r24162 - /branches/disp_spin_speed/lib/dispersion/ns_cpmg_2site_3d.py -- June 19, 2014 - 17:42

Author: tlinnet
Date: Thu Jun 19 17:42:23 2014
New Revision: 24162

URL: http://svn.gna.org/viewcvs/relax?rev=24162&view=rev
Log:
Removed unused variables in NS CPMG 2site 3D, to clean up the code.

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_cpmg_2site_3d.py

Modified: branches/disp_spin_speed/lib/dispersion/ns_cpmg_2site_3d.py
URL: 
http://svn.gna.org/viewcvs/relax/branches/disp_spin_speed/lib/dispersion/ns_cpmg_2site_3d.py?rev=24162&r1=24161&r2=24162&view=diff
==============================================================================
--- branches/disp_spin_speed/lib/dispersion/ns_cpmg_2site_3d.py (original)
+++ branches/disp_spin_speed/lib/dispersion/ns_cpmg_2site_3d.py Thu Jun 19 
17:42:23 2014
@@ -157,7 +157,6 @@
             # Loop over the time points, back calculating the R2eff values.
             for di in range(num_points_si_mi):
                 # Extract the values from the higher dimensional arrays.
-                tcp_si_mi_di = tcp[0, si, mi, 0, di]
                 inv_tcpmg_si_mi_di = inv_tcpmg[0, si, mi, 0, di]
                 power_si_mi_di = int(power[0, si, mi, 0, di])
                 r20a_si_mi_di = r20a[0, si, mi, 0, di]
@@ -166,8 +165,6 @@
                 Mint_i = Mint_mat[0, si, mi, 0, di]
 
                 # This matrix is a propagator that will evolve the 
magnetization with the matrix R for a delay tcp.
-                Rexpo_i = Rexpo_mat[0, si, mi, 0, di]
-                r180x_i = r180x_mat[0, si, mi, 0, di]
                 evolution_matrix_i = evolution_matrix_mat[0, si, mi, 0, di]
 
                 # Loop over the CPMG elements, propagating the magnetisation.