Author: bugman Date: Tue Jul 16 17:18:03 2013 New Revision: 20339 URL: http://svn.gna.org/viewcvs/relax?rev=20339&view=rev Log: Added support for the 'NS 2-site 3D' model to the relax_disp.select_model user function back end. This is the model of the numerical solution for the 2-site Bloch-McConnell equations. It originates as optimization function number 1 from the fitting_main_kex.py script from Mathilde Lescanne, Paul Schanda, and Dominique Marion (see http://thread.gmane.org/gmane.science.nmr.relax.devel/4138, https://gna.org/task/?7712#comment2 and https://gna.org/support/download.php?file_id=18262). This commit follows step 6 of the relaxation dispersion model addition tutorial (http://thread.gmane.org/gmane.science.nmr.relax.devel/3907). Modified: branches/relax_disp/specific_analyses/relax_disp/api.py Modified: branches/relax_disp/specific_analyses/relax_disp/api.py URL: http://svn.gna.org/viewcvs/relax/branches/relax_disp/specific_analyses/relax_disp/api.py?rev=20339&r1=20338&r2=20339&view=diff ============================================================================== --- branches/relax_disp/specific_analyses/relax_disp/api.py (original) +++ branches/relax_disp/specific_analyses/relax_disp/api.py Tue Jul 16 17:18:03 2013 @@ -48,7 +48,7 @@ from specific_analyses.api_common import API_common from specific_analyses.relax_disp.disp_data import average_intensity, find_intensity_keys, loop_cluster, loop_frq, loop_frq_point, loop_frq_point_key, loop_frq_point_time, loop_point, loop_time, relax_time, return_cpmg_frqs, return_index_from_disp_point, return_index_from_frq, return_key_from_disp_point_index, return_param_key_from_data, return_r2eff_arrays, return_spin_lock_nu1, return_value_from_frq_index, spin_ids_to_containers from specific_analyses.relax_disp.parameters import assemble_param_vector, assemble_scaling_matrix, disassemble_param_vector, linear_constraints, loop_parameters, param_conversion, param_index_to_param_info, param_num -from specific_analyses.relax_disp.variables import CPMG_EXP, FIXED_TIME_EXP, MODEL_LIST_FULL, MODEL_LM63, MODEL_CR72, MODEL_CR72_RED, MODEL_DPL94, MODEL_IT99, MODEL_M61, MODEL_M61B, MODEL_NOREX, MODEL_NS_2SITE_STAR, MODEL_NS_2SITE_STAR_RED, MODEL_R2EFF, R1RHO_EXP, VAR_TIME_EXP +from specific_analyses.relax_disp.variables import CPMG_EXP, FIXED_TIME_EXP, MODEL_LIST_FULL, MODEL_LM63, MODEL_CR72, MODEL_CR72_RED, MODEL_DPL94, MODEL_IT99, MODEL_M61, MODEL_M61B, MODEL_NOREX, MODEL_NS_2SITE_3D, MODEL_NS_2SITE_STAR, MODEL_NS_2SITE_STAR_RED, MODEL_R2EFF, R1RHO_EXP, VAR_TIME_EXP from target_functions.relax_disp import Dispersion from user_functions.data import Uf_tables; uf_tables = Uf_tables() from user_functions.objects import Desc_container @@ -703,6 +703,16 @@ params.append('r2') params += ['pA', 'dw', 'kex'] + # NS 2-site 3D model. + elif model == MODEL_NS_2SITE_3D: + print("The numerical solution for the 2-site Bloch-McConnell equations using 3D magnetisation vectors.") + params = [] + for frq in loop_frq(): + params.append('r2a') + for frq in loop_frq(): + params.append('r2b') + params += ['pA', 'dw', 'kex'] + # NS 2-site star model. elif model == MODEL_NS_2SITE_STAR: print("The numerical solution for the 2-site Bloch-McConnell equations using complex conjugate matrices.")