Hi,

Great, the delta_omega value should be different when clustering.  For
the high values, you should check the fitted curves to see if you see
any issues.  It is likely that this is actually the values at the
minimum, and that noise or some experimental bias is pushing the
values too high.  But if that's what the data says, then there is
nothing you can do about it.  Adding constraints to prevent such
situations is just an ugly hack - the end result will be meaningless
anyway as it is not the minimum.  The best is to report the value with
its Monte Carlo simulation error.  You will probably find that the
errors for these high delta_omega values will also be large and hence
the large values are not statistically meaningful.

Regards,

Edward



On 30 April 2014 15:25, Troels Emtekær Linnet <[email protected]> wrote:
> Hi Edward.
>
> For 68 residues, i get this:
>
> # Parameter description:  The population for state A.
> # mol_name    res_num    res_name    spin_num    spin_name    value
>                error
> None          10         G           None        N
> 0.995627205128479    None
>
> # Parameter description:  The exchange rate.
> # mol_name    res_num    res_name    spin_num    spin_name    value
>                error
> None          10         G           None        N
> 843.138159024003    None
>
> # Parameter description:  The chemical shift difference between states
> A and B (in ppm).
> #
> # mol_name    res_num    res_name    spin_num    spin_name    value
>                error
> None          10         G           None        N
> 5.66240190353847    None
> None          11         D           None        N
> 7.24018919066445    None
> None          15         Q           None        N
> 1.27388427761583    None
> None          16         G           None        N
> 1.70637956735682    None
> None          37         G           None        N
> 1.39439146332152    None
> None          41         G           None        N
> 2.00489971256184    None
> None          42         L           None        N
> 1.14631824779138    None
> None          43         H           None        N
> 4.11812700604344    None
> None          46         H           None        N
> 6.74721119884288    None
> None          47         V           None        N
> 18.6941069719393    None
> None          49         E           None        N
> 7.41204467390198    None
> None          50         E           None        N
> 6.73571806460759    None
> None          51         E           None        N
> 2.6906237906698    None
> None          53         N           None        N
> 3.43636822580998    None
> None          54         T           None        N
> 1.72434404944155    None
> None          56         G           None        N
> 7.38662030427091    None
> None          57         C           None        N
> 1.88126168471543    None
> None          58         T           None        N
> 6.61594197477923    None
> None          61         G           None        N
> 3.42205122284923    None
> None          67         L           None        N
> 4.00714078384803    None
> None          68         S           None        N
> 3.02933093965657    None
> None          70         K           None        N
> 2.65894254799687    None
> None          72         G           None        N
> 4.01752138022632    None
> None          73         G           None        N
> 3.10502419263122    None
> None          75         K           None        N
> 5.52331683531287    None
> None          78         E           None        N
> 2.39121460031728    None
> None          79         R           None        N
> 2.95565292785431    None
> None          80         H           None        N
> 10.6521951761457    None
> None          81         V           None        N
> 6.46552900214463    None
> None          82         G           None        N
> 5.48378904252769    None
> None          85         G           None        N
> 4.72783895083071    None
> None          86         N           None        N
> 2.2535643167938    None
> None          87         V           None        N
> 3.42430152185329    None
> None          102        S           None        N
> 1.33719888517455    None
> None          103        V           None        N
> 1.78945522230369    None
> None          104        I           None        N
> 2.1193021535956    None
> None          105        S           None        N
> 1.20023816089299    None
> None          111        A           None        N
> 3.68849791596676    None
> None          112        I           None        N
> 1.92921136977377    None
> None          115        R           None        N
> 2.1336531230742    None
> None          118        V           None        N
> 1.1301287075642    None
> None          121        E           None        N
> 1.68619193009267    None
> None          123        A           None        N
> 4.91019478151119    None
> None          126        L           None        N
> 7.6255827307843    None
> None          127        G           None        N
> 4.89765215595432    None
> None          128        K           None        N
> 2.26502557102985    None
> None          129        G           None        N
> 1.79003350167683    None
> None          130        G           None        N
> 1.74650398353974    None
> None          131        N           None        N
> 4.91476102864345    None
> None          133        E           None        N
> 1.02559032422555    None
> None          134        S           None        N
> 0.842131709855722    None
> None          135        T           None        N
> 9.20627022843478    None
> None          137        T           None        N
> 8.00007213116674    None
> None          138        G           None        N
> 1.9412902050166    None
> None          139        N           None        N
> 6.51160366265863    None
> None          140        A           None        N
> 8.89216425477085    None
> None          141        G           None        N
> 2.354941400505    None
> None          142        S           None        N
> 3.50895251891688    None
> None          143        R           None        N
> 2.65884864234097    None
> None          146        C           None        N
> 2.92485233744021    None
> None          147        G           None        N
> 4.71130879214043    None
>
>
> So dw is moving fine.
>
> But we do though think that dw has high values.
> There is a 18 ppm and 10 ppm in there.
>
> Now trying with ShereKhan.
>
> Best
> Troels
>
> 2014-04-30 10:45 GMT+02:00 Edward d'Auvergne <[email protected]>:
>> Hi,
>>
>> I should expand on the statistics a bit more.  Maybe using AIC would
>> clarify the noise vs. real data components.  Here is a short table:
>>
>> Set          Chi2    k  AIC
>> Individual   32.97  10  52.97
>> Cluster      48.79   8  64.79
>>
>> So even using AIC, the individual fit is better.  Statistically it is
>> not that you are just fitting more noise in the non-clustered fit.
>> That is significant!  One thing I noticed is that dw is the same for
>> both spins in the clustered fit.  Could you check if this is the case
>> for other clustering cases?  It must be different for each spin.
>> Maybe there is an important bug there.
>>
>> Regards,
>>
>> Edward
>>
>>
>>
>> On 30 April 2014 10:16, Edward d'Auvergne <[email protected]> wrote:
>>>> I tried to generate sherekhan output, but since I have time_T2 of 0.04
>>>> and 0.06, for the two fields,
>>>> I cannot generate the input files for ShereKhan.
>>>
>>> ShereKhan should support this, and it would be a good test for relax.
>>> The second line of the input file has this time.  Was it that relax
>>> could not create the input files rather than ShereKhan not handling
>>> this?
>>>
>>>
>>>> My problem origins from that I would like to compare results from Igor
>>>> Pro script.
>>>> Yet, another software solution.
>>>
>>> Have you run the Igor Pro script to compare to relax?  With the same
>>> input data, all software solutions should give the same result.  This
>>> is important - you need to determine if the issue is with relax or
>>> with the data itself.  It is best to first assume that the problem is
>>> with relax, then see if other software produces a different result
>>> (the more comparisons here the better).  Maybe relax is not handling
>>> the two different times correctly.  Otherwise if everything has the pA
>>> = 0.5 problem then the solution, if one exists, will be very
>>> different.
>>>
>>>
>>>> I now got the expected pA values of 0.97 if I did a cluster of two 
>>>> residues.
>>>
>>> This could indicate that the pA = 0.5 issue is in the data itself,
>>> probably due to noise.  You should confirm this by comparing to other
>>> software though.  Comparing to the 'NS CPMG 2-site expanded' might
>>> also be useful.
>>>
>>>
>>>> If I do an initial Grid inc of 21, use
>>>> relax_disp.set_grid_r20_from_min_r2eff(force=False) I get this.
>>>
>>> As I mentioned before
>>> (http://thread.gmane.org/gmane.science.nmr.relax.scm/20597/focus=5390),
>>> maybe it would be better to shorten this user function name as it is a
>>> little misleading - it is about custom value setting and not the grid
>>> search, despite it being useful for the later.
>>>
>>>
>>>> :10@N GRID   r2600=20.28 r2500=18.48 dw=1.0 pA=0.900 kex=2000.80
>>>> chi2=28.28 spin_id=:10@N resi=10 resn=G
>>>> :10@N MIN    r2600=19.64 r2500=17.88 dw=0.7 pA=0.500 kex=2665.16
>>>> chi2=14.61 spin_id=:10@N resi=10 resn=G
>>>> :10@N Clust  r2600=18.43 r2500=16.98 dw=2.7 pA=0.972 kex=3831.77
>>>> chi2=48.79 spin_id=:10@N resi=10 resn=G
>>>>
>>>> :11@N GRID   r2600=19.54 r2500=17.96 dw=1.0 pA=0.825 kex=3500.65
>>>> chi2=47.22 spin_id=:11@N resi=11 resn=D
>>>> :11@N MIN    r2600=14.98 r2500=15.08 dw=1.6 pA=0.760 kex=6687.15
>>>> chi2=18.36 spin_id=:11@N resi=11 resn=D
>>>> :11@N Clust  r2600=18.19 r2500=17.31 dw=2.7 pA=0.972 kex=3831.77
>>>> chi2=48.79 spin_id=:11@N resi=11 resn=D
>>>
>>> If you sum the chi-squared values, which is possible as these are all
>>> the same model, then you can compare the individual fits and the
>>> clustered fit.  The individual fit total chi-squared value is 32.97.
>>> The cluster value is 48.79.  This is very important - the individual
>>> fit is much, much better.  You should make a plot of the fitted curves
>>> for both and compare.  Note that a better fit does not mean a better
>>> result, as you are fitting both a data component and noise component.
>>> So the better fit might be due to the noise component.  This is why
>>> clustering exists.
>>>
>>>
>>>> Ideally, I would like to cluster 68 residues.
>>>>
>>>> But as you can see, if several of my residues start out with dw/pA far
>>>> from the Clustered result, this minimisation takes
>>>> hilarious long time.
>>>
>>> I can see how this would be a problem for you mass screening
>>> exercises.  This will probably require a lot of investigation on your
>>> part to solve, as I have not seen any solution published in the
>>> literature.  Though if you could find a solution in the literature,
>>> that would probably save you a lot of time.  You could also ask others
>>> in the field.  If you remember
>>> (http://thread.gmane.org/gmane.science.nmr.relax.devel/4647/focus=4648),
>>> you changed the parameter averaging to the parameter median for the
>>> clustering.  So maybe that is having an effect.  Anyway, you need to
>>> first compare to other software or models and see if there is a
>>> problem in relax first, before trying to invent a solution.
>>>
>>> Regards,
>>>
>>> Edward

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