mailr23961 - /branches/disp_spin_speed/target_functions/relax_disp.py


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Posted by tlinnet on June 15, 2014 - 15:15:
Author: tlinnet
Date: Sun Jun 15 15:15:19 2014
New Revision: 23961

URL: http://svn.gna.org/viewcvs/relax?rev=23961&view=rev
Log:
Changed the target function of NS CPMG 2site STAR, to reflect the input to 
the function.

Task #7807 (https://gna.org/task/index.php?7807): Speed-up of dispersion 
models for Clustered analysis.

Modified:
    branches/disp_spin_speed/target_functions/relax_disp.py

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=23961&r1=23960&r2=23961&view=diff
==============================================================================
--- branches/disp_spin_speed/target_functions/relax_disp.py     (original)
+++ branches/disp_spin_speed/target_functions/relax_disp.py     Sun Jun 15 
15:15:19 2014
@@ -396,7 +396,7 @@
 
 
         # Setup special numpy array structures, for higher dimensional 
computation.
-        test_models = [MODEL_B14, MODEL_B14_FULL, MODEL_CR72, 
MODEL_CR72_FULL, MODEL_DPL94, MODEL_IT99, MODEL_LM63, MODEL_M61, MODEL_M61B, 
MODEL_MP05, MODEL_NS_CPMG_2SITE_3D, MODEL_NS_CPMG_2SITE_3D_FULL, 
MODEL_NS_CPMG_2SITE_EXPANDED, MODEL_TAP03, MODEL_TP02, MODEL_TSMFK01]
+        test_models = [MODEL_B14, MODEL_B14_FULL, MODEL_CR72, 
MODEL_CR72_FULL, MODEL_DPL94, MODEL_IT99, MODEL_LM63, MODEL_M61, MODEL_M61B, 
MODEL_MP05, MODEL_NS_CPMG_2SITE_3D, MODEL_NS_CPMG_2SITE_3D_FULL, 
MODEL_NS_CPMG_2SITE_STAR, MODEL_NS_CPMG_2SITE_STAR_FULL, 
MODEL_NS_CPMG_2SITE_EXPANDED, MODEL_TAP03, MODEL_TP02, MODEL_TSMFK01]
 
         if model in test_models + [MODEL_NOREX]:
             # Get the shape of back_calc structure.
@@ -666,47 +666,26 @@
         @rtype:         float
         """
 
-        # Once off parameter conversions.
-        pB = 1.0 - pA
-        k_BA = pA * kex
-        k_AB = pB * kex
-
-        # Set up the matrix that contains the exchange terms between the two 
states A and B.
-        self.Rex[0, 0] = -k_AB
-        self.Rex[0, 1] = k_BA
-        self.Rex[1, 0] = k_AB
-        self.Rex[1, 1] = -k_BA
-
-        # This is a vector that contains the initial magnetizations 
corresponding to the A and B state transverse magnetizations.
-        self.M0[0] = pA
-        self.M0[1] = pB
-
-        # Chi-squared initialisation.
-        chi2_sum = 0.0
-
-        # Loop over the spins.
-        for si in range(self.num_spins):
-            # Loop over the spectrometer frequencies.
-            for mi in range(self.num_frq):
-                # The R20 index.
-                r20_index = mi + si*self.num_frq
-
-                # Convert dw from ppm to rad/s.
-                dw_frq = dw[si] * self.frqs[0][si][mi]
-
-                # Back calculate the R2eff values.
-                r2eff_ns_cpmg_2site_star(Rr=self.Rr, Rex=self.Rex, 
RCS=self.RCS, R=self.R, M0=self.M0, r20a=R20A[r20_index], 
r20b=R20B[r20_index], dw=dw_frq, inv_tcpmg=self.inv_relax_times[0][mi], 
tcp=self.tau_cpmg[0][mi], back_calc=self.back_calc[0][si][mi][0], 
num_points=self.num_disp_points[0][si][mi][0], power=self.power[0][mi])
-
-                # For all missing data points, set the back-calculated value 
to the measured values so that it has no effect on the chi-squared value.
-                for di in range(self.num_disp_points[0][si][mi][0]):
-                    if self.missing[0][si][mi][0][di]:
-                        self.back_calc[0][si][mi][0][di] = 
self.values[0][si][mi][0][di]
-
-                # Calculate and return the chi-squared value.
-                chi2_sum += chi2(self.values[0][si][mi][0], 
self.back_calc[0][si][mi][0], self.errors[0][si][mi][0])
-
-        # Return the total chi-squared value.
-        return chi2_sum
+        # Convert dw from ppm to rad/s. Use the out argument, to pass 
directly to structure.
+        multiply( multiply.outer( dw.reshape(self.NE, self.NS), 
self.nm_no_nd_struct ), self.frqs_a, out=self.dw_struct )
+
+        # Reshape R20A and R20B to per experiment, spin and frequency.
+        self.r20a_struct[:] = multiply.outer( R20A.reshape(self.NE, self.NS, 
self.NM), self.no_nd_struct )
+        self.r20b_struct[:] = multiply.outer( R20B.reshape(self.NE, self.NS, 
self.NM), self.no_nd_struct )
+
+        # Back calculate the R2eff values.
+        r2eff_ns_cpmg_2site_star(Rr=self.Rr, Rex=self.Rex, RCS=self.RCS, 
R=self.R, M0=self.M0, r20a=self.r20a_struct, r20b=self.r20b_struct, pA=pA, 
dw=self.dw_struct, dw_orig=dw, kex=kex, inv_tcpmg=self.inv_relax_times_a, 
tcp=self.tau_cpmg_a, back_calc=self.back_calc_a, 
num_points=self.num_disp_points_a, power=self.power_a)
+
+        # Clean the data for all values, which is left over at the end of 
arrays.
+        self.back_calc_a = self.back_calc_a*self.disp_struct
+
+        ## For all missing data points, set the back-calculated value to the 
measured values so that it has no effect on the chi-squared value.
+        if self.has_missing:
+            # Replace with values.
+            self.back_calc_a[self.mask_replace_blank.mask] = 
self.values_a[self.mask_replace_blank.mask]
+
+        ## Calculate the chi-squared statistic.
+        return chi2_rankN(self.values_a, self.back_calc_a, self.errors_a)
 
 
     def calc_ns_mmq_3site_chi2(self, R20A=None, R20B=None, R20C=None, 
dw_AB=None, dw_BC=None, dwH_AB=None, dwH_BC=None, pA=None, pB=None, 
kex_AB=None, kex_BC=None, kex_AC=None):




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