs.m, hfc2pms.m, g2chi.m
Version 2.3, authors: Ilya Kuprov