Hi Edward.

I think I in the start tried following this path.

But I realised with all the "R1 fit" models, that the very important,
relax_disp.select_model(model)

setup all information for this model.

As this was also a new model implementation, I also wanted the
flexibility to be able to select the desired model, and
be able to compare.

I would suggest that this functionality is not digged further down the
code, before more experience is collected.

Best
Troels



2014-08-20 16:22 GMT+02:00 Edward d'Auvergne <[email protected]>:
> Hi,
>
> What would be even more powerful would be to shift this functionality
> even deeper down and merging the 'No Rex' and 'No Rex R1rho off res'
> models into one, just as the 'R2eff' model covers both the exponential
> curve-fitting via minimisation and the two-point approximation by
> calculation.  Rather than switching the model name for the user, the
> target function can be switched.  The 'No Rex R1 fit' model could then
> be created (by simply renaming 'No Rex R1rho off res R1 fit') and this
> would then eventually handle CPMG data as well.
>
> The reason for this is simple.  In the future, certain interested
> parties (you probably know who) plans on developing a combined CPMG
> and R1rho model and on analysing this data together.  This will need a
> 'No Rex' model for statistical comparisons.  The splitting of 'No Rex'
> into two models as is currently coded is incompatible with this.  A
> 'No Rex' model which has a loop over experiment types "for ei in
> range(self.NE):" switching to the different functionality would be a
> better solution.
>
> Regards,
>
> Edward
>
>
> On 20 August 2014 16:09,  <[email protected]> wrote:
>> Author: tlinnet
>> Date: Wed Aug 20 16:09:40 2014
>> New Revision: 25100
>>
>> URL: http://svn.gna.org/viewcvs/relax?rev=25100&view=rev
>> Log:
>> Made the GUI selection of models for relaxation dispersion more simple.
>>
>> After the implementation of a function which will translate the models, the
>> 'No Rex' model will be converted to the 'No Rex' model for R1rho 
>> off-resonance.
>>
>> Also the corresponding 'R1 fit' model will be chosen istead, if R1 data has 
>> not been loaded.
>>
>> This makes the model selection easier in the GUI interface.
>>
>> Modified:
>>     trunk/gui/analyses/auto_relax_disp.py
>>
>> Modified: trunk/gui/analyses/auto_relax_disp.py
>> URL: 
>> http://svn.gna.org/viewcvs/relax/trunk/gui/analyses/auto_relax_disp.py?rev=25100&r1=25099&r2=25100&view=diff
>> ==============================================================================
>> --- trunk/gui/analyses/auto_relax_disp.py       (original)
>> +++ trunk/gui/analyses/auto_relax_disp.py       Wed Aug 20 16:09:40 2014
>> @@ -715,8 +715,8 @@
>>          MODEL_R2EFF,
>>          None,
>>          MODEL_NOREX,
>> -        MODEL_NOREX_R1RHO,
>> -        MODEL_NOREX_R1RHO_FIT_R1,
>> +#        MODEL_NOREX_R1RHO,
>> +#        MODEL_NOREX_R1RHO_FIT_R1,
>>          None,
>>          MODEL_LM63,
>>          MODEL_LM63_3SITE,
>> @@ -735,15 +735,15 @@
>>          MODEL_M61,
>>          MODEL_M61B,
>>          MODEL_DPL94,
>> -        MODEL_DPL94_FIT_R1,
>> +#        MODEL_DPL94_FIT_R1,
>>          MODEL_TP02,
>> -        MODEL_TP02_FIT_R1,
>> +#        MODEL_TP02_FIT_R1,
>>          MODEL_TAP03,
>> -        MODEL_TAP03_FIT_R1,
>> +#        MODEL_TAP03_FIT_R1,
>>          MODEL_MP05,
>> -        MODEL_MP05_FIT_R1,
>> +#        MODEL_MP05_FIT_R1,
>>          MODEL_NS_R1RHO_2SITE,
>> -        MODEL_NS_R1RHO_2SITE_FIT_R1,
>> +#        MODEL_NS_R1RHO_2SITE_FIT_R1,
>>          MODEL_NS_R1RHO_3SITE_LINEAR,
>>          MODEL_NS_R1RHO_3SITE,
>>          None,
>> @@ -756,8 +756,8 @@
>>          "{%s/%s, %s}" % (r2eff, r1rho, i0),
>>          None,
>>          "{%s, ...}" % (r2),
>> -        "{%s, ...}" % (r2),
>> -        "{%s, %s, ...}" % (r1, r2),
>> +#        "{%s, ...}" % (r2),
>> +#        "{%s, %s, ...}" % (r1, r2),
>>          None,
>>          "{%s, ..., %s, %s}" % (r2, phi_ex, kex),
>>          "{%s, ..., %s, kB, %s, kC}" % (r2, phi_exB, phi_exC),
>> @@ -776,15 +776,15 @@
>>          "{%s, ..., %s, %s}" % (r1rho_prime, phi_ex, kex),
>>          "{%s, ..., pA, %s, %s}" % (r1rho_prime, dw, kex),
>>          "{%s, ..., %s, %s}" % (r1rho_prime, phi_ex, kex),
>> -        "{%s, %s, ..., %s, %s}" % (r1, r1rho_prime, phi_ex, kex),
>> +#        "{%s, %s, ..., %s, %s}" % (r1, r1rho_prime, phi_ex, kex),
>>          "{%s, ..., pA, %s, %s}" % (r1rho_prime, dw, kex),
>> -        "{%s, %s, ..., pA, %s, %s}" % (r1, r1rho_prime, dw, kex),
>> +#        "{%s, %s, ..., pA, %s, %s}" % (r1, r1rho_prime, dw, kex),
>>          "{%s, ..., pA, %s, %s}" % (r1rho_prime, dw, kex),
>> -        "{%s, %s, ..., pA, %s, %s}" % (r1, r1rho_prime, dw, kex),
>> +#        "{%s, %s, ..., pA, %s, %s}" % (r1, r1rho_prime, dw, kex),
>>          "{%s, ..., pA, %s, %s}" % (r1rho_prime, dw, kex),
>> -        "{%s, %s, ..., pA, %s, %s}" % (r1, r1rho_prime, dw, kex),
>> +#        "{%s, %s, ..., pA, %s, %s}" % (r1, r1rho_prime, dw, kex),
>>          "{%s, ..., pA, %s, %s}" % (r1rho_prime, dw, kex),
>> -        "{%s, %s, ..., pA, %s, %s}" % (r1, r1rho_prime, dw, kex),
>> +#        "{%s, %s, ..., pA, %s, %s}" % (r1, r1rho_prime, dw, kex),
>>          "{%s, ..., pA, %s, %s, pB, %s, %s}" % (r1rho_prime, dw_AB, kAB, 
>> dw_BC, kBC),
>>          "{%s, ..., pA, %s, %s, pB, %s, %s, %s}" % (r1rho_prime, dw_AB, kAB, 
>> dw_BC, kBC, kAC),
>>          None,
>> @@ -797,8 +797,8 @@
>>          "The base model for determining the %s/%s values and errors for all 
>> other models." % (r2eff, r1rho),
>>          None,
>>          "The model for no chemical exchange relaxation.",
>> -        "The model for no chemical exchange being present, for 
>> off-resonance R1rho-type experiments.  R1rho = R1 * cos(theta)^2 + 
>> r1rho_prime * sin(theta)^2.",
>> -        "The model for no chemical exchange being present, for 
>> off-resonance R1rho-type experiments whereby R1 is fit.  R1rho = R1 * 
>> cos(theta)^2 + r1rho_prime * sin(theta)^2.",
>> +#        "The model for no chemical exchange being present, for 
>> off-resonance R1rho-type experiments.  R1rho = R1 * cos(theta)^2 + 
>> r1rho_prime * sin(theta)^2.",
>> +#        "The model for no chemical exchange being present, for 
>> off-resonance R1rho-type experiments whereby R1 is fit.  R1rho = R1 * 
>> cos(theta)^2 + r1rho_prime * sin(theta)^2.",
>>          None,
>>          "The original Luz and Meiboom (1963) 2-site fast exchange 
>> equation.",
>>          "The original Luz and Meiboom (1963) 3-site fast exchange 
>> equation.",
>> @@ -817,15 +817,15 @@
>>          "The Meiboom (1961) 2-site fast exchange equation.",
>>          "The Meiboom (1961) 2-site equation for all time scales with pA >> 
>> pB.",
>>          "The Davis, Perlman and London (1994) 2-site fast exchange 
>> equation.",
>> -        "The Davis, Perlman and London (1994) 2-site fast exchange 
>> equation, whereby R1 is fit.",
>> +#        "The Davis, Perlman and London (1994) 2-site fast exchange 
>> equation, whereby R1 is fit.",
>>          "The Trott and Palmer (2002) 2-site equation for all time scales.",
>> -        "The Trott and Palmer (2002) 2-site equation for all time scales, 
>> whereby R1 is fit.",
>> +#        "The Trott and Palmer (2002) 2-site equation for all time scales, 
>> whereby R1 is fit.",
>>          "The Trott, Abergel and Palmer (2003) off-resonance 2-site equation 
>> for all time scales.",
>> -        "The Trott, Abergel and Palmer (2003) off-resonance 2-site equation 
>> for all time scales, whereby R1 is fit.",
>> +#        "The Trott, Abergel and Palmer (2003) off-resonance 2-site 
>> equation for all time scales, whereby R1 is fit.",
>>          "The Miloushev and Palmer (2005) off-resonance 2-site equation for 
>> all time scales.",
>> -        "The Miloushev and Palmer (2005) off-resonance 2-site equation for 
>> all time scales, whereby R1 is fit.",
>> +#        "The Miloushev and Palmer (2005) off-resonance 2-site equation for 
>> all time scales, whereby R1 is fit.",
>>          "The 2-site numerical solution using 3D magnetisation vectors.",
>> -        "The 2-site numerical solution using 3D magnetisation vectors, 
>> whereby R1 is fit.",
>> +#        "The 2-site numerical solution using 3D magnetisation vectors, 
>> whereby R1 is fit.",
>>          "The 3-site linearised numerical solution using 3D magnetisation 
>> vectors.",
>>          "The 3-site numerical solution using 3D magnetisation vectors.",
>>          None,
>>
>>
>> _______________________________________________
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>>
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>
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