Hi Troels,

As I mentioned previously (in the thread at
http://thread.gmane.org/gmane.science.nmr.relax.scm/20984), it is good
practice to separate the two changes here.  I.e. have one commit for
the API change, and one commit for the other changes.

Cheers,

Edward



On 20 May 2014 01:47,  <[email protected]> wrote:
> Author: tlinnet
> Date: Tue May 20 01:47:30 2014
> New Revision: 23246
>
> URL: http://svn.gna.org/viewcvs/relax?rev=23246&view=rev
> Log:
> Math-domain catching for model: 'NS CPMG 2-site expanded'.
>
> task #7793: (https://gna.org/task/?7793) Speed-up of dispersion models.
>
> This is to implement catching of math domain errors, before they occur.
> These can be found via the --numpy-raise function to the systemtests.
>
> To make the code look clean, the class object "back_calc" is no longer
> being updated per time point, but is updated in the relax_disp target 
> function in
> one go.
>
> Modified:
>     branches/disp_speed/lib/dispersion/ns_cpmg_2site_expanded.py
>     branches/disp_speed/target_functions/relax_disp.py
>
> Modified: branches/disp_speed/lib/dispersion/ns_cpmg_2site_expanded.py
> URL: 
> http://svn.gna.org/viewcvs/relax/branches/disp_speed/lib/dispersion/ns_cpmg_2site_expanded.py?rev=23246&r1=23245&r2=23246&view=diff
> ==============================================================================
> --- branches/disp_speed/lib/dispersion/ns_cpmg_2site_expanded.py        
> (original)
> +++ branches/disp_speed/lib/dispersion/ns_cpmg_2site_expanded.py        Tue 
> May 20 01:47:30 2014
> @@ -235,14 +235,13 @@
>  """
>
>  # Python module imports.
> -from math import log
> -from numpy import exp, power, sqrt
> +from numpy import array, exp, isfinite, power, log, min, sqrt, sum
>
>  # relax module imports.
>  from lib.float import isNaN
>
>
> -def r2eff_ns_cpmg_2site_expanded(r20=None, pA=None, dw=None, k_AB=None, 
> k_BA=None, relax_time=None, inv_relax_time=None, tcp=None, back_calc=None, 
> num_points=None, num_cpmg=None):
> +def r2eff_ns_cpmg_2site_expanded(r20=None, pA=None, dw=None, k_AB=None, 
> k_BA=None, relax_time=None, inv_relax_time=None, tcp=None, num_points=None, 
> num_cpmg=None):
>      """The 2-site numerical solution to the Bloch-McConnell equation using 
> complex conjugate matrices.
>
>      This function calculates and stores the R2eff values.
> @@ -264,9 +263,7 @@
>      @type inv_relax_time:       float
>      @keyword tcp:               The tau_CPMG times (1 / 4.nu1).
>      @type tcp:                  numpy rank-1 float array
> -    @keyword back_calc:         The array for holding the back calculated 
> R2eff values.  Each element corresponds to one of the CPMG nu1 frequencies.
> -    @type back_calc:            numpy rank-1 float array
> -    @keyword num_points:        The number of points on the dispersion 
> curve, equal to the length of the tcp and back_calc arguments.
> +    @keyword num_points:        The number of points on the dispersion 
> curve, equal to the length of the tcp .
>      @type num_points:           int
>      @keyword num_cpmg:          The array of numbers of CPMG blocks.
>      @type num_cpmg:             numpy int16, rank-1 array
> @@ -342,7 +339,15 @@
>      t116 = power(0.5*(t97_t99 + t112), t115)
>      t118 = 1.0/t112
>      t120 = t97_nt99 + t112
> -    t122 = power(0.5*(t97_t99 - t112), t115)
> +
> +    half_t97_t99_m_t112 = 0.5*(t97_t99 - t112)
> +    # Catch math domain error of power(val < 1.e-7, 40).
> +    # This is when abs(half_t97_t99_m_t112) < 1.e-7.
> +    if min(abs(half_t97_t99_m_t112.real)) < 1.e-7:
> +        R2eff = array([1e100]*num_points)
> +        return R2eff
> +
> +    t122 = power(half_t97_t99_m_t112, t115)
>      t127 = 0.5/t108
>      t120_t122 = t120*t122
>      t139 = 0.5/(k_AB + k_BA) * ((t120_t122 - t113*t116)*t118*k_BA + 
> (t120_t122 - t116*t120)*t127*t113*t118*k_AB)
> @@ -355,8 +360,11 @@
>      Mx = intensity / intensity0
>
>      # Calculate the R2eff using a two-point approximation, i.e. assuming 
> that the decay is mono-exponential, and store it for each dispersion point.
> -    for i in range(num_points):
> -        if Mx[i] <= 0.0 or isNaN(Mx[i]):
> -            back_calc[i] = 1e99
> -        else:
> -            back_calc[i]= -inv_relax_time * log(Mx[i])
> +    R2eff = -inv_relax_time * log(Mx)
> +
> +    # Catch errors, taking a sum over array is the fastest way to check for
> +    # +/- inf (infinity) and nan (not a number).
> +    if not isfinite(sum(R2eff)) or min(Mx) <= 0.0 or not isfinite(sum(Mx)):
> +        R2eff = array([1e100]*num_points)
> +
> +    return R2eff
>
> Modified: branches/disp_speed/target_functions/relax_disp.py
> URL: 
> http://svn.gna.org/viewcvs/relax/branches/disp_speed/target_functions/relax_disp.py?rev=23246&r1=23245&r2=23246&view=diff
> ==============================================================================
> --- branches/disp_speed/target_functions/relax_disp.py  (original)
> +++ branches/disp_speed/target_functions/relax_disp.py  Tue May 20 01:47:30 
> 2014
> @@ -1480,7 +1480,7 @@
>                  dw_frq = dw[si] * self.frqs[0][si][mi]
>
>                  # Back calculate the R2eff values.
> -                r2eff_ns_cpmg_2site_expanded(r20=R20[r20_index], pA=pA, 
> dw=dw_frq, k_AB=k_AB, k_BA=k_BA, relax_time=self.relax_times[0][mi], 
> inv_relax_time=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], num_cpmg=self.power[0][mi])
> +                self.back_calc[0][si][mi][0] = 
> r2eff_ns_cpmg_2site_expanded(r20=R20[r20_index], pA=pA, dw=dw_frq, k_AB=k_AB, 
> k_BA=k_BA, relax_time=self.relax_times[0][mi], 
> inv_relax_time=self.inv_relax_times[0][mi], tcp=self.tau_cpmg[0][mi], 
> num_points=self.num_disp_points[0][si][mi][0], num_cpmg=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]):
>
>
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