Hey,

Farrow et al. (1994) Biochemistry, 33: 5984-6003 also draw a similar 
conclusion
(paragraph starting at bottom left of p. 5988) and apply the RMS value of the
noise as an estimate of the standard deviation of peak intensity. If I'm not
mistaken this is the exact assumption made by relax for steady-state NOE error
propagation by the sum of squares equation from this paper as well.

Also of interest on p. 5988,

"The distribution of the difference in intensities of identical peaks in
duplicate spectra should have a standard deviation [sqrt(2)] times 
greater than
the standard deviation of the individual peaks."

They again conclude that duplicate and RMS baseline data errors are consistent
within those bounds. If the Kay and Palmer labs are going with this conclusion
(even if it doesn't really tell us which error is more appropriate), it seems
like it's a good bet that you can estimate standard deviation this way.

However, I'm sill not clear on the relationship between curve fit 
errors and the
errors measured directly from the spectra. I'm not sure how the nonlinear
fitting error factors in for relax R1, R2 curve-fitting scripts. Certainly, if
curve-fit error alone could be used that would make things easier since no
error measurement on the T1/T2 experiment spectra would be needed, you could
just dump the peak heights to relax.

Tyler




Quoting Tyler Reddy <[EMAIL PROTECTED]>:

> Hi,
>
> I'll try to dig up those references. The other thing I find confusing is that
> some groups use the curve fit error for the parameters. So, the errors in R1
> and R2 per residue are actually from the nonlinear curve fitting process
> itself. In theory, if there is no error in peak height then the fit is
> perfect.
> So I wonder if there is yet another relationship to think about if 
> you want to
> use those values?!
>
> I have these values already for T1 and T2 parameters and their curve fitting
> errors (though I haven't figured out how to propagate these errors to the
> reciprocal rate constants, or if that will even be meaningful), but I'm not
> sure how they compare to the other 2 'error types' we are talking about.
>
> Certainly, S/N = peak height/RMS baseline noise  (From Cavanagh textbook)
>
> And while there are many references that throw around the sqrt(2) in various
> equations, I haven't seen a comprehensive explanation yet.
>
> Tyler
>
>
>
>
> Quoting Edward d'Auvergne <[EMAIL PROTECTED]>:
>
>> Hi,
>>
>> That was the reference I used many years ago when I first added these
>> abilities to relax.  The text is a little confusing, but the important
>> line is the first of that paragraph you mention:
>>
>> The uncertainties in the measured peak heights, sigma_h, were set
>> equal to the root-mean-square baseline noise in the spectra.
>>
>> So if one looks at the code in relax, there is no multiplication by
>> sqrt(2).  As this was a long time ago, I'm not sure if this is the
>> most correct approach.  The confusing chi-squared tests between the
>> sigma_h and sqrt(2)*sigma_h may not statistically significant but
>> considering that the parameter number is identical in both cases, the
>> weighting constant simply changes, then no statistically significant
>> difference doesn't mean that one weight is better than the other or
>> that both weights are correct.
>>
>> There is another early reference (or two) in which the NOE error
>> formula is given.  I think that may have more information, but I'm
>> struggling to remember what that reference is and cannot find it at
>> the moment.  And there may be more recent papers performing a much
>> more thorough noise analysis.  It could even be done using synthetic
>> spectra with white noise added (I recently did this to test the effect
>> of white noise on the uncertainty in peak chemical shift position to
>> validate Ad Bax's RDC error formula LW/SN - strangely the results were
>> far more complex than this formula).
>>
>> There is a bit of time to find the correct baseplane RMSD to peak
>> height uncertainty as I need to wait for Sebastien to finish the work
>> with the loading of NMRView (as well as Sparky and XEasy) peak list
>> intensities.  The rearrangements I plan to do will affect the code he
>> is working on.
>>
>> Regards,
>>
>> Edward
>>
>>
>>
>> On Mon, Oct 13, 2008 at 7:44 PM, Tyler Reddy <[EMAIL PROTECTED]> wrote:
>>> Hi Edward,
>>>
>>> Palmer et al. (1991) JACS. 113: 4371-4380 is a nice reference for the error
>>> conversion. It looks like the value for standard deviation between peaks in
>>> paired spectra is sqrt(2) multiplied by the base plane RMS value (in
>>> particular, see the short paragraph at the top right of page 4375 in this
>>> manuscript). However, the authors seem to use the base plane RMS values
>>> regardless, and then verify that the qualitative conclusions do not change
>>> when
>>> using the more conservative error estimates (i.e. multiplying by 1.4).
>>>
>>> There's an extensive discussion of using chi-square critical values to
>>> verify
>>> the validity of this relationship between the noise types, though I must
>>> concede that I don't grasp all the details after the first reading.
>>>
>>> Tyler
>>>
>>>
>>> Quoting Edward d'Auvergne <[EMAIL PROTECTED]>:
>>>
>>>> Hi,
>>>>
>>>> There are three ways that an error analysis can be done for relaxation
>>>> curve fitting, although one of those is only partly implemented in
>>>> relax at the moment (that means it won't work until I write some
>>>> computer code).  These are:
>>>>
>>>> 1.  Collect all spectra in duplicate, triplicate, or more if you
>>>> really have lot of NMR time to kill, for absolutely no reason.  The
>>>> peak intensity error for a single spin is calculated as the standard
>>>> deviation for each peak.  Because this is inaccurate for a low replica
>>>> number, this error is averaged for all peaks to give one error per
>>>> spectrum.  This error is then used in the Monte Carlo simulations.
>>>>
>>>> 2.  If only some spectra are duplicated, then the average of the
>>>> errors for all spectra is calculated.  This gives a single error value
>>>> for all spins and all spectra.  This is then used in the Monte Carlo
>>>> simulations.
>>>>
>>>> 3.  This is the error analysis technique which is not fully
>>>> implemented yet.  If no spectra are recorded in duplicate, then one
>>>> needs to use the RMSD of the base plane noise.  This is similar to
>>>> what relax uses for the NOE analysis (hence shouldn't be too hard to
>>>> implement for relaxation curve fitting).  I would need to find the
>>>> reference, but I think this value needs to be divided or multiplied by
>>>> root 2 to convert it to a peak height uncertainty.  Does anyone know a
>>>> reference for this?  Then a separate error value for all spins and all
>>>> spectra can be used in the Monte Carlo simulations.
>>>>
>>>> Wei Xia has recently asked the same question
>>>> (https://mail.gna.org/public/relax-users/2008-09/msg00000.html).  It
>>>> might be worth reading my reply at
>>>> https://mail.gna.org/public/relax-users/2008-09/msg00002.html.  So
>>>> this feature will be added to relax, but the question is how long will
>>>> that take.  I'd first need the error conversion factor from RMSD of
>>>> base plane noise to peak height, and then add the ability to use the
>>>> RMSD value in relaxation curve fitting.  The first part will be the
>>>> hardest, but you'll need that to do a proper Monte Carlo simulation
>>>> error analysis for the curve fitting.  To do the second part I would
>>>> set up a mini analysis, lets call it a 'system test' because it tests
>>>> the system - relax - to see if the analysis works, and then make this
>>>> system test pass - i.e. implement the feature.
>>>>
>>>> Don't forget that the errors in a complex analysis (e.g model-free and
>>>> reduced spectral density mapping) are just as important as the values
>>>> themselves, if not more.  Getting these wrong will really damage
>>>> optimisation, model selection, and error propagation to the final
>>>> parameters via Monte Carlo simulations.  So both your model-free
>>>> values and errors will be incorrect.
>>>>
>>>> Regards,
>>>>
>>>> Edward
>>>>
>>>>
>>>> On Wed, Oct 8, 2008 at 5:07 PM, Tyler Reddy <[EMAIL PROTECTED]> wrote:
>>>>>
>>>>> Hello,
>>>>>
>>>>> It seems that Relax_fit.py requires replicate data because average and
>>>>> standard
>>>>> deviation values are used downstream in the analysis. With no replicate
>>>>> data
>>>>> (since I don't have any) the output is shown below. Also, commenting out
>>>>> the
>>>>> average and error propagation across multiple spectra
>>>>>
>>>>> #relax_fit.mean_and_error()
>>>>>
>>>>> doesn't work either, and I get another error output that is looking for
>>>>> an
>>>>> averaged value. I'll probably try using a duplicate data set to
>>>>> circumvent this
>>>>> for now (unless this is actually another problem).
>>>>>
>>>>> Tyler
>>>>>
>>>>> Output:
>>>>>
>>>>> relax> relax_fit.mean_and_error()
>>>>>
>>>>> Calculating the average intensity and standard deviation of all spectra.
>>>>>
>>>>> Time point:  0.01 s
>>>>> Number of spectra:  1
>>>>> Standard deviation for time point 0:  0.0
>>>>>
>>>>> Time point:  0.050000000000000003 s
>>>>> Number of spectra:  1
>>>>> Standard deviation for time point 1:  0.0
>>>>>
>>>>> Time point:  0.10000000000000001 s
>>>>> Number of spectra:  1
>>>>> Standard deviation for time point 2:  0.0
>>>>>
>>>>> Time point:  0.20000000000000001 s
>>>>> Number of spectra:  1
>>>>> Standard deviation for time point 3:  0.0
>>>>>
>>>>> Time point:  0.29999999999999999 s
>>>>> Number of spectra:  1
>>>>> Standard deviation for time point 4:  0.0
>>>>>
>>>>> Time point:  0.5 s
>>>>> Number of spectra:  1
>>>>> Standard deviation for time point 5:  0.0
>>>>>
>>>>> Time point:  0.80000000000000004 s
>>>>> Number of spectra:  1
>>>>> Standard deviation for time point 6:  0.0
>>>>> Traceback (most recent call last):
>>>>>  File "/Applications/relax-1.3.1/relax", line 408, in <module>
>>>>>   Relax()
>>>>>  File "/Applications/relax-1.3.1/relax", line 125, in __init__
>>>>>   self.interpreter.run(self.script_file)
>>>>>  File "/Applications/relax-1.3.1/prompt/interpreter.py", line 270, in run
>>>>>   return run_script(intro=self.__intro_string, local=self.local,
>>>>> script_file=script_file, quit=self.__quit_flag,
>>>>> show_script=self.__show_script,
>>>>> raise_relax_error=self.__raise_relax_error)
>>>>>  File "/Applications/relax-1.3.1/prompt/interpreter.py", line 531, in
>>>>> run_script
>>>>>   return console.interact(intro, local, script_file, quit,
>>>>> show_script=show_script, raise_relax_error=raise_relax_error)
>>>>>  File "/Applications/relax-1.3.1/prompt/interpreter.py", line 427, in
>>>>> interact_script
>>>>>   execfile(script_file, local)
>>>>>  File "relax_fit_T1_500Mhz.py", line 45, in <module>
>>>>>   relax_fit.mean_and_error()
>>>>>  File "/Applications/relax-1.3.1/prompt/relax_fit.py", line 96, in
>>>>> mean_and_error
>>>>>   relax_fit_obj.mean_and_error()
>>>>>  File "/Applications/relax-1.3.1/specific_fns/relax_fit.py", line 729, in
>>>>> mean_and_error
>>>>>   sd = sd / float(num_dups)
>>>>> ZeroDivisionError: float division
>>>>>
>>>>>
>>>>> _______________________________________________
>>>>> relax (http://nmr-relax.com)
>>>>>
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>>>>>
>>>>
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>>>
>>>
>>>
>>>
>>
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>
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