[ccp4bb] problems with ccp4-6.4.0 occurrences in ccp4-6.5
Hello,
I just installed ccp4-6.5
I get an error at run time (relating to $PATH I suppose, see below) that
still contains occurrences of ccp4-6.4.0 even though the line that was
supposed to get rid of these was made active in ccp4.setup-csh
# To remove previously added CCP4 directories from the PATH, uncomment:
if $?CCP4 setenv PATH `echo $PATH | sed s,${CCP4}[^:]*:,,g`
The previous distribution of ccp4 (6.4.0) was removed during the 6.5
installation step. I get this for example when launching ccp4i:
Error in startup script: couldn't read file
/home/prog/ccp4-6.4.0/share/dbccp4i/ClientAPI/dbClientAPI.tcl: no such
file or directory
while executing
source [FileJoin [GetEnvPath DBCCP4I_TOP] ClientAPI dbClientAPI.tcl]
(file /home/prog/ccp4-6.5/share/ccp4i/src/projectdirs.tcl line 23)
invoked from within
source [SearchPath TOP src projectdirs.tcl]
(file /home/prog/ccp4-6.5/share/ccp4i/src/system.tcl line 3379)
invoked from within
source [file join $env(CCP4I_TOP) src system.tcl]
(file /home/prog/ccp4-6.5/share/ccp4i/bin/ccp4i.tcl line 79)
invoked from within
source [file join $env(CCP4I_TOP) bin ccp4i.tcl]
(file /home/prog/ccp4-6.5/bin/ccp4i line 12)
and echo $PATH contains the following entry that shouldn't be there:
/home/prog/ccp4-6.4.0/share/xia2/Applications
Would anyone know how to deal with this ?
Thank you in advance,
Fred.
--
Fred. Vellieux (B.Sc., Ph.D., hdr)
IBS / ELMA
Campus EPN
71 avenue des Martyrs
CS 10090
F-38044 Grenoble Cedex 9
Tel: +33 457428605
Fax: +33 476501890
[ccp4bb] SHELX for Macromolecules Course
Immediately after the DGK Meeting in Goettingen, there will be an IRTG Methods Course on Macromolecular Applications of SHELX there on the afternoon of Thursday March 19th. See: http://shelx.uni-ac.gwdg.de/SHELX/workshops.php for details. George -- Prof. George M. Sheldrick FRS Dept. Structural Chemistry, University of Goettingen, Tammannstr. 4, D37077 Goettingen, Germany Tel. +49-551-39-33021 or -33068 Fax. +49-551-39-22582
Re: [ccp4bb] Continuous-Single Versus Coarse-Multiple Sampling
No wikipedia link yet? JPK -Original Message- From: CCP4 bulletin board [mailto:CCP4BB@JISCMAIL.AC.UK] On Behalf Of Keller, Jacob Sent: Thursday, January 22, 2015 5:20 PM To: CCP4BB@JISCMAIL.AC.UK Subject: [ccp4bb] Continuous-Single Versus Coarse-Multiple Sampling Dear Crystallographers, This is more general than crystallography, but has applications therein, particularly in understanding fine phi-slicing. The general question is: Given one needs to collect data to fit parameters for a known function, and given a limited total number of measurements, is it generally better to measure a small group of points multiple times or to distribute each individual measurement over the measureable extent of the function? I have a strong intuition that it is the latter, but all errors being equal, it would seem prima facie that both are equivalent. For example, a line (y = mx + b) can be fit from two points. One could either measure the line at two points A and B five times each for a total of 10 independent measurements, or measure ten points evenly-spaced from A to B. Are these equivalent in terms of fitting and information content or not? Which is better? Again, conjecture and intuition suggest the evenly-spaced experiment is better, but I cannot formulate or prove to myself why, yet. The application of this to crystallography might be another reason that fine phi-slicing (0.1 degrees * 3600 frames) is better than coarse (1 degree * 3600 frames), even though the number of times one measures reflections is tenfold higher in the second case (assuming no radiation damage). In the first case, one never measures the same phi angle twice, but one does have multiple measurements in a sense, i.e., of different parts of the same reflection. Yes, 3D profile-fitting may be a big reason fine phi-slicing works, but beyond that, perhaps this sampling choice plays a role as well. Or maybe the profile-fitting works so well precisely because of this diffuse-single type of sampling rather than coarse-multiple sampling? This general math/science concept must have been discussed somewhere--can anyone point to where? JPK *** Jacob Pearson Keller, PhD Looger Lab/HHMI Janelia Research Campus 19700 Helix Dr, Ashburn, VA 20147 email: kell...@janelia.hhmi.org ***
Re: [ccp4bb] problems with ccp4-6.4.0 occurrences in ccp4-6.5
Hi Fred,
I had about the same problem that disappeared when I logged out and in
again - just a new terminal was no help. Does that help in your case,
too? Maybe there is an environment variable that gets appended by the
setup script.
Best,
Tim
On 01/23/2015 06:07 PM, vellieux wrote:
Hello,
I just installed ccp4-6.5
I get an error at run time (relating to $PATH I suppose, see below) that
still contains occurrences of ccp4-6.4.0 even though the line that was
supposed to get rid of these was made active in ccp4.setup-csh
# To remove previously added CCP4 directories from the PATH, uncomment:
if $?CCP4 setenv PATH `echo $PATH | sed s,${CCP4}[^:]*:,,g`
The previous distribution of ccp4 (6.4.0) was removed during the 6.5
installation step. I get this for example when launching ccp4i:
Error in startup script: couldn't read file
/home/prog/ccp4-6.4.0/share/dbccp4i/ClientAPI/dbClientAPI.tcl: no such
file or directory
while executing
source [FileJoin [GetEnvPath DBCCP4I_TOP] ClientAPI dbClientAPI.tcl]
(file /home/prog/ccp4-6.5/share/ccp4i/src/projectdirs.tcl line 23)
invoked from within
source [SearchPath TOP src projectdirs.tcl]
(file /home/prog/ccp4-6.5/share/ccp4i/src/system.tcl line 3379)
invoked from within
source [file join $env(CCP4I_TOP) src system.tcl]
(file /home/prog/ccp4-6.5/share/ccp4i/bin/ccp4i.tcl line 79)
invoked from within
source [file join $env(CCP4I_TOP) bin ccp4i.tcl]
(file /home/prog/ccp4-6.5/bin/ccp4i line 12)
and echo $PATH contains the following entry that shouldn't be there:
/home/prog/ccp4-6.4.0/share/xia2/Applications
Would anyone know how to deal with this ?
Thank you in advance,
Fred.
--
Dr Tim Gruene
Institut fuer anorganische Chemie
Tammannstr. 4
D-37077 Goettingen
GPG Key ID = A46BEE1A
signature.asc
Description: OpenPGP digital signature
Re: [ccp4bb] Crystallography Workshop in South America - CCP4 / Institut Pasteur de Montevideo 2015
Dear all, nasty auto-corrector”-driven mistake affecting Kay Diederichs’ name! My apologies! Sorry for the duplication…now duly written below (+ extra advertisement as well! ;) ) best wishes Alejandro On Jan 23, 2015, at 20:42, Alejandro Buschiazzo ale...@pasteur.edu.uy wrote: Dear colleagues, We are pleased to remind you about the Workshop: Macromolecular Crystallography School From data processing to structure refinement and beyond, to be held at the Institut Pasteur de Montevideo (Uruguay). Dates: April 6 - 16, 2015 Invited speakers and tutors: Alejandro Buschiazzo, Montevideo, Uruguay Kay Diederichs, Konstanz, Germany Paul Emsley, Cambridge, UK Richard Garrat, São Carlos, Brazil Ronan Keegan, Oxford, UK Eugene Krissinel, Oxford, UK Victor Lamzin, Hamburg, Germany Andrey Lebedev, Oxford, UK Andrew Leslie, Cambridge, UK Garib Murshudov, Cambridge, UK Rob Nicholls, Cambridge, UK Randy Read, Cambridge, UK William Shepard, Paris, France Pavol Skubak, Leiden, the Netherlands Clemens Vonrhein, Cambridge, UK This edition will count with an optional introductory day. A Scientific Satellite Symposium will take place during the course. Sponsored by the Insttitut Pasteur and the Institut Pasteur International Network, this symposium will gather top research scientists from the Pasteur Network, who will discuss about Structural Biology in the study of infectious diseases: Pedro Alzari and Michael Nilges (Inst Pasteur, Paris), Beatriz Guimaraes (Fiocruz, Parana) and Joo Hwan No (Inst Pasteur, Korea), together with several scientists from Inst Pasteur Montevideo. Please find the program of the Workshop and Satellite Symposium, the application form and further contact information, at www.pasteur.edu.uy/mx2015 http://www.pasteur.edu.uy/mx2015 The site will be updated regularly, stay tuned. We acknowledge the support from the Reseau International des Instituts Pasteur (RIIP); the Collaborative Computational Project Nº4 (CCP4, UK) Science and Technology Facilities Council (UK); the International Union of Crystallography (IUCr); and the Institut Pasteur de Montevideo. Applicants: 24 students will be selected, aiming at advanced PhD, postdocs and young researchers. The Course will provide financial support covering registration fees, and for the case of those students coming from abroad, all local expenses (lodging, per diem and local transportation). Look in the www site http://www.pasteur.edu.uy/mx2015 for details on application procedures. The application deadline is February 16, 2015. The results will be announced by March 6. Please address further inquiries to: mx2...@pasteur.edu.uy mailto:mx2...@pasteur.edu.uy Organizers: Alejandro Buschiazzo, PhD. Institut Pasteur de Montevideo, Uruguay Ronan Keegan, PhD. CCP4, STFC Rutherford Appleton Laboratory, United Kingdom We look forward to welcoming you soon in Montevideo! -- Alejandro Buschiazzo, PhD Research Scientist Unit of Protein Crystallography Institut Pasteur de Montevideo Mataojo 2020 Montevideo 11400 URUGUAY Phone: +598 25220910 int. 120 Fax: +598 25224185 http://www.pasteur.edu.uy/pxf http://www.pasteur.edu.uy/pxf
Re: [ccp4bb] Continuous-Single Versus Coarse-Multiple Sampling
On Friday, 23 January, 2015 20:36:08 Keller, Jacob wrote: No wikipedia link yet? In practice the issue usually comes down to a consideration of the noise. Is the noise systematic? Is the signal/noise constant over time? If the noise is systematic, then repeated measurement of the same data points will be biased by that systematic factor and will overestimate the accuracy of the data. This is an example of when precision is distinct from accuracy. On the other hand this protocol may allow you to better estimate and correct for a decrease in signal/noise as a function of time. Conversely spreading the measurement effort over a larger number of points may result in a larger apparent sigma (lower precision) but greater accuracy overall since the systematic effects are more likely to be correctly identified as noise. Relating this back to fine-slicing on phi, if the noise has a large per-image component then fine-slicing is a bad idea because you increase the noise for no gain in signal. On the other hand if there is little or no per-image noise component, as is the case for photon counting detectors, then fine-slicing potentially decreases the noise because you do not have to estimate and subtract the background from the portion of the time the reflection of interest does not intersect the Ewald sphere. Ethan JPK -Original Message- From: CCP4 bulletin board [mailto:CCP4BB@JISCMAIL.AC.UK] On Behalf Of Keller, Jacob Sent: Thursday, January 22, 2015 5:20 PM To: CCP4BB@JISCMAIL.AC.UK Subject: [ccp4bb] Continuous-Single Versus Coarse-Multiple Sampling Dear Crystallographers, This is more general than crystallography, but has applications therein, particularly in understanding fine phi-slicing. The general question is: Given one needs to collect data to fit parameters for a known function, and given a limited total number of measurements, is it generally better to measure a small group of points multiple times or to distribute each individual measurement over the measureable extent of the function? I have a strong intuition that it is the latter, but all errors being equal, it would seem prima facie that both are equivalent. For example, a line (y = mx + b) can be fit from two points. One could either measure the line at two points A and B five times each for a total of 10 independent measurements, or measure ten points evenly-spaced from A to B. Are these equivalent in terms of fitting and information content or not? Which is better? Again, conjecture and intuition suggest the evenly-spaced experiment is better, but I cannot formulate or prove to myself why, yet. The application of this to crystallography might be another reason that fine phi-slicing (0.1 degrees * 3600 frames) is better than coarse (1 degree * 3600 frames), even though the number of times one measures reflections is tenfold higher in the second case (assuming no radiation damage). In the first case, one never measures the same phi angle twice, but one does have multiple measurements in a sense, i.e., of different parts of the same reflection. Yes, 3D profile-fitting may be a big reason fine phi-slicing works, but beyond that, perhaps this sampling choice plays a role as well. Or maybe the profile-fitting works so well precisely because of this diffuse-single type of sampling rather than coarse-multiple sampling? This general math/science concept must have been discussed somewhere--can anyone point to where? JPK *** Jacob Pearson Keller, PhD Looger Lab/HHMI Janelia Research Campus 19700 Helix Dr, Ashburn, VA 20147 email: kell...@janelia.hhmi.org *** -- Ethan A Merritt Biomolecular Structure Center, K-428 Health Sciences Bldg MS 357742, University of Washington, Seattle 98195-7742
Re: [ccp4bb] Continuous-Single Versus Coarse-Multiple Sampling
Hi Jacob,
My intuition for the line fit case was exactly the opposite to yours. My
reasoning is a sort of physical one. If you imagine the line as a stiff rod
with hooks for masses evenly spread along its length at 10 positions, then
the object where you put 5 masses at positions 1 and 10 has a greater
moment of inertia than the case where there is one mass at each position.
This tells me that changes to the masses in the further spread case would
be more effective (faster) at changing the orientation of the rod. Then
it's a bit of leap I admit, but I felt that measurements of a line's height
made in such a way would be more effective at determining the fit
parameters than the evenly spread case.
But I decided not to rely on intuition when I could simulate it. At the
bottom of the message is a script in the R language that does 2 line
fits of the function y = m*x + c, where c = 100, m = 1 and x is the
sequence 1..10 for the first 1 fits and (1, 1, 1, 1, 1, 10, 10, 10, 10,
10) for the rest of them. The data being fit to are 'measurements' taken by
adding a standard normal deviate to x + 100 at each position.
After running all these simulations (it takes a few seconds) the script
then calculates the mean and standard deviations of the fit parameters, m
and c. The standard deviations are interesting:
mean intercept of fit1: 99.99619
sd of intercept of fit1 0.6833687
mean intercept of fit2: 99.99909
sd of intercept of fit2 0.498759
mean gradient of fit1: 1.00076
sd of gradient of fit1 0.1100296
mean gradient of fit2: 0.9996967
sd of gradient of fit2 0.07021113
Fit 2 has a tighter distribution for both the intercept and the gradient.
It is therefore the more precise way of fitting the line, and this was the
'heavy-ended' case.
Script follows:
line_fit - function(x_seq)
{
y_seq - 100 + x_seq + rnorm(length(x_seq))
return(coef(lm(y_seq~x_seq)))
}
even_spaced_x - seq(1,10)
heavy_ended_x - c(rep(1,5), rep(10,5))
fit1 - replicate(1, line_fit(even_spaced_x))
fit2 - replicate(1, line_fit(heavy_ended_x))
cat(mean intercept of fit1:, mean(fit1[1,]), \n)
cat(sd of intercept of fit1, sd(fit1[1,]), \n\n)
cat(mean intercept of fit2:, mean(fit2[1,]), \n)
cat(sd of intercept of fit2, sd(fit2[1,]), \n\n)
cat(mean gradient of fit1:, mean(fit1[2,]),\n)
cat(sd of gradient of fit1, sd(fit1[2,]), \n\n)
cat(mean gradient of fit2:, mean(fit2[2,]), \n)
cat(sd of gradient of fit2, sd(fit2[2,]), \n\n)
Cheers
-- David
On 22 January 2015 at 22:20, Keller, Jacob kell...@janelia.hhmi.org wrote:
Dear Crystallographers,
This is more general than crystallography, but has applications therein,
particularly in understanding fine phi-slicing.
The general question is:
Given one needs to collect data to fit parameters for a known function,
and given a limited total number of measurements, is it generally better to
measure a small group of points multiple times or to distribute each
individual measurement over the measureable extent of the function? I have
a strong intuition that it is the latter, but all errors being equal, it
would seem prima facie that both are equivalent. For example, a line (y =
mx + b) can be fit from two points. One could either measure the line at
two points A and B five times each for a total of 10 independent
measurements, or measure ten points evenly-spaced from A to B. Are these
equivalent in terms of fitting and information content or not? Which is
better? Again, conjecture and intuition suggest the evenly-spaced
experiment is better, but I cannot formulate or prove to myself why, yet.
The application of this to crystallography might be another reason that
fine phi-slicing (0.1 degrees * 3600 frames) is better than coarse (1
degree * 3600 frames), even though the number of times one measures
reflections is tenfold higher in the second case (assuming no radiation
damage). In the first case, one never measures the same phi angle twice,
but one does have multiple measurements in a sense, i.e., of different
parts of the same reflection.
Yes, 3D profile-fitting may be a big reason fine phi-slicing works, but
beyond that, perhaps this sampling choice plays a role as well. Or maybe
the profile-fitting works so well precisely because of this diffuse-single
type of sampling rather than coarse-multiple sampling?
This general math/science concept must have been discussed somewhere--can
anyone point to where?
JPK
***
Jacob Pearson Keller, PhD
Looger Lab/HHMI Janelia Research Campus
19700 Helix Dr, Ashburn, VA 20147
email: kell...@janelia.hhmi.org
***
[ccp4bb] Crystallography Workshop in South America - CCP4 / Institut Pasteur de Montevideo 2015
Dear colleagues, We are pleased to remind you about the Workshop: Macromolecular Crystallography School From data processing to structure refinement and beyond, to be held at the Institut Pasteur de Montevideo (Uruguay). Dates: April 6 - 16, 2015 Invited speakers and tutors: Alejandro Buschiazzo, Montevideo, Uruguay Kay Dietrichs, Konstanz, Germany Paul Emsley, Cambridge, UK Richard Garrat, São Carlos, Brazil Ronan Keegan, Oxford, UK Eugene Krissinel, Oxford, UK Victor Lamzin, Hamburg, Germany Andrey Lebedev, Oxford, UK Andrew Leslie, Cambridge, UK Garib Murshudov, Cambridge, UK Rob Nicholls, Cambridge, UK Randy Read, Cambridge, UK William Shepard, Paris, France Pavol Skubak, Leiden, the Netherlands Clemens Vonrhein, Cambridge, UK This edition will count with an optional introductory day. A Scientific Satellite Symposium will take place during the course. Sponsored by the Insttitut Pasteur and the Institut Pasteur International Network, this symposium will gather top research scientists from the Pasteur Network, who will discuss about Structural Biology in the study of infectious diseases: Pedro Alzari and Michael Nilges (Inst Pasteur, Paris), Beatriz Guimaraes (Fiocruz, Parana) and Joo Hwan No (Inst Pasteur, Korea), together with several scientists from Inst Pasteur Montevideo. Please find the program of the Workshop and Satellite Symposium, the application form and further contact information, at www.pasteur.edu.uy/mx2015 http://www.pasteur.edu.uy/mx2015 The site will be updated regularly, stay tuned. We acknowledge the support from the Reseau International des Instituts Pasteur (RIIP); the Collaborative Computational Project Nº4 (CCP4, UK) Science and Technology Facilities Council (UK); the International Union of Crystallography (IUCr); and the Institut Pasteur de Montevideo. Applicants: 24 students will be selected, aiming at advanced PhD, postdocs and young researchers. The Course will provide financial support covering registration fees, and for the case of those students coming from abroad, all local expenses (lodging, per diem and local transportation). Look in the www site http://www.pasteur.edu.uy/mx2015 for details on application procedures. The application deadline is February 16, 2015. The results will be announced by March 6. Please address further inquiries to: mx2...@pasteur.edu.uy mailto:mx2...@pasteur.edu.uy Organizers: Alejandro Buschiazzo, PhD. Institut Pasteur de Montevideo, Uruguay Ronan Keegan, PhD. CCP4, STFC Rutherford Appleton Laboratory, United Kingdom We look forward to welcoming you soon in Montevideo! -- Alejandro Buschiazzo, PhD Research Scientist Unit of Protein Crystallography Institut Pasteur de Montevideo Mataojo 2020 Montevideo 11400 URUGUAY Phone: +598 25220910 int. 120 Fax: +598 25224185 http://www.pasteur.edu.uy/pxf
[ccp4bb] BALBES exits after searching the internal database
Hi all Im trying to use BALBES locally to perofrm MR. I have given mtz file and sequence file as input. Upon successful completion of program it is giving an message #---# # Search for Structures with Similar Cell and Space Group # #---# No structure of similar cell and space group was found #---# # Model Database Analysis # #---# number of amino acids in the input sequence file is 377 null BALBES exits after searching the internal database #CCP4I TERMINATION STATUS 1 #CCP4I TERMINATION TIME 23 Jan 2015 16:46:18 #CCP4I TERMINATION OUTPUT_FILES /home/user1/projects/pramod/fmt_all/ccp4/167_balbes/167_balbes_MR_SEARCH_MOD.pdb /home/user1/projects/pramod/fmt_all/ccp4 /home/user1/projects/pramod/fmt_all/ccp4/167_balbes #CCP4I MESSAGE Task completed successfully help?? -- Thanks Regards, Pooja Kesari Indian Institute of Technology Roorkee INDIA
Re: [ccp4bb] Continuous-Single Versus Coarse-Multiple Sampling
Hi Jacob, It seems reasonable for your straight line case that the two would be equivalent. I would guess though that as the function to be fitted against becomes more complex (e.g. a rectangular hyperbola in enzyme kinetics) it would be advantageous to have more points of the independent variable measured a fewer number of times (assuming you measured each one enough to get a reasonable estimate of the experimental error). Another reason I can think of to measure more points less frequently is so you can detect possible deviations in the data from the expected function (there might be a peak in the middle of your straight line for some reason). Looking forward to reading other responses! Philip On Thu, Jan 22, 2015 at 5:20 PM, Keller, Jacob kell...@janelia.hhmi.org wrote: Dear Crystallographers, This is more general than crystallography, but has applications therein, particularly in understanding fine phi-slicing. The general question is: Given one needs to collect data to fit parameters for a known function, and given a limited total number of measurements, is it generally better to measure a small group of points multiple times or to distribute each individual measurement over the measureable extent of the function? I have a strong intuition that it is the latter, but all errors being equal, it would seem prima facie that both are equivalent. For example, a line (y = mx + b) can be fit from two points. One could either measure the line at two points A and B five times each for a total of 10 independent measurements, or measure ten points evenly-spaced from A to B. Are these equivalent in terms of fitting and information content or not? Which is better? Again, conjecture and intuition suggest the evenly-spaced experiment is better, but I cannot formulate or prove to myself why, yet. The application of this to crystallography might be another reason that fine phi-slicing (0.1 degrees * 3600 frames) is better than coarse (1 degree * 3600 frames), even though the number of times one measures reflections is tenfold higher in the second case (assuming no radiation damage). In the first case, one never measures the same phi angle twice, but one does have multiple measurements in a sense, i.e., of different parts of the same reflection. Yes, 3D profile-fitting may be a big reason fine phi-slicing works, but beyond that, perhaps this sampling choice plays a role as well. Or maybe the profile-fitting works so well precisely because of this diffuse-single type of sampling rather than coarse-multiple sampling? This general math/science concept must have been discussed somewhere--can anyone point to where? JPK *** Jacob Pearson Keller, PhD Looger Lab/HHMI Janelia Research Campus 19700 Helix Dr, Ashburn, VA 20147 email: kell...@janelia.hhmi.org ***
Re: [ccp4bb] Continuous-Single Versus Coarse-Multiple Sampling
Dear Jacob, There are a multitude of directions you can go from here - a few comments spring to mind: - are repeated observations of the same reflection on the same part of the detector really independent? - for the wide phi sliced vs. fine sliced discussion the detector type matters a great deal - a CCD has one set of properties, a PAD another - are we limited to megabytes? why not do both? i.e. 36,000 0.1 degree images? or if time limited are 360 1 degree images good enough?! - if you have a kappa goniostat are you better off re-orientating the sample between scans (so you are not repeating measurements in your graph fitting analogy) but you are getting [more] independent measurements or keeping the sample orientation the same so you are sampling the source signal (incoming X-ray beam) better? former probably allows better scaling, latter allows clearer radiation damage analysis - if you do have radiation damage (which clearly we do, even if it is radiation induced small changes) then which strategy would best allow you to go back retrospectively truncate your data set? your 10-spin approach wins out here... A really interesting question comes from your comment about the information content of the data - really what information is in there - are we talking about the absolute amount of information or just the amount of information we currently extract use? Profile fitting wise the ideal should (in principle) be to have a very small number of events on every image (exactly one?) from which you could recover the perfect time series of events have a relatively exact orientation for every one, and from this know or be able to assign whether each event comes from background or signal or signal from protein signal from solvent signal from air from a different point of view (or more likely probability that event E has class S). Only problem with this is that it does not work (yet!) From a practical point of view, I tend to like taking weak data many times from crystals when using a pixel array detector as the overhead / cost is small the option to revisit the data retrospectively stop collecting data is there. This is expensive in MB but these are cheap: given the choices above I would tend to select 10 x 3600 x 0.1 degree [not one of your two options I acknowledge] ;o) but that is just gut instinct. There are radiation damage arguments for doing the exact opposite too... Your final question, on the general problem - I suspect that statistically it has been well treated, but the fact that we record a convolution of reciprocal space with lots of other stuff (background, readout noise, source signal, ...) may make mapping MX data collection to this treatment a study in it's own right. I look forward to reading the rest of this thread! Best wishes Graeme On Thu Jan 22 2015 at 10:20:21 PM Keller, Jacob kell...@janelia.hhmi.org wrote: Dear Crystallographers, This is more general than crystallography, but has applications therein, particularly in understanding fine phi-slicing. The general question is: Given one needs to collect data to fit parameters for a known function, and given a limited total number of measurements, is it generally better to measure a small group of points multiple times or to distribute each individual measurement over the measureable extent of the function? I have a strong intuition that it is the latter, but all errors being equal, it would seem prima facie that both are equivalent. For example, a line (y = mx + b) can be fit from two points. One could either measure the line at two points A and B five times each for a total of 10 independent measurements, or measure ten points evenly-spaced from A to B. Are these equivalent in terms of fitting and information content or not? Which is better? Again, conjecture and intuition suggest the evenly-spaced experiment is better, but I cannot formulate or prove to myself why, yet. The application of this to crystallography might be another reason that fine phi-slicing (0.1 degrees * 3600 frames) is better than coarse (1 degree * 3600 frames), even though the number of times one measures reflections is tenfold higher in the second case (assuming no radiation damage). In the first case, one never measures the same phi angle twice, but one does have multiple measurements in a sense, i.e., of different parts of the same reflection. Yes, 3D profile-fitting may be a big reason fine phi-slicing works, but beyond that, perhaps this sampling choice plays a role as well. Or maybe the profile-fitting works so well precisely because of this diffuse-single type of sampling rather than coarse-multiple sampling? This general math/science concept must have been discussed somewhere--can anyone point to where? JPK *** Jacob Pearson Keller, PhD Looger Lab/HHMI Janelia Research Campus 19700 Helix Dr, Ashburn, VA 20147 email: kell...@janelia.hhmi.org
[ccp4bb] Announcement: Second International Summer School of Crystallography 2015, Hamburg, 7. - 13. June 2015
Second International Summer School of Crystallography 2015, Hamburg, 7. - 13. June 2015 (Application open - deadline 15th of March) Dear ccp4bb, We are pleased to announce the second International Summer School of Crystallography at the Center for Free-Electron Laser Science at DESY, Hamburg (D). Prof. Carmelo Giacovazzo will lecture on the basics of crystallography, covering mathematical understanding of crystallographic point and space groups, diffraction experiments, structure factor calculations, systematic absences, determination of space groups , background of phasing for structure determination of biomolecules and many additional topics. Participants will also learn modern applications and instrumentation of protein crystallography experiments at advanced light sources, such as 3rd generation synchrotron and XFELs. Speakers: Prof. Carmelo Giacovazzo (University of Bari), Prof. Henry Chapman (CFEL / DESY, University of Hamburg), Prof. Arwen Pearson (CUI, University of Hamburg), Dr. Thomas Schneider (EMBL), Dr. Gleb Bourenkov (EMBL), Dr. Adrian Mancuso (European X-FEL), Dr. Thomas White (CFEL / DESY) The summer school program is geared for PhD students working in the field of crystallography, but exceptions for motivated PostDocs and MSc students can be made. The course will mostly cover mathematical background of crystallography, hence we are looking for students, having a (bio)physics background. This will NOT be a workshop covering protein crystallographic programs but rather will be theory oriented. Besides the lessons there will be guided tours of PETRAIII/European XFEL, a BBQ and a harbor boat trip scheduled. Accepted applicants will be asked to pay a registration fee of approx. 100 EUR (includes coffee breaks and lunch). In addition, participants will have to pay for their own travel expenses, accommodation will cost 70 EUR at the DESY Guest House (the rest will be covered by the school budget). The application deadline is on the 15th of March, 2015. Notification of accepted applicants will be sent end of March. Places and accommodation are limited to 30 students in total. The application is as simple as follows: - Applicants must provide a motivation letter, as well as, a CV, directly to the organizer Cornelius Gati (cornelius.g...@desy.de). For further information about the school, please visit: http://conferences.cfel.de/issc15 We look forward to welcoming you in Hamburg! With kind regards Cornelius Gati -- Dr. Dominik Oberthür CFEL - Center for Free-Electron Laser Science Coherent Imaging Division Notkestrasse 85 22607 Hamburg Germany phone: +49 (0)40 8998 6394 dominik.oberth...@cfel.de
