I have data at 3 field strengths. Thanks for the references--I had already had
your 2008 papers, but some of the others could be useful. Also good to know I
was using the wrong script!

Tyler




Quoting Edward d'Auvergne <[EMAIL PROTECTED]>:

> On Tue, Oct 21, 2008 at 3:44 AM, Tyler Reddy <[EMAIL PROTECTED]> wrote:
>> Hello,
>>
>> 1) I changed that line and I'm still having a bit of trouble (see output
>> below).
>>
>> 2) The errors that I'm using are described as 'the standard error for each
>> parameter... [which] is an easy calculation from the covariance matrix.'
>> Paraphrasing from the author there--I'm guessing this isn't the optimal
>> input?
>
> These are not completely unreasonable for a simple exponential fit,
> but are not great.  The use of the covariance matrix is known to be
> the dirtiest and roughest technique for parameter errors and requires
> that the optimisation space be quadratic, which is often not the case.
> The space in the immediate vacinity of the minimum is quadratic, but
> further out where the errors are scattered, the space is more
> convoluted and hence the errors aren't very accurate.
>
>
>> 3) I'm not sure it's explicitly stated in the manual, but I'm proceeding on
>> the
>> assumption that you run the multi-model script first and then modsel to
>> decide
>> on the right model for each given residue. A few weeks ago I was
>> experimenting
>> with this and if I didn't leave the global correlation time as fixed the
>> computation seemed to take a VERY long time (unclear if it was ever going to
>> finish).
>
> If you have data at more than one field strength, I would recommend
> the 'full_analysis.py' sample script.  The reasons are given in
> d'Auvergne, E. J. and Gooley, P. R. (2008). Optimisation of NMR
> dynamic models II. (http://www.nmr-relax.com/refs.html).  If not, then
> you'll need to be careful as to what you do here.  The multi-model and
> modsel script are only a small part of the picture.  You need to then
> optimise the diffusion tensor.  These are 3 components of one element
> of the analysis.  You must repeat these until convergence of the
> global model.  Please see figures 6.1, 6.2, and 6.3 of the 1.3.2 or
> 1.2.14 relax manuals for more details.  I can't emphasise enough how
> important applying all of these steps are.  And if you want to avoid
> the problems of artificial motions (d'Auvergne E. J., Gooley P. R.
> (2007). Set theory formulation of the model-free problem and the
> diffusion seeded model-free paradigm. Mol. Biosyst., 3(7), 483-494.
> http://www.nmr-relax.com/refs.html), then I would highly recommend
> data at 2 or more field strengths.
>
> And finally, once convergence of the global model has been reached,
> you can then do Monte Carlo simulations to propagate the errors from
> the relaxation data to the model-free parameters.  This will generate
> the s2_sim, etc. data structures that are missing from the LaTeX table
> generating script.  I'll add checks to this script so that errors are
> not required, but an analysis must have Monte Carlo simulations.
>
> As for the calculation taking a very long time when optimisating the
> global model (model-free parameters of all spins + diffusion tensor),
> that is because this model is absolutely huge, the space is highly
> convoluted, and you are starting a very long way away from the global
> minimum.  And then which model-free models are selected influence this
> model and vice verse.  Again see the 2007 reference for a full
> investigation of this issue.
>
>
>> Also, as a side note, since my peptide is actually in a micelle, I'm not
>> sure if
>> there's anything extra I can do for diffusion tensor and correlation time
>> type
>> stuff. I know some programs (i.e. the Mathematica notebooks by Dr.
>> Spyracopoulos) read in PDB files for diffusion tensor calculations, but I
>> suspect it's a bit of a mess when the system is more complicated than the
>> structure in the PDB file would suggest.
>
> Ah, so you'll have quite a mobile system.  You will have nanosecond
> motions throughout the system on top of the diffusion tensor and the
> fast picosecond internal motions.  I would suggest you look to the
> similar bacteriorhodopsin work of Orekhov, V. Y., Korzhnev, D. M.,
> Diercks, T., Kessler, H., and Arseniev, A. S. (1999). H-1-N-15 NMR
> dynamic study of an isolated alpha-helical peptide
> (1-36)-bacteriorhodopsin reveals the equilibrium helix-coil
> transitions. J. Biomol. NMR, 14(4), 345–356.  The verdict, and I would
> 100% recommend as being 100% essential - you must, must have data at
> more than 1 field strength to study this system!  This system is
> absolutely impossible to study the dynamics of otherwise.  If you
> don't believe me, see also sections 6.4.3, 6.4.4, and all of chapter 5
> of my PhD thesis (http://repository.unimelb.edu.au/10187/2281).
> Chapter 5, which is almost the same as my 2007 Mol. Biosyst. paper,
> will point you to many other references which should hopefully
> demonstrate the absolute must of having multiple field strength data
> for such a highly mobile system.
>
> Regards,
>
> Edward
>
>
>>
>> Output:
>>
>> Latex()
>> ----------------------------------------------------------------------------------------------------
>>
>> relax> pipe.create(pipe_name='results', pipe_type='mf')
>>
>> relax> results.read(file='results', dir=None)
>> Opening the file 'results' for reading.
>> Traceback (most recent call last):
>>  File "/Applications/relax-1.3.1/relax-1.3/relax", line 408, in <module>
>>   Relax()
>>  File "/Applications/relax-1.3.1/relax-1.3/relax", line 125, in __init__
>>   self.interpreter.run(self.script_file)
>>  File "/Applications/relax-1.3.1/relax-1.3/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/relax-1.3/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/relax-1.3/prompt/interpreter.py", line 427,
>> in
>> interact_script
>>   execfile(script_file, local)
>>  File "latex_mf_table.py", line 220, in <module>
>>   Latex()
>>  File "latex_mf_table.py", line 68, in __init__
>>   self.table_body()
>>  File "latex_mf_table.py", line 186, in table_body
>>   self.file.write("%9.3f & %9.3f & " % (spin.s2, spin.s2_err))
>> AttributeError: 'SpinContainer' object has no attribute 's2_err'
>>
>>
>>
>> Quoting Edward d'Auvergne <[EMAIL PROTECTED]>:
>>
>>> Hi,
>>>
>>> Using a new system test, I found one more bug in the script.  This has
>>> been fixed in the 1.3 repository line.  If you haven't used subversion
>>> to check out (and update) the 1.3 line, then you can see the changes
>>> required in my commit at:
>>>
>>> https://mail.gna.org/public/relax-commits/2008-10/msg00402.html
>>>
>>> Just change the line starting with '-' to the line starting with '+'.
>>> Oh, it may take a few minutes for the link to be generated.
>>>
>>> Regards,
>>>
>>> Edward
>>>
>>>
>>> On Mon, Oct 20, 2008 at 10:12 PM, Edward d'Auvergne
>>> <[EMAIL PROTECTED]> wrote:
>>>>
>>>> Hi,
>>>>
>>>> That's a bug in the sample script.  Try adding a ':' character to the
>>>> end of line 171 in your script.  I've fixed this in the 1.3 repository
>>>> line and will try to add a system test to the program to try to catch
>>>> any bugs before you do ;)
>>>>
>>>> Cheers,
>>>>
>>>> Edward
>>>>
>>>>
>>>>
>>>> On Mon, Oct 20, 2008 at 9:27 PM, Tyler Reddy <[EMAIL PROTECTED]> wrote:
>>>>>
>>>>> I've been trying to use the latex python script on the aic results file.
>>>>> I get
>>>>> the syntax error below. Not sure if I'm doing something wrong or if
>>>>> there's
>>>>> just a small problem with that line of code:
>>>>>
>>>>> Latex()
>>>>>
>>>>> ----------------------------------------------------------------------------------------------------
>>>>> Traceback (most recent call last):
>>>>>  File "/Applications/relax-1.3.1/relax-1.3/relax", line 408, in <module>
>>>>>   Relax()
>>>>>  File "/Applications/relax-1.3.1/relax-1.3/relax", line 125, in __init__
>>>>>   self.interpreter.run(self.script_file)
>>>>>  File "/Applications/relax-1.3.1/relax-1.3/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/relax-1.3/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/relax-1.3/prompt/interpreter.py",
>>>>> line 427, in
>>>>> interact_script
>>>>>   execfile(script_file, local)
>>>>>  File "latex_mf_table.py", line 171
>>>>>   for spin, spin_id in spin_loop(return_id=True)
>>>>> SyntaxError: invalid syntax
>>>>>
>>>>>
>>>>>
>>>>>
>>>>>
>>>>>
>>>>>
>>>>>
>>>>>
>>>>>
>>>>> Quoting Edward d'Auvergne <[EMAIL PROTECTED]>:
>>>>>
>>>>>> On Mon, Oct 20, 2008 at 5:12 PM, Tyler Reddy <[EMAIL PROTECTED]> wrote:
>>>>>>>
>>>>>>> Hello,
>>>>>>>
>>>>>>> 1)
>>>>>>>
>>>>>>> I have been using the multi model and model selection scripts in
>>>>>>> relax 1.3.2 but
>>>>>>> I have trouble displaying the output in a tabulated format. Both
>>>>>>> scripts seem
>>>>>>> to produce an xml document with various headers that isn't easy to
>>>>>>> read. It
>>>>>>> looks like format='columnar' isn't supported. I wonder what other
>>>>>>> options I
>>>>>>> have to look at this data? For some reason, I don't recall having
>>>>>>> this problem
>>>>>>> on a Linux machine a few weeks ago (using a Mac OS 10.4 at the
>>>>>>> moment), but
>>>>>>> anyways it would be nice to get readable model-free output.
>>>>>>
>>>>>> The results file is now in XML format and the more readable 'columnar'
>>>>>> format has been removed from the 1.3 line.  With the change to the new
>>>>>> XML results file all the contents of a data pipe, irrespective of what
>>>>>> that data is, is packaged.  So you can put data into this pipe
>>>>>> yourself and it will save that information (for advanced users,
>>>>>> complex python objects will need the to_xml() and from_xml() methods
>>>>>> to package and unpackage the data).  The reason for removing the
>>>>>> 'columnar' format was that it was considered too inflexible for the
>>>>>> changes occuring in the 1.3 line, it contained duplicate information,
>>>>>> had numerical precision issues, and there were alternatives to easily
>>>>>> view this data.  You can use the value.display() and value.write()
>>>>>> user functions to display and save the results for a single parameter.
>>>>>> If needed, these user functions could be extended to accept a list of
>>>>>> parameters.
>>>>>>
>>>>>> Then there is the sample_scripts/latex_mf_table.py sample script which
>>>>>> will generate a LaTeX table of the model-free results.  This file can
>>>>>> be copied and modified - this requires learning a bit of python - to
>>>>>> format and display the results any way you wish.  And finally if
>>>>>> anyone really wants to, and has the skills to, they can modify this
>>>>>> sample script to recreate a version of the 'columnar' format.  This
>>>>>> could be added to the relax sample scripts, and if their skills are
>>>>>> very advanced, then much code from the 1.2 relax versions can be
>>>>>> recycled.
>>>>>>
>>>>>>
>>>>>>> 2)
>>>>>>>
>>>>>>> The error input for the relaxation rate parameters is currently my
>>>>>>> non-linear
>>>>>>> curve fitting standard deviation. I'm not sure if that means
>>>>>>> subsequent
>>>>>>> analysis will be completely incorrect? I guess it depends on the
>>>>>>> comparison of
>>>>>>> magnitude between these errors and the type of error that is
>>>>>>> propagated by
>>>>>>> relax during its own curve-fitting (which I am unable to do at the
>>>>>>> moment).
>>>>>>
>>>>>> I'm guessing this is the sum of squared error value (SSE) from the
>>>>>> fit.  Or is it a regression coefficient or a chi-squared value?  Did
>>>>>> the fitting use a technique such as bootstrapping or jackknife
>>>>>> simulations to estimate the parameter errors via propagation?  Or did
>>>>>> it use the covariance matrix?  If it is the SSE, chi-squared, or
>>>>>> regression coefficient then that value cannot be used.  This will be
>>>>>> wildly wrong and cause massive failure in model selection.  It will
>>>>>> cause big problems in optimisation, and if you are unlucky and have
>>>>>> spaces with long, curved valleys or flat curved spaces leading to the
>>>>>> minimum (that's model-free models m5 to m8 in most cases and not so
>>>>>> uncommon in model m4) then the minimum can be squeezed and appear in
>>>>>> another completely different region in the space.  It will likely also
>>>>>> cause model failure issues, which although removed by the eliminate()
>>>>>> user function, might discount the best solution.  I would guess that
>>>>>> all of this will have a measurable affect on the final diffusion
>>>>>> tensor as well and, if so, this will cause the appearance of
>>>>>> artificial motions (my 2007 JBNMR paper at
>>>>>> http://dx.doi.org/10.1039/b702202f explains these problems in detail).
>>>>>> If one is not careful with the errors and they are significantly off,
>>>>>> then the result is that the results may not be real.  So I would only
>>>>>> use the error if it comes from an established error propagation
>>>>>> technique (i.e. from data to parameter error propagation).
>>>>>>
>>>>>> Regards,
>>>>>>
>>>>>> Edward
>>>>>>
>>>>>
>>>>>
>>>>>
>>>>>
>>>>> _______________________________________________
>>>>> relax (http://nmr-relax.com)
>>>>>
>>>>> This is the relax-users mailing list
>>>>> relax-users@gna.org
>>>>>
>>>>> To unsubscribe from this list, get a password
>>>>> reminder, or change your subscription options,
>>>>> visit the list information page at
>>>>> https://mail.gna.org/listinfo/relax-users
>>>>>
>>>>
>>>
>>
>>
>>
>>
>




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