Author: tlinnet Date: Wed May 7 15:54:42 2014 New Revision: 23044 URL: http://svn.gna.org/viewcvs/relax?rev=23044&view=rev Log: Replaced "ex0c" with "v1s" to follow manual and paper. sr #3154: (https://gna.org/support/?3154) Implementation of Baldwin (2014) B14 model - 2-site exact solution model for all time scales. This follows the tutorial for adding relaxation dispersion models at: http://wiki.nmr-relax.com/Tutorial_for_adding_relaxation_dispersion_models_to_relax#Debugging Modified: trunk/lib/dispersion/b14.py Modified: trunk/lib/dispersion/b14.py URL: http://svn.gna.org/viewcvs/relax/trunk/lib/dispersion/b14.py?rev=23044&r1=23043&r2=23044&view=diff ============================================================================== --- trunk/lib/dispersion/b14.py (original) +++ trunk/lib/dispersion/b14.py Wed May 7 15:54:42 2014 @@ -211,7 +211,7 @@ v1c = F0 * cosh(E0) - f2 * cos(E2) # Complex. - ex0c = F0 * sinh(E0) - f2 * sin(E2)*1j + v1s = F0 * sinh(E0) - f2 * sin(E2)*1j # Complex. ex1c = sinh(E1) @@ -222,7 +222,7 @@ y = power( (v1c - v3) / (v1c + v3), ncyc) # Off diagonal common factor. sinh fuctions. - v2pPdN = (-deltaR2 + kex + dw*1j) * ex0c - 2. * (oGt2 + k_AB * t1pt2) * ex1c + v2pPdN = (-deltaR2 + kex + dw*1j) * v1s - 2. * (oGt2 + k_AB * t1pt2) * ex1c Tog = (1. + y) / 2. + (1. - y) / (2. * v3) * v2pPdN / N