Author: tlinnet Date: Tue Jun 17 19:08:19 2014 New Revision: 24054 URL: http://svn.gna.org/viewcvs/relax?rev=24054&view=rev Log: Removal of the temporary offset argument. Task #7807 (https://gna.org/task/index.php?7807): Speed-up of dispersion models for Clustered analysis. Modified: branches/disp_spin_speed/lib/dispersion/ns_r1rho_2site.py branches/disp_spin_speed/target_functions/relax_disp.py Modified: branches/disp_spin_speed/lib/dispersion/ns_r1rho_2site.py URL: http://svn.gna.org/viewcvs/relax/branches/disp_spin_speed/lib/dispersion/ns_r1rho_2site.py?rev=24054&r1=24053&r2=24054&view=diff ============================================================================== --- branches/disp_spin_speed/lib/dispersion/ns_r1rho_2site.py (original) +++ branches/disp_spin_speed/lib/dispersion/ns_r1rho_2site.py Tue Jun 17 19:08:19 2014 @@ -58,7 +58,7 @@ from lib.linear_algebra.matrix_exponential import matrix_exponential -def ns_r1rho_2site(M0=None, matrix=None, r1rho_prime=None, omega=None, offset=None, r1=0.0, pA=None, pB=None, dw=None, k_AB=None, k_BA=None, spin_lock_fields=None, relax_time=None, inv_relax_time=None, back_calc=None, num_points=None, num_offsets=None): +def ns_r1rho_2site(M0=None, matrix=None, r1rho_prime=None, omega=None, offset=None, r1=0.0, pA=None, pB=None, dw=None, k_AB=None, k_BA=None, spin_lock_fields=None, relax_time=None, inv_relax_time=None, back_calc=None, num_points=None): """The 2-site numerical solution to the Bloch-McConnell equation for R1rho data. This function calculates and stores the R1rho values. @@ -106,7 +106,7 @@ # Loop over the spectrometer frequencies. for mi in range(NM): # Loop over offsets: - for oi in range(num_offsets[0, si, mi]): + for oi in range(NO): omega_i = omega[0, si, mi, oi, 0] offset_i = offset[0, si, mi, oi, 0] Modified: branches/disp_spin_speed/target_functions/relax_disp.py URL: http://svn.gna.org/viewcvs/relax/branches/disp_spin_speed/target_functions/relax_disp.py?rev=24054&r1=24053&r2=24054&view=diff ============================================================================== --- branches/disp_spin_speed/target_functions/relax_disp.py (original) +++ branches/disp_spin_speed/target_functions/relax_disp.py Tue Jun 17 19:08:19 2014 @@ -1662,7 +1662,7 @@ self.r20_struct[:] = multiply.outer( r1rho_prime.reshape(self.NE, self.NS, self.NM), self.no_nd_ones ) # Back calculate the R2eff values. - ns_r1rho_2site(M0=self.M0, matrix=self.matrix, r1rho_prime=self.r20_struct, omega=self.chemical_shifts, offset=self.offset, r1=self.r1, pA=pA, pB=pB, dw=self.dw_struct, k_AB=k_AB, k_BA=k_BA, spin_lock_fields=self.spin_lock_omega1, relax_time=self.relax_times, inv_relax_time=self.inv_relax_times, back_calc=self.back_calc, num_points=self.num_disp_points, num_offsets=self.num_offsets) + ns_r1rho_2site(M0=self.M0, matrix=self.matrix, r1rho_prime=self.r20_struct, omega=self.chemical_shifts, offset=self.offset, r1=self.r1, pA=pA, pB=pB, dw=self.dw_struct, k_AB=k_AB, k_BA=k_BA, spin_lock_fields=self.spin_lock_omega1, relax_time=self.relax_times, inv_relax_time=self.inv_relax_times, back_calc=self.back_calc, num_points=self.num_disp_points) # Clean the data for all values, which is left over at the end of arrays. self.back_calc = self.back_calc*self.disp_struct