Re: [ccp4bb] Some questions on tools for CCP4i2cloud: pdbset, pdbcur, coordconv, sftools

2021-08-31 Thread Dirk Kostrewa

Dear Robbie,

I use pdbset in scripts from time to time, mainly to generate symmetry 
equivalent copies. I use sftools on the command line more frequently, 
because it allows a lot of mathematical operations on data in mtz files. 
I also use sftools to produce lists of average data values against 
resolution (that I plot then with gnuplot). I can't recall having used 
coordconv at all.


Best regards,

Dirk.

On 8/26/21 12:29 PM, Robbie Joosten wrote:

Dear CCP4 users,

We (as in, the CCP4 developers) are investigating some (potentially) missing 
functionality in CCP4i2 and/or Cloud with respect to the programs pdbset, 
pdbcur, coordconv, and sftools. Some of these tools are quite old and may need 
to be replaced by other tools with similar functionality. Could you answer a 
few questions:

- Do you use any of these tools?
- If so, how often? (Few times a week, month, year, or less than once a year).
- Which functionality of program X do you use?
- Would you like a graphical interface to that functionality or are you happy 
to use the command line?

Personal example:
I use pdbset a few times a month, but only the "noise" function. I don't need a graphical 
interface for it (because it is used in the context of pdb-redo). I also use sftools, "reduce 
-> merge average" a few times a year. Again, only from the command line.


Feel free to send your answers directly to me or to the bulletin board if you 
want to start a discussion. Tips on alternative CCP4 tools to achieve similar 
effects are probably also interesting for other BB users.

Cheers,
Robbie


  




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Re: [ccp4bb] AW: [ccp4bb] Antwort: Re: [ccp4bb] chain on 2-fold axis?

2021-08-27 Thread Dirk Kostrewa

Dear Jeffrey,

just using thin shells of reflections for the test set might not be 
enough to eliminate any correlation to working set reflections. The 
distance of the test set reflections in reciprocal space, after applying 
the NCS rotations in reciprocal space, to any reflections of the working 
set should be large enough to be uncorrelated. A typical maximum 
distance for correlation in reciprocal space is the first zero (root) of 
the Fourier transform of the approximated spherical shape of the protein 
molecule, the so-called G-function (see [1) and [2]). However, this 
means, that shells should be thicker than 2 times this distance to 
blindly exclude any potential correlation between test set and working 
set reflection in reciprocal space. This would be way too expensive!


An better way to select uncorrelated reflections is described in [3] 
(same reference that Kay has given), where for each test set reflection, 
after applying the NCS rotations in reciprocal space, the distances to 
the working set reflections are taken into account, and test and working 
set reflections are chosen such that their distances are large enough to 
be uncorrelated.


Best regards,

Dirk.

[1] Rossmann & Blow, Acta Cryst, 15, 24 -31 (1962)

[2] Main & Rossmann, Acta Cryst, 21, 67-72 (1966)

[3] Fabiola, Korostelev & Chapman, Acta Cryst, D62, 227-238 (2006)

On 8/27/21 4:47 PM, Kay Diederichs wrote:

Hi Jeffrey,

good question. Both twinning and NCS may couple reflections across free and 
working sets, and this should be avoided by proper selection - otherwise Rfree 
is biased towards Rwork. Selecting thin shells should be a good option, and can 
be done in SFTOOLS (or DATAMAN, or SHELXPRO).

How much does it matter? Actually I started to search the literature after 
reading your question, and expected that one of Z. Dauter's papers would 
enlighten me, but until a minute ago couldn't find the one(s) that I thought 
existed. But I found Fabiola et al., Acta Cryst. (2006). D62, 227–238 which is 
relevant for the coupling by NCS. Ah I just found Smietanska et al., Acta 
Cryst. (2020). D76, 653-667 where they indeed selected thin shells.

Best wishes,
Kay

On Fri, 27 Aug 2021 13:24:05 +, Jeffrey B Bonanno 
 wrote:


Hi Kay,

Can you also comment on Rfree set selection? It seems thin shell might be 
preferred in these cases?

jbb

Jeffrey B. Bonanno, Ph.D.
Department of Biochemistry
Albert Einstein College of Medicine
1300 Morris Park Avenue
Bronx, NY 10461
off. 718-430-2452 fax. 718-430-8565
email jeffrey.bona...@einsteinmed.org



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D-81377 Munich
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Phone:  +49-89-2180-76845
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Re: [ccp4bb] Omit maps in phenix and ccp4

2021-04-07 Thread Dirk Kostrewa

Dear Eleanor,

setting occupancies of omitted atoms to zero has the danger of leaving a 
hole with the shape of these atoms in the bulk solvent mask, leading to 
positive difference density just because of the missing bulk solvent 
density. Since the days of X-PLOR, I always removed the omitted atoms. I 
never tried this with REFMAC5, though.


Cheers,

Dirk.

On 07.04.21 11:46, Eleanor Dodson wrote:
Well - I use COOT for this sort of task, and dont trust the automated 
tools.

my procedure is
load COOT - probably after a refinement cycle
set occupancy of ligand(s) to 0.00 ( Measures - residue information - 
change occupancy)
Look at the environment critically . eg if an ARG or other bulky side 
chain nearby , or waters etc selectively set occupancies to 0.00


Doo some more cycles of refinement with this coordinate set to remove 
any memory of the ligand.


Look at the map - if the ligand and other zero occ atoms is still in 
the right place reinstate them, or try to reinterpret density..

Eleanor



On Wed, 7 Apr 2021 at 08:39, Bjarte Aarmo Lund <mailto:bjarte.l...@uit.no>> wrote:


Dear Hari,

With regards to 1) Is 15 the number of atoms in your molecule? Or
is it the number of hydrogens? The CIF file may have the wrong
residue name or lack the hydrogens depending on how you built the
ligand-protein complex.

There is also a phenixbb for phenix questions,
http://www.phenix-online.org/mailman/listinfo/phenixbb
<http://www.phenix-online.org/mailman/listinfo/phenixbb>

Kind regards,

Bjarte Aarmo Lund

Postdoc

UiT The Arctic University of Norway

*From:* CCP4 bulletin board mailto:CCP4BB@JISCMAIL.AC.UK>> *On Behalf Of *Hari shankar
*Sent:* Wednesday, April 7, 2021 08:47
*To:* CCP4BB@JISCMAIL.AC.UK <mailto:CCP4BB@JISCMAIL.AC.UK>
*Subject:* [ccp4bb] Omit maps in phenix and ccp4


Dear All,

I have a ligand-protein complex and I wish to calculate different
kinds of omit maps (say, composite omit maps, simulated annealing
maps, other unbiased fo-fc maps ). I wish to omit the ligand and
3.5 angstrom 3D space around it. I have tried phenix for this
purpose but get this error message consistently.

"Fatal problems interpreting model file: no of atoms with unknown
nonbonded energy type symbols: 15 Please edit the model file to
resolve the problems and/of supply a CIF file with matching
restraint definitions, along with apply_cif_modification and
apply_cif_link parameter definitions if necessary."

This error occurs despite supplying the CIF file for the ligand. I
have tried to remake the CIF/PDB files from SMILES strings, by
drawing the molecule in both ccp4 (acedrug) as well as phenix
(elBOW and Readyset go). Nothing seems to work.

1. Is there something I have missed out that can solve this issue?

2. Is there a program in CCP4i that can be used to generate the
required omit maps?

3. In general, how do I omit 3.5 ang of the space around the
ligand during this map calculations?


Thank you so much for your time.
Hari



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Re: [ccp4bb] phenix.refine with ligand with ambiguous electron density

2020-12-03 Thread Dirk Kostrewa
ected 
to outline a strategy for every eventuality a priori - that sounds 
more like the design of an automated pipeline, not advice that users 
should be expected follow.
In summary, it's unadvisable to put all eggs in one basket (of one 
type of map, Polder or otherwise). If an experienced user likes a 
particular tool because it's worked well for them in the past, it 
doesn't mean that they shouldn't try other tools now (in this case: 
view other types of maps) the next time they encounter a 
problem. Especially given that tools in our field are still very 
much evolving over time. Different approaches may have more value 
and provide more insight in different circumstances.

Best regards,
Rob

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Re: [ccp4bb] [xds] how to specify measuring angle

2020-10-09 Thread Dirk Kostrewa

Dear Doo Nam Kim,

On 09.10.20 08:43, Doo Nam Kim wrote:

Since I don't know correct value of OSCILLATION_RANGE, I just changed to the 
example value (0.1) from (0.89976, I know it is not a positive multiple of 
0.0001, but worked for ketone data).


without knowing the correct value for the OSCILLATION_RANGE, data 
processing might run through but produces non-sense results, independent 
of the data processing program you use. So, it is absolutely important 
to know the correct value for the oscillation range per frame.


Cheers,

Dirk.

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Gene Center Munich
Department of Biochemistry, AG Hopfner
Ludwig-Maximilians-Universität München
Feodor-Lynen-Str. 25
D-81377 Munich
Germany
Phone:  +49-89-2180-76845
Fax:+49-89-2180-76998
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Re: [ccp4bb] AW: Going back to Coot 0.8

2020-09-11 Thread Dirk Kostrewa

Hi Paul,

thanks - I've setup my own key bindings, already ;-)

Cheers,

Dirk.

On 11.09.20 12:34, Paul Emsley wrote:
Maybe because I've never attended a Coot course? And maybe because, 
I've even never searched for Coot tutorials because the usage of Coot 
was (almost) always very intuitive? I am open for any new developments 


OK "Pro Tip of the Day!" then...

Edit -> Settings -> Install Template Key Bindings  # you need only do 
this once.


(this is how I move around in Coot)

Fast navigation by residue: Ctrl-G {Type a number in the little box} 
Enter -> Coot jumps to that residue number


Fast navigation by blob: {Point at a blob with your mouse cursor} G -> 
Coot brings blob to screen centre




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Re: [ccp4bb] AW: Going back to Coot 0.8

2020-09-11 Thread Dirk Kostrewa
rience in our lab.



What experience is that? I am still in the dark about you think is 
now worse.



Personally, I did would not like to judge here, as so far, I did 
not have had enough time to get into the new RSR of coot 0.9.x by 
myself. But many colleagues did not like the new refinement module 
maybe just as they are used to the method in all coot versions before.



You have a Ferrari parked beside your house but you want to to take 
the bus to work because that's what you've always done. Or maybe the 
Ferrari is parked around the back and you don't know it's there?





I just thought if it wouldn't be an option to let the user decide 
what kind of RSR implementation she/he would like to use and give 
them the choice via an option in coot preferences?



That would be possible but not easy. Unlike much of the CCP4 suite, 
Coot is Free Software. But, again... why would you want to take the 
bus? Explain.



regards,


Paul.

 



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Re: [ccp4bb] Help With Setting up a Stereo view system_walkthrough

2020-08-03 Thread Dirk Kostrewa
MAIL.AC.UK>
*Subject:*[ccp4bb] Help With Setting up a Stereo view system
Dear colleagues.
I would like to check if some one can help me with the setup of my 
hardware stereo system in Coot under Ubuntu 14

With the help of a friend I collect a bunch of second hand stuff.
1 NVIDIA 3D Video 2 system.
1 Monitor ASUS VG248 conectes through the display port
1 NVIDIA QUADRO 4000 video card.
After connecting everything and having a nightmare to install the 
Legacy Drivers 390.138

And following this instructions
https://strucbio.biologie.uni-konstanz.de/ccp4wiki/index.php/Stereo
I run nvidia-xconfig --stereo=10
I connected the emitter both by USB and the DIN 3 pin conector
I connected the monitor through the Display Port
I reboot and , the emitter finally shows the green light
I can run nvidia-settings and I have the control panel


I see Stereo 3D Vision Stereo but only the left cube running.
But when I activate hardware stereo nothing works.
Does anybody have a clue of what to do?
Thanks in advance,
Marian
Marian Oliva
CSIC-Centro de Investigaciones Biológicas Margarita Salas
9, Ramiro de Maeztu
28040-Madrid (Spain)

phone: 0034 91 8373112 (x4380)
e-mail: mar...@cib.csic.es <mailto:mar...@cib.csic.es>

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Re: [ccp4bb] Help With Setting up a Stereo view system

2020-07-31 Thread Dirk Kostrewa

Dear Marian Oliva,

in my experience, MATE, XFCE and Plasma 5/KDE work well with 3D stereo 
if the compositor is disabled. You don't even have to disable COMPOSITE 
in the xorg.conf - for those desktops, it is sufficient to disable 
composite in the respective desktop/compositor/window manager settings 
(tested with Debian Stable and CentOS 8; unfortunately, I can't access 
my documents for more details).


For Gnome 3, the picture is somewhat mixed: the gnome3 shell crashes if 
you disable composite in xorg.conf. However, if you use a recent Fedora 
or CentOS 8 (which is based on relatively recent Fedoras), 3D stereo 
works under Gnome 3 out-of-the-box. Upon switching 3D stereo on/off, you 
will notice a delay of ~1 second, before a message appears that stereo 
has been enabled/disabled. I guess, in these distributions, the 
compositor is somehow switched in the background without crashing the 
session.


Independent of the desktop, for Fedora/CentOS 8, it might be necessary 
to place a udev rule to give write permissions to the USB emitter for 
regular users. So, if 3D stereo works under root, but not under a 
regular user, you should create a rule like 
/etc/udev/rules.d/98-nvstusb.rules, with the contents


# NVIDIA 3D Vision USB IR Emitter
SUBSYSTEM=="usb", ATTR{idVendor}=="0955", ATTR{idProduct}=="0007", 
MODE="0666"


Cheers,

Dirk.


On 30.07.20 14:46, Marian Oliva wrote:

Dear colleagues.

I would like to check if some one can help me with the setup of my 
hardware stereo system in Coot under Ubuntu 14


With the help of a friend I collect a bunch of second hand stuff.

1 NVIDIA 3D Video 2 system.
1 Monitor ASUS VG248 conectes through the display port
1 NVIDIA QUADRO 4000 video card.

After connecting everything and having a nightmare to install the 
Legacy Drivers 390.138


And following this instructions

https://strucbio.biologie.uni-konstanz.de/ccp4wiki/index.php/Stereo

I run nvidia-xconfig --stereo=10

I connected the emitter both by USB and the DIN 3 pin conector
I connected the monitor through the Display Port

I reboot and , the emitter finally shows the green light

I can run nvidia-settings and I have the control panel

I see Stereo 3D Vision Stereo but only the left cube running.

But when I activate hardware stereo nothing works.

Does anybody have a clue of what to do?

Thanks in advance,

Marian


Marian Oliva
CSIC-Centro de Investigaciones Biológicas Margarita Salas
9, Ramiro de Maeztu
28040-Madrid (Spain)

phone: 0034 91 8373112 (x4380)
e-mail: mar...@cib.csic.es <mailto:mar...@cib.csic.es>

**NOTA DE CONFIDENCIALIDAD** Este correo electrónico, y en su caso los 
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D-81377 Munich
Germany
Phone:  +49-89-2180-76845
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Re: [ccp4bb] AW: [ccp4bb] [EXTERNAL] Re: [ccp4bb] number of frames to get a full dataset?

2020-07-01 Thread Dirk Kostrewa

Dear Kay & Gerard,

the only reason, why I want to count differently, is to distinguish 
between true and pseudo-multiplicity. Apparently, I get on thin ice by 
trying to define "identical" reflections ... maybe, instead, we should 
start working with unmerged data in all programs. If I remember 
correctly, this is something that Gerard proposed long time ago for 
phasing programs.


Best wishes,

Dirk.

On 01.07.20 11:52, Kay Diederichs wrote:

Dear Dirk,

one cannot fully correct radiation damage. Normal scaling procedures take care of the 
average decay by a smooth resolution-dependant function. Zero-dose extrapolation goes 
beyond that but needs all symmetry mates - this does not fulfill your definition of 
"identical".

If we really could correct radiation damage then we could collect data to high 
resolution from all crystals just by using very high dose, and solve structures 
much more easily.

How often you count a reflection is up to you; I don't see what you gain by 
this.

best,
Kay

Am 01.07.20 um 11:42 schrieb Dirk Kostrewa:

Dear Gerard and Kay,

yes, you are both right - I have totally forgotten radiation damage! And 
correcting for this really makes a difference!

However, if radiation damage is corrected for reflections measured at different 
time points under the same geometry, does anything speak against it, to average 
them and count them only once (say, for crystals measured multiple rounds of 
360 degrees to find identical geometries)?

Best wishes,

Dirk.

On 01.07.20 11:02, Gerard Bricogne wrote:

Dear Dirk,

   Aren't you for getting about radiation damage? The n measurements of
the same hkl with the same geometry would not be equivalent, although they
would enable the tracking of radiation damage without the confounding with
absorption effects that comes from considering symmetry-related hkls. I
mentioned that in my second message yesterday.

   The notion of "identical" reflections measurements is problematic for
the same reason that Heraclitus wrote (something like) "You cannot step
twice into the same river".


   With best wishes,

    Gerard.

--
On Wed, Jul 01, 2020 at 10:46:57AM +0200, Dirk Kostrewa wrote:

Dear Herman,

I think, your MPR proposal is a great idea and would like to second it! And
I would also like to propose that data processing programs just average
"identical" reflections measured under the same geometry and count them only
once (*), so that, in the end, we will get a realistic number of truly
independent measurements.

Cheers,

Dirk.

(*) I don't see a difference between measuring the same reflection with the
same geometry n-times and measuring it n-times as long (apart from, maybe,
catching instabilities in the experimental setup). Just averaging such
"identical" reflections would simplify the subsequent scaling process with
equivalent reflections that were measured under different geometry.

On 01.07.20 09:32, Schreuder, Herman /DE wrote:

Dear Bernard and other bulletin board members,

As Gerard mentioned, current data processing programs and table 1’s do
not make this distinction, but of course, you are free to ask the
community to introduce it.

My proposal to use “measurements per reflections” is not a joke. It
exactly describes what is meant by the parameter and it is easily
understood even by lay people like journal editors and referees, without
the need of lengthy explanations like the ones we have seen in this
thread.

I really would like to ask you to consider replacing
multiplicity/redundancy/abundancy by MPR. At minimum, it may prevent a
thread about completeness of data sets to be hijacked by a discussion on
whether use the name multiplicity of redundancy for the number of
measurements per reflection.

My 2 cents,

Herman

*Von:* CCP4 bulletin board  *Im Auftrag von
*Bernhard Rupp
*Gesendet:* Dienstag, 30. Juni 2020 17:50
*An:* CCP4BB@JISCMAIL.AC.UK
*Betreff:* Re: [ccp4bb] [EXTERNAL] Re: [ccp4bb] number of frames to get
a full dataset?

*EXTERNAL : *Real sender is owner-ccp...@jiscmail.ac.uk
<mailto:owner-ccp...@jiscmail.ac.uk>

.…but there is a difference whether I measure the same identical hkl
over again or ‘preferably in more than one symmetry-equivalent
position’, to quote the

IUCr. So do we have a MPSR for the same reflection and a MPRR for the
related reflections?

Cacophonically yours,

BR

*From:*CCP4 bulletin board mailto:CCP4BB@JISCMAIL.AC.UK>> *On Behalf Of *John R Helliwell
*Sent:* Tuesday, June 30, 2020 08:36
*To:* CCP4BB@JISCMAIL.AC.UK <mailto:CCP4BB@JISCMAIL.AC.UK>
*Subject:* Re: [ccp4bb] [EXTERNAL] Re: [ccp4bb] number of frames to get
a full dataset?

Dear Herman,

I think that MPR is a very neat and tidy, excellent, proposal.

Moreover it uses the word “measurements”, and we are an experimental
based science.

I support it.

Great.

Greetings,

John

Emeritus Professor John R Helliwell DSc

  On 30 Jun 2020, at 1

Re: [ccp4bb] AW: [ccp4bb] [EXTERNAL] Re: [ccp4bb] number of frames to get a full dataset?

2020-07-01 Thread Dirk Kostrewa

Dear Gerard and Kay,

yes, you are both right - I have totally forgotten radiation damage! And 
correcting for this really makes a difference!


However, if radiation damage is corrected for reflections measured at 
different time points under the same geometry, does anything speak 
against it, to average them and count them only once (say, for crystals 
measured multiple rounds of 360 degrees to find identical geometries)?


Best wishes,

Dirk.

On 01.07.20 11:02, Gerard Bricogne wrote:

Dear Dirk,

  Aren't you for getting about radiation damage? The n measurements of
the same hkl with the same geometry would not be equivalent, although they
would enable the tracking of radiation damage without the confounding with
absorption effects that comes from considering symmetry-related hkls. I
mentioned that in my second message yesterday.

  The notion of "identical" reflections measurements is problematic for
the same reason that Heraclitus wrote (something like) "You cannot step
twice into the same river".


  With best wishes,

   Gerard.

--
On Wed, Jul 01, 2020 at 10:46:57AM +0200, Dirk Kostrewa wrote:

Dear Herman,

I think, your MPR proposal is a great idea and would like to second it! And
I would also like to propose that data processing programs just average
"identical" reflections measured under the same geometry and count them only
once (*), so that, in the end, we will get a realistic number of truly
independent measurements.

Cheers,

Dirk.

(*) I don't see a difference between measuring the same reflection with the
same geometry n-times and measuring it n-times as long (apart from, maybe,
catching instabilities in the experimental setup). Just averaging such
"identical" reflections would simplify the subsequent scaling process with
equivalent reflections that were measured under different geometry.

On 01.07.20 09:32, Schreuder, Herman /DE wrote:

Dear Bernard and other bulletin board members,

As Gerard mentioned, current data processing programs and table 1’s do
not make this distinction, but of course, you are free to ask the
community to introduce it.

My proposal to use “measurements per reflections” is not a joke. It
exactly describes what is meant by the parameter and it is easily
understood even by lay people like journal editors and referees, without
the need of lengthy explanations like the ones we have seen in this
thread.

I really would like to ask you to consider replacing
multiplicity/redundancy/abundancy by MPR. At minimum, it may prevent a
thread about completeness of data sets to be hijacked by a discussion on
whether use the name multiplicity of redundancy for the number of
measurements per reflection.

My 2 cents,

Herman

*Von:* CCP4 bulletin board  *Im Auftrag von
*Bernhard Rupp
*Gesendet:* Dienstag, 30. Juni 2020 17:50
*An:* CCP4BB@JISCMAIL.AC.UK
*Betreff:* Re: [ccp4bb] [EXTERNAL] Re: [ccp4bb] number of frames to get
a full dataset?

*EXTERNAL : *Real sender is owner-ccp...@jiscmail.ac.uk
<mailto:owner-ccp...@jiscmail.ac.uk>

.…but there is a difference whether I measure the same identical hkl
over again or ‘preferably in more than one symmetry-equivalent
position’, to quote the

IUCr. So do we have a MPSR for the same reflection and a MPRR for the
related reflections?

Cacophonically yours,

BR

*From:*CCP4 bulletin board mailto:CCP4BB@JISCMAIL.AC.UK>> *On Behalf Of *John R Helliwell
*Sent:* Tuesday, June 30, 2020 08:36
*To:* CCP4BB@JISCMAIL.AC.UK <mailto:CCP4BB@JISCMAIL.AC.UK>
*Subject:* Re: [ccp4bb] [EXTERNAL] Re: [ccp4bb] number of frames to get
a full dataset?

Dear Herman,

I think that MPR is a very neat and tidy, excellent, proposal.

Moreover it uses the word “measurements”, and we are an experimental
based science.

I support it.

Great.

Greetings,

John

Emeritus Professor John R Helliwell DSc

 On 30 Jun 2020, at 15:10, Schreuder, Herman /DE
 mailto:herman.schreu...@sanofi.com>>
 wrote:

 

 Dear BB,

 Since there does not seem a generally accepted term for the
 subject of this discussions, and since even the IUCR scriptures do
 not give any guidance, I would propose to introduce a completely
 new term:

 Measurements per reflection or MPR

 This term is politically neutral, should adequately describe this
 particular statistic and is not associated with entrenched
 traditions at either side of the Atlantic.

 What do you think?

 Herman

 *Von:*CCP4 bulletin board mailto:CCP4BB@JISCMAIL.AC.UK>> *Im Auftrag von *John R Helliwell
 *Gesendet:* Dienstag, 30. Juni 2020 14:34
 *An:* CCP4BB@JISCMAIL.AC.UK <mailto:CCP4BB@JISCMAIL.AC.UK>
 *Betreff:* [EXTERNAL] Re: [ccp4bb] number of frames to get a full
 dataset?

 *EXTERNAL : *Real sender is owner-ccp...@jiscmail.ac.uk
 <mailto:owner-ccp...@jiscmail.ac.uk>

 Dear Colleagues,

 In an effort to break this naming deadlock, 

Re: [ccp4bb] AW: [ccp4bb] [EXTERNAL] Re: [ccp4bb] number of frames to get a full dataset?

2020-07-01 Thread Dirk Kostrewa
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***
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Gene Center Munich
Department of Biochemistry, AG Hopfner
Ludwig-Maximilians-Universität München
Feodor-Lynen-Str. 25
D-81377 Munich
Germany
Phone:  +49-89-2180-76845
Fax:+49-89-2180-76998
E-mail: dirk.kostr...@lmu.de
WWW:www.genzentrum.lmu.de
strubio.userweb.mwn.de
***




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Re: [ccp4bb] Space group/Unit cell

2020-05-22 Thread Dirk Kostrewa

Dear Maria,

are you sure, it's I222? From the extinction rules, you can't 
distinguish between I222 and I2(1)2(1)2(1).


Best regards,

Dirk.

On 22.05.20 12:08, Demou, Maria wrote:

Dear all,
I have a question that may have a straight forward answer, and was 
wondering if this is a common issue. We have a protein crystallised in 
I222 space group. This is CRP, but the monomer/pentamer is not predicted 
to fit in this space group. Is there a possibility of the lipid cubic 
phase being crystallised on it's own, or is there any other obvious reason?


Thank you,
Maria




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***
Dirk Kostrewa
Gene Center Munich
Department of Biochemistry, AG Hopfner
Ludwig-Maximilians-Universität München
Feodor-Lynen-Str. 25
D-81377 Munich
Germany
Phone:  +49-89-2180-76845
Fax:+49-89-2180-76998
E-mail: dirk.kostr...@lmu.de
WWW:www.genzentrum.lmu.de
strubio.userweb.mwn.de
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Re: [ccp4bb] nVidia 3D Vision2 glasses

2020-01-15 Thread Dirk Kostrewa
rsten Beneke (stellv. Vorsitzender), Prof. Dr.-Ing. Harald Bolt,
Prof. Dr. Sebastian M. Schmidt





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**
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Gene Center Munich
Department of Biochemistry, AG Hopfner
Ludwig-Maximilians-Universität München
Feodor-Lynen-Str. 25
D-81377 Munich
Germany
Phone:  +49-89-2180-76845
Fax:+49-89-2180-76998
E-mail: dirk.kostr...@lmu.de
kostr...@genzentrum.lmu.de
WWW:www.genzentrum.lmu.de
strubio.userweb.mwn.de
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Re: [ccp4bb] nVidia 3D Vision2 glasses

2020-01-09 Thread Dirk Kostrewa

Hi Matthias,


although, Nvidia announced that the final driver with 3D stereo is the 
418 driver, the more recent drivers (at least up to 440) under Linux 
(CentOS 7.7) apparently still support quad-buffered 3D stereo on our 
Quadro cards. This is in line with the 3D Vision End-of-Life FAQ 
<https://nvidia.custhelp.com/app/answers/detail/a_id/4845/~/3d-vision-end-of-life---faq> 
on the Nvidia site.



Best regards,


Dirk Kostrewa.


On 1/9/20 10:37 AM, Barone, Matthias wrote:


Hi Patricia

All modern graphics cards still support 3D vision, but you are correct 
that nvidia is addressing critical issues in release 418 only till 
April. So if you got a new card, you should not run into problems 
anytime soon. Just make sure the card is supported with the new kernel 
packages before updating and stick to the driver release 418. I did so 
for the last 7 years and just recently had to refurbish the card as it 
was no longer supported by centos 7.7.1908


So, I dont have an alternative yet either..

Best, matthias



Dr. Matthias Barone

AG Kuehne, Rational Drug Design

Leibniz-Forschungsinstitut für Molekulare Pharmakologie (FMP)
Robert-Rössle-Strasse 10
13125 Berlin

Germany
Phone: +49 (0)30 94793-284


*From:* CCP4 bulletin board  on behalf of 
Patricia Borges 

*Sent:* Wednesday, January 8, 2020 7:25:20 PM
*To:* CCP4BB@JISCMAIL.AC.UK
*Subject:* [ccp4bb] nVidia 3D Vision2 glasses
Dear all,

Does anyone knows any alternative to the nVidia 3D Vision2 glasses for 
a Ubuntu workstation, since these are at the moment discontinued?


Thanks a lot for the help,
Best regards
Patricia



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Gene Center Munich
Department of Biochemistry, AG Hopfner
Ludwig-Maximilians-Universität München
Feodor-Lynen-Str. 25
D-81377 Munich
Germany
Phone:  +49-89-2180-76845
Fax:+49-89-2180-76998
E-mail: dirk.kostr...@lmu.de
kostr...@genzentrum.lmu.de
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strubio.userweb.mwn.de
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Re: [ccp4bb] OT: Nvidia 3D vision 2 glasses with Ubuntu workstation

2019-01-08 Thread Dirk Kostrewa

Dear colleagues,

since approximately end of last year, there is indeed a 3D stereo 
problem under CentOS/Scientific Linux 7.6. I found the odd reason for 
this by a small warning message in the Xorg-log file and some 
trial-and-error and just want to share this with you, in case, you come 
across the same problem:


My xorg.conf contains the usual switch-off of the composite extension, 
since this is incompatible with 3D stereo:


Section "Extensions"
    Option "Composite" "Disable"
EndSection

However, in recent Xorg-log files, there is a warning that the extension 
"Composite" is not recognized, but the extension "COMPOSITE" is loaded. 
This doesn't lead to 3D stereo problems on the KDE desktop, but disables 
3D stereo on the MATE and probably the XFCE desktop. The solution is 
both odd and easy - you have to modify the composite option in your 
xorg.conf as follows:


Section "Extensions"
    Option "COMPOSITE" "Disable"
EndSection

I have no idea, since when Xorg is case-sensitive, or whether this has 
anything to do with the Nvidia driver (I use the one from ELRepo). 
Anyway, this solution appears to work.


Best wishes,

Dirk.

On 20.12.18 22:28, Kay Diederichs wrote:

Unfortunately, monitors with built-in emitter are no longer being manufactured. 
The NVIDIA website has not been updated for years. So that path leads nowhere.

Stereo has worked well for us (for existing monitors with built-in emitter, and 
with Quadro cards /USB emitter) until and including CentOS 7.5. Recently, this 
stopped after updating to CentOS 7.6 - coot finds the stereo-capable hardware 
and reports the switch to stereo, but the monitor does not flip the pictures. 
We are investigating. We are using the Nvidia drivers through the EPEL 
repository.

best,

Kay


On Thu, 20 Dec 2018 16:11:56 -0500, David Schuller  wrote:


I can see two possible paths here:

1) Make the card work with an emitter

or 2) Switch to a monitor with a built-in emitter

Datasheet on the graphics card:
<https://www.nvidia.com/content/dam/en-zz/Solutions/design-visualization/productspage/quadro/quadro-desktop/quadro-pascal-p4000-data-sheet-us-nvidia-704358-r2-web.pdf>

"3D Stereo support with Stereo Connector1
...
1 VGA/DVI/HDMI/stereo support via adapter/connector/bracket"

The task then is to identify the correct bracket to work with this card,
and find a source for purchase.
Something like this:

https://www.bhphotovideo.com/c/product/652465-REG/PNY_Technologies_900_50762__000_Stereo_Bracket_for_Quadro.html
"PNY Technoligies Stereo Bracket for Quadro FX 3800"

Is this part also compatible with the Quadro P4000? I do not know.

http://www8.hp.com/h20195/v2/GetPDF.aspx/c04658472.pdf
"NVidia 3D Stereo Bracket...
Supports NVIDIA Quadro® K4000, K5000, K6000, K4200, K5200,
M4000, M5000, M6000, P4000, P5000, P6000 graphics cards"


Seems promising.

-
Here is a web page listing compatible monitors. You can filter for those
with "built-in emitter"

https://www.nvidia.com/object/3d-vision-displays.html





On 12/20/18 3:45 PM, Adarsh Kumar wrote:

Hello everyone

We have just purchased a Dell workstation for crystallography data analysis. We 
were trying to use Nvidia 3D vision 2 glasses with it, but failed to do so. 
Please help me out with this one. Some relevant information is as follows:
OS: Ubuntu 16.04 LTS
Graphics : Quadro P4000 (unfortunately doesn't have a 3-pin DIN socket)
Monitor: Asus VG248QE

Thanks and regards
Adarsh Kumar
Suo Lab
Florida State University College of Medicine



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All Things Serve the Beam
===
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modern man in a post-modern world
MacCHESS, Cornell University
schul...@cornell.edu




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**
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Gene Center Munich
Department of Biochemistry, AG Hopfner
Ludwig-Maximilians-Universität München
Feodor-Lynen-Str. 25
D-81377 Munich
Germany
Phone:  +49-89-

[ccp4bb] Fwd: Re: [ccp4bb] OT: Nvidia 3D vision 2 glasses with Ubuntu workstation

2019-01-07 Thread Dirk Kostrewa
Sorry for spamming the CCP4BB with this e-mail meant for Kay, only - I 
accidentally used the "Reply All" button instead of the "Reply" button 
... ;-)


Anyway, I wish the CCP4 community a Happy New Year!

Cheers,

Dirk.

 Forwarded Message 
Subject: 	Re: [ccp4bb] OT: Nvidia 3D vision 2 glasses with Ubuntu 
workstation

Date:   Mon, 7 Jan 2019 14:12:05 +0100
From:   Dirk Kostrewa 
Reply-To:   dirk.kostr...@lmu.de
To: CCP4BB@JISCMAIL.AC.UK



Lieber Kay,

ich wünsche Dir ein Frohes und Gesundes Neues Jahr!

Ich staune auch, dass es anscheinend keine "3D-Ready"-Monitore mehr 
gibt! Wir haben einmal versuchsweise einen 144 Hz ASUS Monitor ohne 
"3D-Ready" gekauft - leider hat da die Synchronisation mit der 
Stereo-Brille nicht funktioniert ...


Mit unseren alten 3D-Ready-Monitoren haben wir unter Scientific Linux 
7.6 bisher keine 3D Stereo-Probleme beobachten können. Die 
Nvidia-Treiber kommen aus dem ELRepo-Repository. Habt Ihr die 
Stereo-Probleme noch?


Liebe Grüße,

Dirk.

On 20.12.18 22:28, Kay Diederichs wrote:
Unfortunately, monitors with built-in emitter are no longer being 
manufactured. The NVIDIA website has not been updated for years. So 
that path leads nowhere.


Stereo has worked well for us (for existing monitors with built-in 
emitter, and with Quadro cards /USB emitter) until and including 
CentOS 7.5. Recently, this stopped after updating to CentOS 7.6 - coot 
finds the stereo-capable hardware and reports the switch to stereo, 
but the monitor does not flip the pictures. We are investigating. We 
are using the Nvidia drivers through the EPEL repository.


best,

Kay


On Thu, 20 Dec 2018 16:11:56 -0500, David Schuller 
 wrote:



I can see two possible paths here:

1) Make the card work with an emitter

or 2) Switch to a monitor with a built-in emitter

Datasheet on the graphics card:
<https://www.nvidia.com/content/dam/en-zz/Solutions/design-visualization/productspage/quadro/quadro-desktop/quadro-pascal-p4000-data-sheet-us-nvidia-704358-r2-web.pdf>

"3D Stereo support with Stereo Connector1
...
1 VGA/DVI/HDMI/stereo support via adapter/connector/bracket"

The task then is to identify the correct bracket to work with this card,
and find a source for purchase.
Something like this:

https://www.bhphotovideo.com/c/product/652465-REG/PNY_Technologies_900_50762__000_Stereo_Bracket_for_Quadro.html
"PNY Technoligies Stereo Bracket for Quadro FX 3800"

Is this part also compatible with the Quadro P4000? I do not know.

http://www8.hp.com/h20195/v2/GetPDF.aspx/c04658472.pdf
"NVidia 3D Stereo Bracket...
Supports NVIDIA Quadro® K4000, K5000, K6000, K4200, K5200,
M4000, M5000, M6000, P4000, P5000, P6000 graphics cards"


Seems promising.

-
Here is a web page listing compatible monitors. You can filter for those
with "built-in emitter"

https://www.nvidia.com/object/3d-vision-displays.html





On 12/20/18 3:45 PM, Adarsh Kumar wrote:

Hello everyone

We have just purchased a Dell workstation for crystallography data 
analysis. We were trying to use Nvidia 3D vision 2 glasses with it, 
but failed to do so. Please help me out with this one. Some relevant 
informationis as follows:

OS: Ubuntu 16.04 LTS
Graphics : Quadro P4000 (unfortunately doesn't have a 3-pin DIN socket)
Monitor: Asus VG248QE

Thanks and regards
Adarsh Kumar
Suo Lab
Florida State University College of Medicine



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#

Re: [ccp4bb] OT: Nvidia 3D vision 2 glasses with Ubuntu workstation

2019-01-07 Thread Dirk Kostrewa

Lieber Kay,

ich wünsche Dir ein Frohes und Gesundes Neues Jahr!

Ich staune auch, dass es anscheinend keine "3D-Ready"-Monitore mehr 
gibt! Wir haben einmal versuchsweise einen 144 Hz ASUS Monitor ohne 
"3D-Ready" gekauft - leider hat da die Synchronisation mit der 
Stereo-Brille nicht funktioniert ...


Mit unseren alten 3D-Ready-Monitoren haben wir unter Scientific Linux 
7.6 bisher keine 3D Stereo-Probleme beobachten können. Die 
Nvidia-Treiber kommen aus dem ELRepo-Repository. Habt Ihr die 
Stereo-Probleme noch?


Liebe Grüße,

Dirk.

On 20.12.18 22:28, Kay Diederichs wrote:

Unfortunately, monitors with built-in emitter are no longer being manufactured. 
The NVIDIA website has not been updated for years. So that path leads nowhere.

Stereo has worked well for us (for existing monitors with built-in emitter, and 
with Quadro cards /USB emitter) until and including CentOS 7.5. Recently, this 
stopped after updating to CentOS 7.6 - coot finds the stereo-capable hardware 
and reports the switch to stereo, but the monitor does not flip the pictures. 
We are investigating. We are using the Nvidia drivers through the EPEL 
repository.

best,

Kay


On Thu, 20 Dec 2018 16:11:56 -0500, David Schuller  wrote:


I can see two possible paths here:

1) Make the card work with an emitter

or 2) Switch to a monitor with a built-in emitter

Datasheet on the graphics card:
<https://www.nvidia.com/content/dam/en-zz/Solutions/design-visualization/productspage/quadro/quadro-desktop/quadro-pascal-p4000-data-sheet-us-nvidia-704358-r2-web.pdf>

"3D Stereo support with Stereo Connector1
...
1 VGA/DVI/HDMI/stereo support via adapter/connector/bracket"

The task then is to identify the correct bracket to work with this card,
and find a source for purchase.
Something like this:

https://www.bhphotovideo.com/c/product/652465-REG/PNY_Technologies_900_50762__000_Stereo_Bracket_for_Quadro.html
"PNY Technoligies Stereo Bracket for Quadro FX 3800"

Is this part also compatible with the Quadro P4000? I do not know.

http://www8.hp.com/h20195/v2/GetPDF.aspx/c04658472.pdf
"NVidia 3D Stereo Bracket...
Supports NVIDIA Quadro® K4000, K5000, K6000, K4200, K5200,
M4000, M5000, M6000, P4000, P5000, P6000 graphics cards"


Seems promising.

-
Here is a web page listing compatible monitors. You can filter for those
with "built-in emitter"

https://www.nvidia.com/object/3d-vision-displays.html





On 12/20/18 3:45 PM, Adarsh Kumar wrote:

Hello everyone

We have just purchased a Dell workstation for crystallography data analysis. We 
were trying to use Nvidia 3D vision 2 glasses with it, but failed to do so. 
Please help me out with this one. Some relevant information is as follows:
OS: Ubuntu 16.04 LTS
Graphics : Quadro P4000 (unfortunately doesn't have a 3-pin DIN socket)
Monitor: Asus VG248QE

Thanks and regards
Adarsh Kumar
Suo Lab
Florida State University College of Medicine



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https://www.jiscmail.ac.uk/cgi-bin/webadmin?SUBED1=CCP4BB=1


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===
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MacCHESS, Cornell University
schul...@cornell.edu




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**
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Gene Center Munich
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Ludwig-Maximilians-Universität München
Feodor-Lynen-Str. 25
D-81377 Munich
Germany
Phone:  +49-89-2180-76845
Fax:+49-89-2180-76998
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[ccp4bb] Fwd: [ccp4bb] Calculation of generalised R-factor?

2016-12-20 Thread Dirk Kostrewa

Dear CCP4ers,

many thanks to all of you who replied to my request!

I wish you a Merry Christmas and a Happy New Year!

Dirk.


 Forwarded Message 
Subject:[ccp4bb] Calculation of generalised R-factor?
Date:   Tue, 20 Dec 2016 14:47:00 +0100
From:   Dirk Kostrewa <kostr...@genzentrum.lmu.de>
Reply-To:   Dirk Kostrewa <kostr...@genzentrum.lmu.de>
To: CCP4BB@JISCMAIL.AC.UK



Dear CCP4ers,

I want to check the validity of the refinement of anisotropic B-factors
vs. TLS + isototropic B-factors using the Hamilton R-value ratio test as
described in Ethan Merritt's paper "To B or not to B", Acta Cryst. D,
Vol 68, pp 468. This test uses the generalised R-factors (assuming unit
weights), RG=(Sum(Fo-Fc)^2/Sum(Fo)^2)^1/2. Although Hamilton wrote that
at the end of refinement, one could also use the similar ratio of the
usual R-factors, I really would like to check the ratio of the RG-values
after refinement. As far as I can see, this value is not reported by the
usual refinement programs.

Is there a program that reads an mtz file with Fo and refined Fc and
just calculates RG?

Best regards,

Dirk.

--

***
Dirk Kostrewa
Gene Center Munich, A5.07
Department of Biochemistry
Ludwig-Maximilians-Universität München
Feodor-Lynen-Str. 25
D-81377 Munich
Germany
Phone:  +49-89-2180-76845
Fax:+49-89-2180-76998
E-mail: kostr...@genzentrum.lmu.de
WWW:www.genzentrum.lmu.de
***


--

***
Dirk Kostrewa
Gene Center Munich, A5.07
Department of Biochemistry
Ludwig-Maximilians-Universität München
Feodor-Lynen-Str. 25
D-81377 Munich
Germany
Phone:  +49-89-2180-76845
Fax:+49-89-2180-76998
E-mail: kostr...@genzentrum.lmu.de
WWW:www.genzentrum.lmu.de
***



Re: [ccp4bb] Calculation of generalised R-factor?

2016-12-20 Thread Dirk Kostrewa

Dear Robbie,

thanks for your reply. According to the REFMAC5 manual, the weighted 
R-factor is just:


weighted R factor = sum w ||F_o -|F_c ||/sum w |F_o |

So, unfortunately, it is not the generalised R-factor.

Do you have a reference for that follow-up paper?

PDB_REDO does too much for my purpose ...

Cheers,

Dirk.


On 20.12.2016 15:37, Robbie Joosten wrote:


The value for the Hamilton test is written by Refmac as the weighted 
R-factor. There was a follow-up paper that showed that you shouldn’t 
use the normal R-factor for the Hamilton test.


PDB_REDO does the Hamilton test automatically, but you can also feed 
two Refmac logfiles to the bselect program to do your own Hamilton test.


Cheers,

Robbie

Sent from my Windows 10 phone

*Van: *Keller, Jacob <mailto:kell...@janelia.hhmi.org>
*Verzonden: *dinsdag 20 december 2016 14:23
*Aan: *CCP4BB@JISCMAIL.AC.UK <mailto:CCP4BB@JISCMAIL.AC.UK>
*Onderwerp: *Re: [ccp4bb] Calculation of generalised R-factor?

I'd be interested as well.

JPK

-Original Message-
From: CCP4 bulletin board [mailto:CCP4BB@JISCMAIL.AC.UK] On Behalf Of 
Dirk Kostrewa

Sent: Tuesday, December 20, 2016 8:47 AM
To: CCP4BB@JISCMAIL.AC.UK
Subject: [ccp4bb] Calculation of generalised R-factor?

Dear CCP4ers,

I want to check the validity of the refinement of anisotropic 
B-factors vs. TLS + isototropic B-factors using the Hamilton R-value 
ratio test as described in Ethan Merritt's paper "To B or not to B", 
Acta Cryst. D, Vol 68, pp 468. This test uses the generalised 
R-factors (assuming unit weights), RG=(Sum(Fo-Fc)^2/Sum(Fo)^2)^1/2. 
Although Hamilton wrote that at the end of refinement, one could also 
use the similar ratio of the usual R-factors, I really would like to 
check the ratio of the RG-values after refinement. As far as I can 
see, this value is not reported by the usual refinement programs.


Is there a program that reads an mtz file with Fo and refined Fc and 
just calculates RG?


Best regards,

Dirk.

--

***
Dirk Kostrewa
Gene Center Munich, A5.07
Department of Biochemistry
Ludwig-Maximilians-Universität München
Feodor-Lynen-Str. 25
D-81377 Munich
Germany
Phone:  +49-89-2180-76845
Fax:+49-89-2180-76998
E-mail: kostr...@genzentrum.lmu.de
WWW: www.genzentrum.lmu.de <http://www.genzentrum.lmu.de>
***


--

***
Dirk Kostrewa
Gene Center Munich, A5.07
Department of Biochemistry
Ludwig-Maximilians-Universität München
Feodor-Lynen-Str. 25
D-81377 Munich
Germany
Phone:  +49-89-2180-76845
Fax:+49-89-2180-76998
E-mail: kostr...@genzentrum.lmu.de
WWW:www.genzentrum.lmu.de
***



[ccp4bb] Calculation of generalised R-factor?

2016-12-20 Thread Dirk Kostrewa

Dear CCP4ers,

I want to check the validity of the refinement of anisotropic B-factors 
vs. TLS + isototropic B-factors using the Hamilton R-value ratio test as 
described in Ethan Merritt's paper "To B or not to B", Acta Cryst. D, 
Vol 68, pp 468. This test uses the generalised R-factors (assuming unit 
weights), RG=(Sum(Fo-Fc)^2/Sum(Fo)^2)^1/2. Although Hamilton wrote that 
at the end of refinement, one could also use the similar ratio of the 
usual R-factors, I really would like to check the ratio of the RG-values 
after refinement. As far as I can see, this value is not reported by the 
usual refinement programs.


Is there a program that reads an mtz file with Fo and refined Fc and 
just calculates RG?


Best regards,

Dirk.

--

***
Dirk Kostrewa
Gene Center Munich, A5.07
Department of Biochemistry
Ludwig-Maximilians-Universität München
Feodor-Lynen-Str. 25
D-81377 Munich
Germany
Phone:  +49-89-2180-76845
Fax:+49-89-2180-76998
E-mail: kostr...@genzentrum.lmu.de
WWW:www.genzentrum.lmu.de
***


Re: [ccp4bb] AW: [ccp4bb] Rfree below Rwork

2015-07-02 Thread Dirk Kostrewa
 stresses the independence assumption of the 
free set.
 Am I correct in believing that Rfree *may* be smaller than Rcryst 
even in

 the absence of a major mistake? My hope is that the combined wisdom of
 ccp4bb followers can point out my possible mistake,  suggest tests 
that I

 may perform to avoid them and, possibly, arguments in defense of a
 crystallographic model with Rfree  Rcryst.
 Many thanks,
 Wolfram Tempel

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***
Dirk Kostrewa
Gene Center Munich, A5.07
Department of Biochemistry
Ludwig-Maximilians-Universität München
Feodor-Lynen-Str. 25
D-81377 Munich
Germany
Phone:  +49-89-2180-76845
Fax:+49-89-2180-76999
E-mail: kostr...@genzentrum.lmu.de
WWW:www.genzentrum.lmu.de
***



Re: [ccp4bb] [SUSPECTED SPAM] Re: [ccp4bb] nVidia quadro Update for Linux

2015-04-07 Thread Dirk Kostrewa
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Dirk Kostrewa
Gene Center Munich, A5.07
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Feodor-Lynen-Str. 25
D-81377 Munich
Germany
Phone:  +49-89-2180-76845
Fax:+49-89-2180-76999
E-mail: kostr...@genzentrum.lmu.de
WWW:www.genzentrum.lmu.de
***



Re: [ccp4bb] Bulk solvent

2015-01-12 Thread Dirk Kostrewa
-
From: CCP4 bulletin board [mailto:CCP4BB@JISCMAIL.AC.UK 
mailto:CCP4BB@JISCMAIL.AC.UK] On Behalf Of Armando Albert

Sent: Friday, January 09, 2015 12:56 AM
To: CCP4BB@JISCMAIL.AC.UK mailto:CCP4BB@JISCMAIL.AC.UK
Subject: [ccp4bb] Bulk solvent

Dear all,
Is there any reason for using Babinet scaling for bulk solvent 
correction instead of mask based scaling?

Armando



--

***
Dirk Kostrewa
Gene Center Munich, A5.07
Department of Biochemistry
Ludwig-Maximilians-Universität München
Feodor-Lynen-Str. 25
D-81377 Munich
Germany
Phone:  +49-89-2180-76845
Fax:+49-89-2180-76999
E-mail: kostr...@genzentrum.lmu.de
WWW:www.genzentrum.lmu.de
***



Re: [ccp4bb] Bulk solvent

2015-01-12 Thread Dirk Kostrewa

Dear Bernhard,

further thinking about the Babinet scaling effects, I have to correct my 
conclusion in the last sentence:


On 12.01.2015 14:21, Dirk Kostrewa wrote:
If, however, the unmodelled part is less well ordered (which is the 
more common case), it's contribution will mainly affect the model's 
Fcalc at low resolution. If the overall scaling is dominated by the 
high resolution terms (which is usually the case), the unmodelled part 
will not have an effect on the overall scale factor of the model's 
Fcalc, leaving only the Fcalc at low resolution somewhat too low. 
Since lowering the model's Fcalc scale factor at low resolution is the 
main purpose of the Babinet solvent correction, this will lead to an 
_underestimation_ (!) of the Babinet bulk solvent contribution scale 
factor (ksol). This, in principle, should increase, or overestimate, 
the signal of the difference densities at low resolution, which might 
also help with interpretation of the unmodelled part.


The underestimation of the Babinet bulk solvent scale factor is 
equivalent to an overestimation of the contrast between protein and 
solvent and should therefore lead to an overestimation of the Fcalc at 
low resolution. If scaling is still dominated by the high resolution 
terms, this should lead to a decrease, or underestimation, of the 
structure factor differences at low resolution, which would reduce the 
overall signal of the difference densities. But still, this will be an 
overall effect and not restricted to the location of the unmodelled part.


Best regards,

Dirk.

--

***
Dirk Kostrewa
Gene Center Munich, A5.07
Department of Biochemistry
Ludwig-Maximilians-Universität München
Feodor-Lynen-Str. 25
D-81377 Munich
Germany
Phone:  +49-89-2180-76845
Fax:+49-89-2180-76999
E-mail: kostr...@genzentrum.lmu.de
WWW:www.genzentrum.lmu.de
***



Re: [ccp4bb] Bulk solvent

2015-01-09 Thread Dirk Kostrewa

On 09.01.2015 08:56, Armando Albert wrote:

Dear all,
Is there any reason for using Babinet scaling for bulk solvent correction 
instead of mask based scaling?
Armando


Dear Armando,

yes: the mask bulk solvent correction depends on the proper calculation 
of a protein mask. The bulk solvent density is then assigned outside the 
protein mask. This mask calculation is based on one or two radii around 
the protein atoms and is always a compromise. Sometimes, the protein 
mask misses really empty cavities usually surrounded by hydrophobic 
residues, wrongly filling these cavities with bulk solvent density. This 
results in relatively large blobs with negative difference density. 
Sometimes, the protein mask covers narrow cavities really filled with 
bulk solvent electron density, which is then missing in the model. This 
results in positive difference densities, that are not easy to 
interpret. The Babinet bulk solvent correction only uses two parameters, 
is less effective in describing the contribution of the bulk solvent to 
the scattering, but is free of these artefacts. I use the Babinet bulk 
solvent correction sometimes as a control if I'm not sure about the 
origin of possibly important difference density peaks in narrow regions.


Best regards,

Dirk.

--

***
Dirk Kostrewa
Gene Center Munich, A5.07
Department of Biochemistry
Ludwig-Maximilians-Universität München
Feodor-Lynen-Str. 25
D-81377 Munich
Germany
Phone:  +49-89-2180-76845
Fax:+49-89-2180-76999
E-mail: kostr...@genzentrum.lmu.de
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***


Re: [ccp4bb] twin or untwinned

2014-07-03 Thread Dirk Kostrewa
... and please check, whether phenix.xtriage recognized the input data 
as intensities or as amplitudes.
In case of doubt, convert the intensives first into an mtz file with Fs 
instead of Is and run phenix.xtriage on the mtz file.


Best regards,

Dirk.

Am 03.07.2014 13:36, schrieb Tim Gruene:

Hi Yamei,

did you by any chance feed the output file from XDS into xtriage? It
would indicate the data were twinned even for a near perfect insulin
test crystal. After discussion with the developers I understand that
phenix does not seem to handle unmerged data well.

With phenix.xtriage V. phenix-1.9-1692:, XDS_ASCII.HKL
   Mean |L|   :0.392  (untwinned: 0.500; perfect twin: 0.375)
   Mean  L^2  :0.219  (untwinned: 0.333; perfect twin: 0.200)

after pointless and merging with aimless:
   Mean |L|   :0.492  (untwinned: 0.500; perfect twin: 0.375)
   Mean  L^2  :0.322  (untwinned: 0.333; perfect twin: 0.200)

As workaround, run the data through pointless/aimless first.

Best,
Tim

On 07/03/2014 05:04 AM, Yamei Yu wrote:

HI all,

I have a data set processed to P42 21 2 (the space group was suggested by 
pointless ). then I use phenix.xtriage to analysis the data. I was confused by 
the phenix.xtriage result.
According to the following number it is twin data, but why it couldn’t find any 
possible twin law?

Determining possible twin laws.

   0 merohedral twin operators found
   0 pseudo-merohedral twin operators found
In total,   0 twin operator were found


  Mean |L|   :0.378  (untwinned: 0.500; perfect twin: 0.375)
   Mean  L^2  :0.205  (untwinned: 0.333; perfect twin: 0.200)


How could be that? Is it twin or no twin?

Please find the log file of phenix.xtrage in attachment.

Thank you so much for your suggestion!




Yamei Yu




--

***
Dirk Kostrewa
Gene Center Munich, A5.07
Department of Biochemistry
Ludwig-Maximilians-Universität München
Feodor-Lynen-Str. 25
D-81377 Munich
Germany
Phone:  +49-89-2180-76845
Fax:+49-89-2180-76999
E-mail: kostr...@genzentrum.lmu.de
WWW:www.genzentrum.lmu.de
***


Re: [ccp4bb] twin or untwinned

2014-07-03 Thread Dirk Kostrewa

Hi Tim,

yes - unfortunately, in my hands, phenix.xtriage reads the XDS_ASCII.HKL 
intensities as amplitudes, producing very different output statistics, 
compared both to the XDS statistics and to an mtz file with amplitudes 
created from that XDS file. I've contacted a phenix developer a few 
weeks ago, but got no reply, yet (maybe, my e-mail got lost).


Cheers,

Dirk.

Am 03.07.2014 13:46, schrieb Tim Gruene:

Hi Dirk,

that would truely be very sad - the XDS file format is such a beautiful,
self-contained and well documented format for diffraction data that a
misinterpretation should really not happen.

Cheers,
Tim

On 07/03/2014 01:42 PM, Dirk Kostrewa wrote:

... and please check, whether phenix.xtriage recognized the input data
as intensities or as amplitudes.
In case of doubt, convert the intensives first into an mtz file with Fs
instead of Is and run phenix.xtriage on the mtz file.

Best regards,

Dirk.

Am 03.07.2014 13:36, schrieb Tim Gruene:

Hi Yamei,

did you by any chance feed the output file from XDS into xtriage? It
would indicate the data were twinned even for a near perfect insulin
test crystal. After discussion with the developers I understand that
phenix does not seem to handle unmerged data well.

With phenix.xtriage V. phenix-1.9-1692:, XDS_ASCII.HKL
Mean |L|   :0.392  (untwinned: 0.500; perfect twin: 0.375)
Mean  L^2  :0.219  (untwinned: 0.333; perfect twin: 0.200)

after pointless and merging with aimless:
Mean |L|   :0.492  (untwinned: 0.500; perfect twin: 0.375)
Mean  L^2  :0.322  (untwinned: 0.333; perfect twin: 0.200)

As workaround, run the data through pointless/aimless first.

Best,
Tim

On 07/03/2014 05:04 AM, Yamei Yu wrote:

HI all,

 I have a data set processed to P42 21 2 (the space group was
suggested by pointless ). then I use phenix.xtriage to analysis the
data. I was confused by the phenix.xtriage result.
According to the following number it is twin data, but why it
couldn’t find any possible twin law?

Determining possible twin laws.

0 merohedral twin operators found
0 pseudo-merohedral twin operators found
In total,   0 twin operator were found


   Mean |L|   :0.378  (untwinned: 0.500; perfect twin: 0.375)
Mean  L^2  :0.205  (untwinned: 0.333; perfect twin: 0.200)


How could be that? Is it twin or no twin?

Please find the log file of phenix.xtrage in attachment.

Thank you so much for your suggestion!




Yamei Yu




--

***
Dirk Kostrewa
Gene Center Munich, A5.07
Department of Biochemistry
Ludwig-Maximilians-Universität München
Feodor-Lynen-Str. 25
D-81377 Munich
Germany
Phone:  +49-89-2180-76845
Fax:+49-89-2180-76999
E-mail: kostr...@genzentrum.lmu.de
WWW:www.genzentrum.lmu.de
***


Re: [ccp4bb] twinning fun

2014-01-28 Thread Dirk Kostrewa

Dear Bert Van-Den-Berg,

as far as I understand this, if you have true P622, process the data in 
P6 and then test for twinning, both the Britton-test and H-test will 
indicate perfect merohedral twinning.
This is because the Britton-test checks for a sudden increase of 
negative intensities after de-twinning, which happens only at twin 
fractions close to 0.5 if the intensities used for de-twinning are the 
same. But this is true if they are related by crystallographic symmetry.
The H-test relates the absolute difference to the sum of the presumably 
twinned intensities, which gives 0 for intensities related by 
crystallographic symmetry, again resulting in twin fractions close to 0.5.
In other words, intensities related by crystallographic symmetry would 
indicate perfect twinning in both of these tests.


A better test for perfect merohedral twinning would be the ratio of 
I^2/I^2 which should be 2 for untwinned and 1.5 for perfectly 
twinned data, tested in the higher space group. These values are 
reported by data processing programs like XDS. Please, be aware that 
these ratios have rather strange values if you have an unusually high 
background (loop fiber diffraction, ice rings, etc.) or extremely weak data.


For a really good discussion of twin tests, see Yeates, Methods. 
Enzymol. 276, 344-358, 1997.


Best regards,

Dirk.

Am 28.01.14 18:26, schrieb Bert Van-Den-Berg:

Dear all,

I recently collected several datasets for a protein that needs 
experimental phasing.
The crystals are hexagonal plates, and (automatic) data processing 
suggests with high confidence that the space group is P622. This is 
where the fun begins.
For some datasets (processed in P622), the intensity distributions are 
normal, and the L-test (aimless, xtriage) and Z-scores (xtriage) 
suggest that there is no twinning (twinning fractions  0.05). 
However, for other datasets (same cell dimensions), the intensity 
distributions are not normal (eg Z-scores  10). Given that twinning 
is not possible in P622, this suggests to me that the real space group 
could be P6 with (near) perfect twinning.


If I now process the normal L-test P622 datasets in P6, the twin-law 
based tests (britton and H-test in xtriage) give high twin fractions 
(0.45- 0.5), suggesting all my data is twinned.
Does this make sense (ie can one have twinning with normal intensity 
distributions)?
If it does, would the normal L-test datasets have a higher 
probability of being solvable?


Is there any strategy for experimental phasing of (near) perfect 
twins? SAD would be more suitable than SIR/MIR? (I also have potential 
heavy atom derivatives).


Thanks for any insights!

Bert


--

***
Dirk Kostrewa
Gene Center Munich, A5.07
Department of Biochemistry
Ludwig-Maximilians-Universität München
Feodor-Lynen-Str. 25
D-81377 Munich
Germany
Phone:  +49-89-2180-76845
Fax:+49-89-2180-76999
E-mail: kostr...@genzentrum.lmu.de
WWW:www.genzentrum.lmu.de
***



Re: [ccp4bb] Fractional coordinate shift with two-character chain names?

2013-09-02 Thread Dirk Kostrewa

Dear Martyn, Pavel and other interested,

I think, an official extension by the PDB to two characters for the 
chain names and 5 digits for residues would really help. I'm currently 
working on a structure with 6x15 chains (through NCS) - it is huge and 
only a few programs can handle this by extending the PDB format.
The last PDB format revision 3.3 
http://www.wwpdb.org/documentation/format33/sect9.html#ATOM still only 
allows one character for the chain name and four digits for the residue 
number.
More bigger structures will be published in the future and an official 
human-readable extended PDB format would really help.


Cheers,

Dirk.


Am 30.08.13 18:14, schrieb MARTYN SYMMONS:

Hold your horsemen!
Does not this option save us from 'formatagedon'?
We currently only have single letters or numbers for chains. But we 
could easily agree to switch to double letters. And long chains can be 
a sequence of letter number permutations such as A1, A2, A3 etc 
(actually I notice single numbers are allowed for the PDB - although 
are deprecated until all the letters have been used).
We could allow the first character to be a number as well - so 11 12 
13 as a valid sequence.for a single polymer.
Conversely we could expand the atom identifier to include letters as 
is the case with most computing identifiers - however not many 
programs seem to pay attention to the atom 'numbers' in any case.


Cheers
  Martyn

Martyn Symmons (not Winn)
Cambridge


*From:* Dirk Kostrewa kostr...@genzentrum.lmu.de
*To:* CCP4BB@JISCMAIL.AC.UK
*Sent:* Friday, 30 August 2013, 15:36
*Subject:* Re: [ccp4bb] Fractional coordinate shift with two-character 
chain names?


Hi Martyn,

excellent - this worked!

Many thanks!

Cheers,

Dirk.

Am 30.08.13 16:04, schrieb Martyn Winn:
 IIRC the CCP4 library (i.e. mmdb) can handle 2-character chain 
names. There may be something specific in pdbset which interferes. You 
can try pdbcur as an alternative. Something like:


 pdbcur xyzin toxd_AA.pdb xyzout toxd_out.pdb eof
 translate * frac 0 0.2 0
 end
 eof

 I just tried it on a little example, and it works for me.

 Cheers
 Martyn

 -Original Message-
 From: CCP4 bulletin board [mailto:CCP4BB@JISCMAIL.AC.UK 
mailto:CCP4BB@JISCMAIL.AC.UK] On Behalf Of

 Dirk Kostrewa
 Sent: 30 August 2013 14:41
 To: ccp4bb
 Subject: [ccp4bb] Fractional coordinate shift with two-character chain
 names?

 Dear CCP4ers,

 I want to apply a fractional coordinate shift along a polar b-axis with
 coordinates that have non-standard two-character chain names, such as
 AA, AB, and so forth. Unfortunately, neither the old USF moleman2
 nor the actual CCP4 pdbset can handle these chain names. To my
 knowledge, only COOT and PHENIX can cope with them.
 Before I start writing my own little jiffy, is there a quick way to use
 COOT or PHENIX to apply a fractional coordinate shift, or could you
 tell me, which other program I can use in this special case?

 Best regards,

 Dirk.

 --

 ***
 Dirk Kostrewa
 Gene Center Munich
 Department of Biochemistry
 Ludwig-Maximilians-Universität München
 Feodor-Lynen-Str. 25
 D-81377 Munich
 Germany
 Phone: +49-89-2180-76845
 Fax: +49-89-2180-76999
 E-mail: kostr...@genzentrum.lmu.de mailto:kostr...@genzentrum.lmu.de
 WWW:www.genzentrum.lmu.de
 ***

--

***
Dirk Kostrewa
Gene Center Munich
Department of Biochemistry
Ludwig-Maximilians-Universität München
Feodor-Lynen-Str. 25
D-81377 Munich
Germany
Phone: +49-89-2180-76845
Fax: +49-89-2180-76999
E-mail: kostr...@genzentrum.lmu.de mailto:kostr...@genzentrum.lmu.de
WWW:www.genzentrum.lmu.de
***




--

***
Dirk Kostrewa
Gene Center Munich
Department of Biochemistry
Ludwig-Maximilians-Universität München
Feodor-Lynen-Str. 25
D-81377 Munich
Germany
Phone:  +49-89-2180-76845
Fax:+49-89-2180-76999
E-mail: kostr...@genzentrum.lmu.de
WWW:www.genzentrum.lmu.de
***



[ccp4bb] Fractional coordinate shift with two-character chain names?

2013-08-30 Thread Dirk Kostrewa

Dear CCP4ers,

I want to apply a fractional coordinate shift along a polar b-axis with 
coordinates that have non-standard two-character chain names, such as 
AA, AB, and so forth. Unfortunately, neither the old USF moleman2 
nor the actual CCP4 pdbset can handle these chain names. To my 
knowledge, only COOT and PHENIX can cope with them.
Before I start writing my own little jiffy, is there a quick way to use 
COOT or PHENIX to apply a fractional coordinate shift, or could you tell 
me, which other program I can use in this special case?


Best regards,

Dirk.

--

***
Dirk Kostrewa
Gene Center Munich
Department of Biochemistry
Ludwig-Maximilians-Universität München
Feodor-Lynen-Str. 25
D-81377 Munich
Germany
Phone:  +49-89-2180-76845
Fax:+49-89-2180-76999
E-mail: kostr...@genzentrum.lmu.de
WWW:www.genzentrum.lmu.de
***


Re: [ccp4bb] Fractional coordinate shift with two-character chain names?

2013-08-30 Thread Dirk Kostrewa

Hi Martyn,

excellent - this worked!

Many thanks!

Cheers,

Dirk.

Am 30.08.13 16:04, schrieb Martyn Winn:

IIRC the CCP4 library (i.e. mmdb) can handle 2-character chain names. There may 
be something specific in pdbset which interferes. You can try pdbcur as an 
alternative. Something like:

pdbcur xyzin toxd_AA.pdb xyzout toxd_out.pdb eof
translate * frac 0 0.2 0
end
eof

I just tried it on a little example, and it works for me.

Cheers
Martyn


-Original Message-
From: CCP4 bulletin board [mailto:CCP4BB@JISCMAIL.AC.UK] On Behalf Of
Dirk Kostrewa
Sent: 30 August 2013 14:41
To: ccp4bb
Subject: [ccp4bb] Fractional coordinate shift with two-character chain
names?

Dear CCP4ers,

I want to apply a fractional coordinate shift along a polar b-axis with
coordinates that have non-standard two-character chain names, such as
AA, AB, and so forth. Unfortunately, neither the old USF moleman2
nor the actual CCP4 pdbset can handle these chain names. To my
knowledge, only COOT and PHENIX can cope with them.
Before I start writing my own little jiffy, is there a quick way to use
COOT or PHENIX to apply a fractional coordinate shift, or could you
tell me, which other program I can use in this special case?

Best regards,

Dirk.

--

***
Dirk Kostrewa
Gene Center Munich
Department of Biochemistry
Ludwig-Maximilians-Universität München
Feodor-Lynen-Str. 25
D-81377 Munich
Germany
Phone:  +49-89-2180-76845
Fax:+49-89-2180-76999
E-mail: kostr...@genzentrum.lmu.de
WWW:www.genzentrum.lmu.de
***


--

***
Dirk Kostrewa
Gene Center Munich
Department of Biochemistry
Ludwig-Maximilians-Universität München
Feodor-Lynen-Str. 25
D-81377 Munich
Germany
Phone:  +49-89-2180-76845
Fax:+49-89-2180-76999
E-mail: kostr...@genzentrum.lmu.de
WWW:www.genzentrum.lmu.de
***


Re: [ccp4bb] Advise on setting up/ maintaining a Ubuntu cluster

2013-07-31 Thread Dirk Kostrewa

We have a very similar setup, and I can only second Kay's experience.

Best regards,

Dirk.


Am 31.07.13 13:36, schrieb Kay Diederichs:

I have a very different experience with NFS: we are using Gigabit Ethernet, and 
a 64bit RHEL6 clone with ECC memory as a file server; it has RAID1 ext4 home 
directories and RAID6 ext4 for synchrotron data. We have had zero performance 
or reliability problems with this in a computer lab with ~ 10 workstations, and 
I have seen 115 MB/sec file transfers via NFS, at peak times.
Just make sure to export using the async option.

HTH,

Kay

On Wed, 31 Jul 2013 09:21:48 +0900, Francois Berenger beren...@riken.jp wrote:


Be careful that running data intensive jobs over NFS
is super slow (at least an order of magnitude compared
to writing things on a local disk).
Not only the computation is slow, but you may be slowing down
all other users of the cluster too...

F.


--

***
Dirk Kostrewa
Gene Center Munich
Department of Biochemistry
Ludwig-Maximilians-Universität München
Feodor-Lynen-Str. 25
D-81377 Munich
Germany
Phone:  +49-89-2180-76845
Fax:+49-89-2180-76999
E-mail: kostr...@genzentrum.lmu.de
WWW:www.genzentrum.lmu.de
***


Re: [ccp4bb] Concerns about statistics

2013-06-14 Thread Dirk Kostrewa

Dear Andrea,

I agree with Tim and still cut the resolution at I/sigma=2. In my 
experience, including higher resolution shells with poorer 
signal-to-noise never changed the apparent resolution of the electron 
density maps.
In addition, the high resolution limit at I/sigma=2 coincides very 
well with the point where the Fo vs. Fo +Gauss(0,1)*sigma(Fo) 
correlation coefficient curve, reported by BUSTER, crosses the 
recommended lower limit of 0.9.


And please note, CC*=0.5 corresponds to CC(1/2)=0.143. In my very 
limited experience, I/sigma=2 corresponds to roughly CC(1/2)~0.7.


Although I'm very excited about the CC(1/2) or CC* paper by Karplus  
Diederichs, I still prefer to be on the save side, until it has been 
verified in numerous cases, that choosing high resolution cutoffs based 
on CC(1/2) really leads to higher resolution structures. The recommended 
procedure to include small resolution increments in refinement to decide 
the high resolution cutoff is very time-consuming.


Best regards,

Dirk.


Am 13.06.13 17:15, schrieb Andrea Edwards:

Hello group,
I have some rather (embarrassingly) basic questions to ask. Mainly.. when 
deciding the resolution limit, which statistics are the most important? I have 
always been taught that the highest resolution bin should be chosen with I/sig 
no less than 2.0, Rmerg no less than 40%, and %Completeness should be as high 
as possible. However, I am currently encountered with a set of statistics that 
are clearly outside this criteria. Is it acceptable cut off resolution using 
I/sig as low as 1.5 as long as the completeness is greater than 75%? Another 
way to put this.. if % completeness is the new criteria for choosing your 
resolution limit (instead of Rmerg or I/sig), then what %completeness is too 
low to be considered? Also, I am aware that Rmerg increases with redundancy, is 
it acceptable to report Rmerg (or Rsym) at 66% and 98% with redundancy at 3.8 
and 2.4 for the highest resolution bin of these crystals? I appreciate any 
comments.
-A


--

***
Dirk Kostrewa
Gene Center Munich
Department of Biochemistry
Ludwig-Maximilians-Universität München
Feodor-Lynen-Str. 25
D-81377 Munich
Germany
Phone:  +49-89-2180-76845
Fax:+49-89-2180-76999
E-mail: kostr...@genzentrum.lmu.de
WWW:www.genzentrum.lmu.de
***


[ccp4bb] Single-Gaussian Atomic Scattering Factors?

2012-11-28 Thread Dirk Kostrewa

Dear colleagues,

for a very simple calculation, I want to use a single-Gaussian atomic 
scattering factor approximation (for nitrogen). I only find 2- or 
5-Gaussian approximations. Could you please give me a pointer to values 
of single-Gaussian atomic scattering factor approximations?


Best regards,

Dirk.

--

***
Dirk Kostrewa
Gene Center Munich
Department of Biochemistry
Ludwig-Maximilians-Universität München
Feodor-Lynen-Str. 25
D-81377 Munich
Germany
Phone:  +49-89-2180-76845
Fax:+49-89-2180-76999
E-mail: kostr...@genzentrum.lmu.de
WWW:www.genzentrum.lmu.de
***


[ccp4bb] Coot Release 0.7 in CCP4 Software Update?

2012-10-01 Thread Dirk Kostrewa

Dear CCP4 developers,

this question might be interesting for many CCP4/Coot users:

will the Coot release 0.7 and future releases be made available to CCP4 
users via the CCP4 software update?


Best regards,

Dirk.


 Original-Nachricht 
Betreff:[COOT] Release 0.7
Datum:  Sat, 29 Sep 2012 10:49:45 +0100
Von:Paul Emsley paul.ems...@bioch.ox.ac.uk
Antwort an: Paul Emsley paul.ems...@bioch.ox.ac.uk
An: c...@jiscmail.ac.uk



Hi Coot-users,

We are pleased to announce Release 0.7 of Coot.

Source:

http://lmb.bioch.ox.ac.uk/coot/software/source/releases/coot-0.7.tar.gz

Binaries:

http://lmb.bioch.ox.ac.uk/coot/software/binaries/releases/

Mac 10.8:

http://psbmini.ucsc.edu/~wgscott/coot/stablereleases/Coot-0.7-stable_64bit_10.8.2.pkg.zip


Now stick a fork in me (as they say)...

Paul.


A few notes:

  o FEATURE: RCrane [RNA builder]

  o FEATURE: Cootaneer [RNA builder]

  o FEATURE: Het-groups are now represented with bond orders.

  o FEATURE: Ligand Builder - working in conjunction with cprodrg.

  o FEATURE: JLigand interface.

  o CHANGE: symmetry operator number are no longer zero indexed. Add
trans component to symmetry file names.

  o CHANGE: Dotted surfaces now are coloured by atom type and are at
atomic radii rather than 1A.

  o CHANGE: map transformation no longer has symmetry overwrite
problems.


--

***
Dirk Kostrewa
Gene Center Munich
Department of Biochemistry
Ludwig-Maximilians-Universität München
Feodor-Lynen-Str. 25
D-81377 Munich
Germany
Phone:  +49-89-2180-76845
Fax:+49-89-2180-76999
E-mail: kostr...@genzentrum.lmu.de
WWW:www.genzentrum.lmu.de
***





smime.p7s
Description: S/MIME Kryptografische Unterschrift


Re: [ccp4bb] Coot Release 0.7 in CCP4 Software Update?

2012-10-01 Thread Dirk Kostrewa

Dear Eugene,

thank you for your kind reply and your explanation!

Since the CCP4 download site offers Coot either as a stand-alone-package 
or via the new package manager, I was hoping that new Coot releases 
could also be handled by the wonderful CCP4 software update.


A software update mechanism for Coot, be it part of CCP4 or part of 
Coot, would help the software administrator :-).


A related question just crossed my mind: when will Coot and CCP4mg 
become part of the CCP4 core packages?


Best regards,

Dirk.

P.S.: I've sent Paul Emsley a CC of this little conversation.


Am 01.10.12 13:13, schrieb eugene.krissi...@stfc.ac.uk:

Thanks for nice question.

Currently, CCP4 update is applicable only to what is distributed as CCP4 core, which 
guarantees a definite location in $CCP4 directory. Also, updates are not supposed to deliver 
releases (upgrades), but rather smallish changes between them.

Coot is not part of CCP4 core, and in fact, is distributed in many different 
ways, therefore, CCP4 update mechanism cannot be applied to Coot 
straightforwardly, and it is unlikely to be applicable to Coot upgrades (e.g., 
0.7 to 08).

However, the updater may be made a part of Coot package, which is something 
completely doable in principle, in which case it can deliver fixes for current 
release.

Eugene


On 1 Oct 2012, at 09:46, Dirk Kostrewa wrote:

Dear CCP4 developers,

this question might be interesting for many CCP4/Coot users:

will the Coot release 0.7 and future releases be made available to CCP4 users 
via the CCP4 software update?

Best regards,

Dirk.


 Original-Nachricht 
Betreff:[COOT] Release 0.7
Datum:  Sat, 29 Sep 2012 10:49:45 +0100
Von:Paul Emsley 
paul.ems...@bioch.ox.ac.ukmailto:paul.ems...@bioch.ox.ac.uk
Antwort an: Paul Emsley 
paul.ems...@bioch.ox.ac.ukmailto:paul.ems...@bioch.ox.ac.uk
An: c...@jiscmail.ac.ukmailto:c...@jiscmail.ac.uk



Hi Coot-users,

We are pleased to announce Release 0.7 of Coot.

Source:

http://lmb.bioch.ox.ac.uk/coot/software/source/releases/coot-0.7.tar.gz

Binaries:

http://lmb.bioch.ox.ac.uk/coot/software/binaries/releases/

Mac 10.8:

http://psbmini.ucsc.edu/~wgscott/coot/stablereleases/Coot-0.7-stable_64bit_10.8.2.pkg.zip


Now stick a fork in me (as they say)...

Paul.


A few notes:

   o FEATURE: RCrane [RNA builder]

   o FEATURE: Cootaneer [RNA builder]

   o FEATURE: Het-groups are now represented with bond orders.

   o FEATURE: Ligand Builder - working in conjunction with cprodrg.

   o FEATURE: JLigand interface.

   o CHANGE: symmetry operator number are no longer zero indexed. Add
 trans component to symmetry file names.

   o CHANGE: Dotted surfaces now are coloured by atom type and are at
 atomic radii rather than 1A.

   o CHANGE: map transformation no longer has symmetry overwrite
 problems.



--

***
Dirk Kostrewa
Gene Center Munich
Department of Biochemistry
Ludwig-Maximilians-Universität München
Feodor-Lynen-Str. 25
D-81377 Munich
Germany
Phone:  +49-89-2180-76845
Fax:+49-89-2180-76999
E-mail: kostr...@genzentrum.lmu.demailto:kostr...@genzentrum.lmu.de
WWW:www.genzentrum.lmu.dehttp://www.genzentrum.lmu.de/
***







--

***
Dirk Kostrewa
Gene Center Munich
Department of Biochemistry
Ludwig-Maximilians-Universität München
Feodor-Lynen-Str. 25
D-81377 Munich
Germany
Phone:  +49-89-2180-76845
Fax:+49-89-2180-76999
E-mail: kostr...@genzentrum.lmu.de
WWW:www.genzentrum.lmu.de
***




smime.p7s
Description: S/MIME Kryptografische Unterschrift


Re: [ccp4bb] Which Coot for Scientific Linux 6.3

2012-09-20 Thread Dirk Kostrewa

Dear Fred  David,

the new CCP4 Package Manager works perfectly on SL 6.3, as does the 
wonderful new CCP4 Update program!


The file command for the coot-real executable (version 0.6.2) tells me:

ELF 64-bit LSB executable, x86-64, version 1 (SYSV), dynamically linked 
(uses shared libs), for GNU/Linux 2.6.9, not stripped


I hope that helps a little bit.

Best regards,

Dirk.


Am 20.09.12 14:37, schrieb David Waterman:

Dear Fred,

You may like to try the CCP4 Package Manager, available from the 
downloads page: http://www.ccp4.ac.uk/download/#os=linux


This allows installation of CCP4 components, including Coot, 
automatically and will attempt to identify the appropriate version for 
you (disclaimer: I have not tried this on SL 6.3, so can't tell you in 
advance what you'll get)


Cheers

-- David


On 19 September 2012 17:12, Fred. Vellieux frederic.velli...@ibs.fr 
mailto:frederic.velli...@ibs.fr wrote:


Hi all,

The question is in the Subject line of this email: which version
of Coot
should I download and install on a Scientific Linux 6.3 box ?

Ta very much in advance,

F.V.

--
F.M.D. Vellieux (B.Sc., Ph.D., hdr)
IBS / ELMA
41 rue Jules Horowitz
38027 Grenoble Cedex 01
France
Tel: +33 438789605 tel:%2B33%20438789605
Fax: +33 438785494 tel:%2B33%20438785494




--

***
Dirk Kostrewa
Gene Center Munich
Department of Biochemistry
Ludwig-Maximilians-Universität München
Feodor-Lynen-Str. 25
D-81377 Munich
Germany
Phone:  +49-89-2180-76845
Fax:+49-89-2180-76999
E-mail: kostr...@genzentrum.lmu.de
WWW:www.genzentrum.lmu.de
***



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Description: S/MIME Kryptografische Unterschrift


Re: [ccp4bb] CNS installation

2012-07-12 Thread Dirk Kostrewa

Dear Fulvio Saccoccia,

along the lines of Ian Tickle's reply: there should be a script 
cns_solve_env_sh using /bin/sh, which is usually a soft-link to 
/bin/bash. I use this script for setup of CNS under bash.


Best regards,

Dirk.

Am 12.07.12 16:49, schrieb fulvio saccoccia:

Dear ccp4 users,
I tried to install CNS under Debian 64bit. I followed the installation
giude as reported by CNS developers but  I received the following
message when souurcing cns_solve_env:

bash: setenv: command not found
bash: setenv: command not found
bash: cns_solve_env: line 32: syntax error near unexpected token
`setenv'
bash: cns_solve_env: line 32: `  if ( ! $?CNS_ARCH ) setenv CNS_ARCH `
$CNS_SOLVE/bin/getarch`'

I know that the script would set all variables; it is indicated for csh
(or tcsh) shell. I tried to run the script under a csh shell but I
received a different error:

Word too long

The above statement is also received if a bash-optimized script is run.

Does anyone have experience in CNS installation and environment setting?
Any advice?

Thanks in advance

Fulvio Saccoccia
Dept. of Biochemical Sciences
Sapienza University of Rome, Italy


--

***
Dirk Kostrewa
Gene Center Munich
Department of Biochemistry
Ludwig-Maximilians-Universität München
Feodor-Lynen-Str. 25
D-81377 Munich
Germany
Phone:  +49-89-2180-76845
Fax:+49-89-2180-76999
E-mail: kostr...@genzentrum.lmu.de
WWW:www.genzentrum.lmu.de
***


Re: [ccp4bb] bulk solvent treatment inside protein cavities

2012-04-17 Thread Dirk Kostrewa

Dear Allister Crow,

in cases like these, I would recommend to apply the Babinet bulk solvent 
correction instead of the mask bulk solvent correction as a control 
(Refmac5 - Scaling - Use Babinet scaling; uncheck Calculcate the 
contribution from the solvent region). The Babinet bulk solvent 
correction only uses two overall scaling factors and is usually simple, 
robust and, in my experience, does not show any local difference density 
artefacts. The mask bulk solvent correction is more powerful, but, 
depending on the project and the various mask radii for generating and 
shrinking the mask, could produce false positive or negative difference 
density. To exclude these cases, you can always calculate the Babinet 
bulk solvent correction as a control.


Best regards,

Dirk.

Am 16.04.12 12:37, schrieb Allister Crow:

Board members,

I have a couple of questions regarding how to improve the solvent model as 
applied to solvent-filled cavities inside proteins.

I am currently nearing the end of refinement of a protein structure at 2.8 A 
resolution.  I recently switched Refmac versions, upon doing this I noticed a 
modest improvement in R factors, but I also notice some new features in the 
difference maps.  These features don't show up in the sigma-weighted 2Fo-Fc 
maps and are unlikely to be 'ligands' of any form.  In fact, I suspect that the 
appearance of these features (which are all located in solvent channels within 
cavities inside the protein) are probably due to some difference in how the 
bulk solvent contribution has been applied.

I've attached a picture of one such feature showing the difference between 
Refmac 5.5 and 5.6.  (Both difference maps are contoured at 3 sigma- both using 
the same model and refinement parameters).

My questions are therefore:

1) has something substantial changed in the bulk solvent treatment between 
Refmac versions 5.5 and 5.6?

2) How can I go about changing the bulk solvent treatment to better account for 
solvent contribution inside the protein cavities?

Best wishes, and thanks in advance for all your help,

- Allister Crow








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Phone:  +49-89-2180-76845
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Re: [ccp4bb] proper or improper ncs?

2012-02-21 Thread Dirk Kostrewa

Hi Francis,

a quick insertion of your rotation matrix into CONVROT (by Alexandre 
Urzhumtsev) gives the following equivalent polar rotation angles 
(definition as in X-PLOR/CNS or Rossmann, 1962):


phi,psi,kappa   :  111.86  128.68  133.38 291.86   51.32  226.62

For a proper two-fold, a kappa of 180 degrees would be expected. This 
looks (very) improper to me.


Best regards,

Dirk.

Am 21.02.12 14:47, schrieb Francis E Reyes:

Hi all

This structure has the following ncs (output via phenix.simple_ncs_from_pdb)
OPERATOR 1
CENTER:   18.3443  -55.4605   23.0986

ROTA 1:1.0.0.
ROTA 2:0.1.0.
ROTA 3:0.0.1.
TRANS: 0.0.0.

OPERATOR 2
CENTER:   37.0405  -23.8676  -14.9388

ROTA 1:   -0.5444   -0.22020.8094
ROTA 2:0.8330   -0.02780.5526
ROTA 3:   -0.09910.97510.1985
TRANS:45.3456  -78.7231   53.0085


It looks two-foldish but I'm not sure if it's proper or improper. (I'm trying 
to rationalize the lack of peaks on the self rotation maps).


Any help would be appreciated.

F



-
Francis E. Reyes M.Sc.
215 UCB
University of Colorado at Boulder


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***
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Re: [ccp4bb] Freezing crystal

2012-02-07 Thread Dirk Kostrewa

Dear Jürgen,

Am 07.02.12 16:58, schrieb Bosch, Juergen:
snip
Then one last remark, LN2 versus cryo-stream freeze. Dipping in LN2 
leads to a quicker freeze of your material.

/snip

Are you sure? There was a publication by Warkentin et al. [1] about a 
cold gas layer above liquid nitrogen that reduces the expected cooling 
rate a lot!
My very personal experience is, that cryo-cooling in the N2-stream 
worked better for me than in LN2 in a variety of projects - but the 
reason could just be me ;-)


Best regards,

Dirk.

[1] Matthew Warkentin, Viatcheslav Berejnov, Naji S Husseini, and Robert 
E Thorne: Hyperquenching for protein cryocrystallography, J. Appl. 
Crystallogr., 39, 805-811 (2006)


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Phone:  +49-89-2180-76845
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Re: [ccp4bb] NMR review

2012-01-12 Thread Dirk Kostrewa

Dear Bernhard,

Am 12.01.12 10:30, schrieb Bernhard Rupp (Hofkristallrat a.D.):

Dear All,

I read an interesting statement in an NMR review:

 regions of a protein or
DNA ⁄ RNA molecule that are flexible in the crystal do
not provide coherent X-ray scattering and hence do
not contribute to the final electron density map. Thus,
for all intents and purposes, they can effectively be
ignored.

Besides that I was not aware that disorder across molecules implies incoherence
in scattering, I think this is quite some strong tobacco coming from what is
primarily a crystallization screening tool ;-)
That doesn't sound wrong to me: the flexible parts are at different 
relative positions in the unit cells and thus their partial-structure 
scattering waves do not have a constant phase relation to each other, 
i.e., they don't give a coherent contribution to the total scattering.


But I don't agree to their conclusion, since disorder doesn't 
necessarily mean, that there won't be any interpretable electron density 
left. The floppy parts could still be interpreted at an effective lower 
resolution and thus will not be ignored.


Maybe the authors were annoyed by a vanishing NMR signal because the 
macromolecule crystallized in the NMR test tube ;-)


Best regards,

Dirk.


Cheers, BR

PS: I am grappling with the meaning of resolution in NMR. I can see that it
could be related to comparable data/parameter ratios, although I am even
less clear about the weights of NMR restraint weights than in the case of MX...
some cross-trained person out there who can explain?


--

***
Dirk Kostrewa
Gene Center Munich
Department of Biochemistry
Ludwig-Maximilians-Universität München
Feodor-Lynen-Str. 25
D-81377 Munich
Germany
Phone:  +49-89-2180-76845
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Re: [ccp4bb] NMR review

2012-01-12 Thread Dirk Kostrewa
My understanding of coherence is a constant phase relation between 
waves. Of course, this breaks down for inelastic scattering, but 
(in)coherence can also be described without any change in wavelength.


Best regards,

Dirk.

Am 12.01.12 11:27, schrieb Bernhard Rupp (Hofkristallrat a.D.):

Does out of phase imply incoherent scattering? I though it means inelastic 
Compton scattering?

-Original Message-
From: CCP4 bulletin board [mailto:CCP4BB@JISCMAIL.AC.UK] On Behalf Of Dirk 
Kostrewa
Sent: Thursday, January 12, 2012 1:58 AM
To: CCP4BB@JISCMAIL.AC.UK
Subject: Re: [ccp4bb] NMR review

Dear Bernhard,

Am 12.01.12 10:30, schrieb Bernhard Rupp (Hofkristallrat a.D.):

Dear All,

I read an interesting statement in an NMR review:

 regions of a protein or
DNA / RNA molecule that are ?exible in the crystal do not provide
coherent X-ray scattering and hence do not contribute to the ?nal
electron density map. Thus, for all intents and purposes, they can
effectively be ignored.

Besides that I was not aware that disorder across molecules implies
incoherence in scattering, I think this is quite some strong tobacco
coming from what is primarily a crystallization screening tool ;-)

That doesn't sound wrong to me: the flexible parts are at different relative positions in 
the unit cells and thus their partial-structure scattering waves do not have 
a constant phase relation to each other, i.e., they don't give a coherent contribution to 
the total scattering.

But I don't agree to their conclusion, since disorder doesn't necessarily mean, 
that there won't be any interpretable electron density left. The floppy parts 
could still be interpreted at an effective lower resolution and thus will not 
be ignored.

Maybe the authors were annoyed by a vanishing NMR signal because the 
macromolecule crystallized in the NMR test tube ;-)

Best regards,

Dirk.

Cheers, BR

PS: I am grappling with the meaning of resolution in NMR. I can see
that it could be related to comparable data/parameter ratios, although
I am even less clear about the weights of NMR restraint weights than in the 
case of MX...
some cross-trained person out there who can explain?


--

***
Dirk Kostrewa
Gene Center Munich
Department of Biochemistry
Ludwig-Maximilians-Universität München
Feodor-Lynen-Str. 25
D-81377 Munich
Germany
Phone:  +49-89-2180-76845
Fax:+49-89-2180-76999
E-mail: kostr...@genzentrum.lmu.de
WWW:www.genzentrum.lmu.de
***


Re: [ccp4bb] NMR review

2012-01-12 Thread Dirk Kostrewa
I'm not a physicist - but isn't (in)coherence also used to describe the 
property of sources of electromagnetic waves with constant wavelength? 
For instance, an incoherent sodium vapour light source (only looking at 
one emission band) compared to a coherent Laser, or the incoherent 
emission from a conventional X-ray source or an X-ray undulator compared 
to a Free-electron-X-ray-Laser? If yes, then we could describe 
diffraction from a crystal in a similar way by treating the crystal as a 
light-source, both with coherent and incoherent scattering from the 
well-ordered and disordered parts, respectively, without any need to 
change the wavelength. In this analogy, the ordered part would have the 
coherence of a Laser, whereas the disordered part would have the 
incoherence of a vapour lamp.


Best regards,

Dirk.

Am 12.01.12 11:57, schrieb Ian Tickle:

On 12 January 2012 10:33, Dirk Kostrewakostr...@genzentrum.lmu.de  wrote:

My understanding of coherence is a constant phase relation between waves.

Correct.  For a perfect crystal all the unit cells are identical so
they scatter in phase
and this gives rise to the interference effect we see as Bragg spots,
as you say arising
from a constant phase relation in specific directions.  For a disordered
crystal the unit cells are not the same: this destroys the
interference effect but there's
still a constant phase relation in any specified direction so it's
still coherent.


Of course, this breaks down for inelastic scattering, but (in)coherence can
also be described without any change in wavelength.

That's not the definition of incoherence used by the physicists.  Of
course you're
free to redefine it but I think that just confuses everyone.

Cheers

-- IAn


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***
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Gene Center Munich
Department of Biochemistry
Ludwig-Maximilians-Universität München
Feodor-Lynen-Str. 25
D-81377 Munich
Germany
Phone:  +49-89-2180-76845
Fax:+49-89-2180-76999
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Re: [ccp4bb] Sub-angstrom resolution

2012-01-11 Thread Dirk Kostrewa

Dear Colin,

Am 10.01.12 18:08, schrieb Colin Nave:

snip


3. The structure factors are lower for large unit cells. This will mean they 
will be harder to detect, particularly if there is a high background.

/snip

But aren't the total structure factors of a unit cell the sum of the 
atomic structure factors? For a larger unit cell (assuming a similar 
solvent content), I would then expect larger structure factors.


Best regards,

Dirk.

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***
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Gene Center Munich
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Ludwig-Maximilians-Universität München
Feodor-Lynen-Str. 25
D-81377 Munich
Germany
Phone:  +49-89-2180-76845
Fax:+49-89-2180-76999
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Re: [ccp4bb] Distinguish NH4 from Na?

2011-11-17 Thread Dirk Kostrewa

Dear Jacob,

for NH4+, you would expect a (partial) tetrahedral coordination with 
typical H-bond distances of ~2.9 A. For Na+, you would expect a 
(partial) octahedral coordination with Metal-to-ligand distances of ~2.4 
A (see Harding, Acta Cryst., D62, 678-682 (2006); Harding, Acta Cryst., 
D58, 872-874 (2002); Glusker, Advances in Protein Chemistry, 42, 1-76 
(1991)).
But depending on your data resolution and quality, and on the 
completeness of the coordination sphere, it might be difficult to 
distinguish between them.


Best regards,

Dirk.

Am 16.11.11 19:20, schrieb Jacob Keller:

Dear Crystallographers,

I have crystals containing 666mM NH4 and 540mM Na, and there appears
to be a water which is only about 2.2 Ang from some polar atoms. It
is currently reasonably happy as a Na, but is there any reasonable way
to decide which cation is there?

JPK



--

***
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Feodor-Lynen-Str. 25
D-81377 Munich
Germany
Phone:  +49-89-2180-76845
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***


Re: [ccp4bb] [PyMOL] Putting a protein molecule into a grid and traversing through the grid

2011-10-28 Thread Dirk Kostrewa

Hi Anasuya,

at least, Gerard Kleywegt's program moleman2 from the Uppsala Software 
Factory http://xray.bmc.uu.se/usf/ has a command XYz 
ALign_inertia_axes should do your first task.
From the moleman2 manual: This will move the currently selected atoms 
such that their centre-of-gravity is at the origin (0,0,0); then it will 
calculate the three principal inertia axes, and align the selected atoms 
such that these axes coincide with the X, Y and Z axis. This alignment 
is done such that the major inertia axis coincides with the X-axis 
(largest eigenvalue), and the minor inertia axis coincides with the 
Z-axis (smallest eigenvalue).


Best regards,

Dirk.

Am 27.10.11 14:17, schrieb Anasuya Dighe:

how do i put a protein molecule inside a cube with x-axis spanning till the
largest x-coordinate, y-axis spanning till the largest y-coordinate, and z-axis
spanning till the largest z-coordinate?

Once i do this, can i divide the larger cube(i.e. the one holding the entire
protein) into smaller ones of lesser dimensions? Say, 5A x 5A x 5A?

Once i generate these smaller cubes, is there a way via pymol, by which i can
navigate through the protein molecule, (smaller)cube by (smaller)cube?
As in, can pymol be used to tell me which residues are lying in which (smaller)
cube and so on?

Can all this be done in a single pymol window/script?
please let me know.

Thanks
-Anasuya




--

***
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Gene Center Munich, A5.07
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Feodor-Lynen-Str. 25
D-81377 Munich
Germany
Phone:  +49-89-2180-76845
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***



Re: [ccp4bb] Linux vs MacOS for crystallographic software

2011-09-29 Thread Dirk Kostrewa

Yes, SHARP and BUSTER both work on a Mac.

Cheers,

Dirk.

Am 29.09.11 09:45, schrieb Sebastiano Pasqualato:

On Sep 29, 2011, at 2:48 AM, Nat Echols wrote:

I don't know of any macromolecular crystallography programs that 
don't run on Mac -


Hey there,
does this mean that SHARP works on a Mac?
ciao,
s


--
Sebastiano Pasqualato, PhD
Crystallography Unit
IFOM-IEO Campus
Cogentech - Consortium for Genomic Technologies
via Adamello, 16
20139 - Milano
Italy

tel +39 02 9437 5172
fax +39 02 9437 5990








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***
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Feodor-Lynen-Str. 25
D-81377 Munich
Germany
Phone:  +49-89-2180-76845
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***



Re: [ccp4bb] question regarding secondary-structure restraints

2011-09-26 Thread Dirk Kostrewa

Dear Nat,

yes, I fully agree - all these restraints that improve the geometry 
either by restraining to high-resolution structures or by introducing 
H-bond restraints for secondary structures are very useful for 
low-resolution structures!


I see your argument with the Ramachandran plot. But imagine a set of 
very strong non-bonding/bonding restraints that would result in an 
absolutely clean Ramachandran plot for any structure, then the 
Ramachandran plot would become useless even in the absence of any 
phi/psi-restraints. So, I prefer to err a bit on the safe side here by 
saying not a truly independent measure.


Personally, I think, that ALL refinement programs, including the 
real-space refinement in Coot, would benefit from inclusion of proper 
H-bonding terms (something, that for instance the very old X-Plor 
version did), since this would automatically restrain secondary 
structures and other hydrophilic interactions to some reasonable 
geometry, even at very low resolution.


Best regards,

Dirk.

Am 26.09.11 16:17, schrieb Nat Echols:
On Mon, Sep 26, 2011 at 1:53 AM, Dirk Kostrewa 
kostr...@genzentrum.lmu.de mailto:kostr...@genzentrum.lmu.de wrote:


when I played with H-bond restraints for secondary structures for
the refinement of a 4.3 A structure (only a few weeks before they
were introduced in phenix), I've made the following observation:
at low resolution without H-bond restraints for secondary
structures, the carbonyl groups of these secondary structures take
the liberty within their globbish electron densities to deviate
from their ideal H-bond conformation, resulting in a tight belt
of outliers around the preferred Ramachandran regions, with
typical deviations of only a few degrees. Introducing the
additional H-bond restraints for maintaining secondary structures
pulls these outlier carbonyl groups back into the preferred
Ramachandran regions. In my case, the number of Ramachandran
outliers was reduced to less than one half! Although, these H-bond
restraints do not directly include information about allowed
Ramachandran regions, the Ramachandran plot is actually affected
by these restraints. Thus, at least in my opinion, the
Ramachandran plot is then not a truly independent measure for
model quality, anymore. The same holds true for all geometrical
restraints, of course.


It depends on how strictly you assess the independence of validation 
criteria.  The Ramachandran plot is considered valid in most cases 
because refinement programs traditionally do not restrain phi and psi 
angles, so we need to rely on the accuracy of the data (and our 
placement of atoms) and various complementary geometry restraints 
(especially nonbonded) to keep residues in the favorable regions of 
the plot.  There are a variety of ways to make the plot better by 
modification of the model and/or restraints (adding hydrogens, 
increasing the weight on the nonbonded restraints, secondary structure 
restraints, etc.), none of which are as drastic as directly 
restraining the model to the plot.  I don't really view this as 
biasing the plot, for two reasons: a) the quantity being measured is 
independent of the quantity restrained, and b) at least in my hands, 
these modifications never completely fix the problem of Ramachandran 
outliers.  (It's the loop regions that are really awful.)


Anyway, I don't think anyone should feel bad about using this kind of 
restraint at low resolution.  The caveat is that of all the 
specialized restraints that we (Jeff Headd and I) have been testing 
for low-resolution refinement (in Phenix), nothing works nearly as 
well in preserving good geometry, and usually improving the R-factors, 
as restraining model parameters to a related high-resolution 
structure, when one is available.  Fortunately, every modern 
refinement program has this ability in some form, and I expect that 
this is going to have the most impact in improving the overall quality 
of low-resolution structures.


-Nat


--

***
Dirk Kostrewa
Gene Center Munich, A5.07
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Ludwig-Maximilians-Universität München
Feodor-Lynen-Str. 25
D-81377 Munich
Germany
Phone:  +49-89-2180-76845
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***



Re: [ccp4bb] Protein structure solved by computer gamers (and phaser)!

2011-09-19 Thread Dirk Kostrewa
Great! Maybe, they should add an extra term for correlation of Fcalc to 
Fobs (or LLG or R) to their game. I wonder, if structures could be 
solved ab inition by players, then :-).


Best regards,

Dirk.

Am 19.09.11 12:33, schrieb Kevin Cowtan:
Crystal structure of a monomeric retroviral protease solved by 
protein folding game players


The paper (Nature SB):
http://www.cs.washington.edu/homes/zoran/NSMBfoldit-2011.pdf

The game:
http://fold.it/portal/


--

***
Dirk Kostrewa
Gene Center Munich, A5.07
Department of Biochemistry
Ludwig-Maximilians-Universität München
Feodor-Lynen-Str. 25
D-81377 Munich
Germany
Phone:  +49-89-2180-76845
Fax:+49-89-2180-76999
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WWW:www.genzentrum.lmu.de
***


[ccp4bb] PIR - was Re: [ccp4bb] Another paper structure retracted

2011-08-12 Thread Dirk Kostrewa

Dear Phil,

I remember one case where reading a sequence file in PIR format failed, 
although I did my best to have the right format. It turned out, that the 
error message about the wrong PIR format was misleading - the real 
cause was a non-standard amino acid letter, in this case a X. Maybe, 
you could check your sequence for this ...


Best regards,

Dirk.


Am 12.08.11 11:16, schrieb Phil Evans:

I was missing the semicolon, but it still fails

On 12 Aug 2011, at 10:12, Antony Oliver wrote:


Interesting iPhone formatting things going on...  Let's try again...

First line is greater than symbol  followed by some text about your protein 
then closed with a semicolon. The next line is blank. The next line contains your amino acid 
sequence, which you can also close with an optional asterisk.

Sent from my iPhone

On 12 Aug 2011, at 10:06, Antony Oliverantony.oli...@sussex.ac.uk  wrote:


PIR is fairly similar to Fasta, from addled memory the format is...


protein name;

empty line
MPREIL...rest of amino acid sequence with an optional asterisk to mark the 
sequence end.

Tony

Sent from my iPhone

On 12 Aug 2011, at 09:14, Phil Evansp...@mrc-lmb.cam.ac.uk  wrote:


Can anyone get this server to work? For me it keeps complaining that my 
sequence file is not a PIR file. The file looks OK to me, but I've never really 
understood what a PIR file is

Phil

On 12 Aug 2011, at 01:39, Kevin Jin wrote:


Should we really have some crystallographers to review and qc those structures 
before the formal releasing?  JCSG has set a very good mechanism for this issue.

There is a sever for self check.

http://smb.slac.stanford.edu/jcsg/QC/






On Thu, Aug 11, 2011 at 4:58 PM, Jacob Kellerj-kell...@fsm.northwestern.edu  
wrote:
I think they fudged the data in this paper...

JPK

On Thu, Aug 11, 2011 at 6:30 PM, David Schullerdj...@cornell.edu  wrote:

link: http://iai.asm.org/cgi/reprint/IAI.05661-11v1

Ferric C. Fang  Arturo Casadevall
Retracted Science and the Retraction Index
Infec. Immun. doi:10.1128/IAI.05661-11

Abstract: Articles may be retracted when their findings are no longer
considered trustworthy due to scientific misconduct or error, they
plagiarize previously published work, or are found to violate ethical
guidelines. Using a novel measure that we call the “retraction index,” we
found that the frequency of retraction varies among journals and shows a
strong correlation with the journal impact factor.
...

(with special attention to Figure 1, Retraction Index vs. Impact Factor)


--
===
All Things Serve the Beam
===
David J. Schuller
modern man in a post-modern world
MacCHESS, Cornell University
schul...@cornell.edu




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***
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Northwestern University
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***



--

***
Dirk Kostrewa
Gene Center Munich, A5.07
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Feodor-Lynen-Str. 25
D-81377 Munich
Germany
Phone:  +49-89-2180-76845
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***


Re: [ccp4bb] Permissions and ownerships in ccp4 6.2.0

2011-07-19 Thread Dirk Kostrewa

Dear all,

or use a modified version of Clemens's commands for that:

find . -perm 700 -exec chmod 755 {} \;
find . -perm 750 -exec chmod 755 {} \;
find . -perm 600 -exec chmod 644 {} \;
find . -perm 640 -exec chmod 644 {} \;

Best regards,

Dirk.

Am 19.07.11 14:34, schrieb Clemens Vonrhein:

Dear all,

ideally, permissions should be either

   rw-r--r-- (0644)

or (for files that need to be executed as well as directories)

   rwxr-xr-x (0755)

One quick fix:

   find . -type d -exec chmod -v 0755 {} ;
   find . -type f -exec chmod -v 0755 {} ;

but that last command makes every single file executable, which is
rather ugly (but doing a selective chmod 0755/0644 is a bit tricky
with all those script files - some need to be executed but others
arent). I don't see a need to have read-only files like all the CIF
dictionaries with permission 0755.


The correct permissions can only be set during packaging
unfortunately.

Cheers

Clemens



--

***
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Gene Center Munich, A5.07
Department of Biochemistry
Ludwig-Maximilians-Universität München
Feodor-Lynen-Str. 25
D-81377 Munich
Germany
Phone:  +49-89-2180-76845
Fax:+49-89-2180-76999
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***


[ccp4bb] Lattice sampling and resolution - a seeming paradox?

2011-04-15 Thread Dirk Kostrewa

Dear colleagues,

I just stumbled across a simple question and a seeming paradox for me in 
crystallography, that puzzles me. Maybe, it is also interesting for you.


The simple question is: is the discrete sampling of the continuous 
molecular Fourier transform imposed by the crystal lattice sufficient to 
get the desired information at a given resolution?


From my old lectures in Biophysics at the University, I know it has 
been theoretically proven, but I don't recall the argument, anymore. I 
looked into a couple of crystallography books and I couldn't find the 
answer in any of those. Maybe, you can help me out.


Let's do a simple gedankenexperiment/thought experiment in the 
1-dimensional crystal case with unit cell length a, and desired 
information at resolution d.


According to Braggs law, the resolution for a first order reflection 
(n=1) is:


1/d = 2*sin(theta)/lambda

with 2*sin(theta)/lambda being the length of the scattering vector |S|, 
which gives:


1/d = |S|

In the 1-dimensional crystal, we sample the continuous molecular 
transform at discrete reciprocal lattice points according to the von 
Laue condition, S*a = h, which gives |S| = h/a here. In other words, the 
unit cell with length a is subdivided into h evenly spaced 
crystallographic planes with distance d = a/h.


Now, the discrete sampling by the crystallographic planes a/h is only 1x 
the resolution d. According to the Nyquist-Shannon sampling theorem in 
Fourier transformation, in order to get a desired information at a given 
frequency, we would need a discrete sampling frequency of *twice* that 
frequency (the Nyquist frequency).


In crystallography, this Nyquist frequency is also used, for instance, 
in the calculation of electron density maps on a discrete grid, where 
the grid spacing for an electron density map at resolution d should be 
= d/2. For calculating that electron density map by Fourier 
transformation, all coefficients from -h to +h would be used, which 
gives twice the number of Fourier coefficients, but the underlying 
sampling of the unit cell along a with maximum index |h| is still only a/h!


This leads to my seeming paradox: according to Braggs law and the von 
Laue conditions, I get the information at resolution d already with a 1x 
sampling a/h, but according to the Nyquist-Shannon sampling theory, I 
would need a 2x sampling a/(2h).


So what is the argument again, that the sampling of the continuous 
molecular transform imposed by the crystal lattice is sufficient to get 
the desired information at a given resolution?


I would be very grateful for your help!

Best regards,

Dirk.

--

***
Dirk Kostrewa
Gene Center Munich, A5.07
Department of Biochemistry
Ludwig-Maximilians-Universität München
Feodor-Lynen-Str. 25
D-81377 Munich
Germany
Phone:  +49-89-2180-76845
Fax:+49-89-2180-76999
E-mail: kostr...@genzentrum.lmu.de
WWW:www.genzentrum.lmu.de
***


Re: [ccp4bb] Lattice sampling and resolution - a seeming paradox?

2011-04-15 Thread Dirk Kostrewa

Dear Ian,

oh, yes, thank you - you are absolutely right! I really confused the 
sampling of the molecular transform with the sampling of the electron 
density in the unit cell! Sometimes I don't see the wood for the trees!


Let me then shift my question from the sampling of the molecular 
transform to the sampling of the electron density within the unit cell. 
For the 1-dimensional case, this is discretely sampled at a/h for 
resolution d, which is still 1x sampling and not 2x sampling, as 
required according to Nyquist-Shannon. Where is my error in reasoning, 
here?


Best regards,

Dirk.

Am 15.04.11 14:25, schrieb Ian Tickle:

Hi Dirk

I think you're confusing the sampling of the molecular transform with
the sampling of the electron density.  You say In the 1-dimensional
crystal, we sample the continuous molecular transform at discrete
reciprocal lattice points according to the von Laue condition, S*a =
h.  In fact the sampling of the molecular transform has nothing to do
with h, it's sampled at points separated by a* = 1/a in the 1-D case.

Cheers

-- Ian

On Fri, Apr 15, 2011 at 12:20 PM, Dirk Kostrewa
kostr...@genzentrum.lmu.de  wrote:

Dear colleagues,

I just stumbled across a simple question and a seeming paradox for me in
crystallography, that puzzles me. Maybe, it is also interesting for you.

The simple question is: is the discrete sampling of the continuous molecular
Fourier transform imposed by the crystal lattice sufficient to get the
desired information at a given resolution?

 From my old lectures in Biophysics at the University, I know it has been
theoretically proven, but I don't recall the argument, anymore. I looked
into a couple of crystallography books and I couldn't find the answer in any
of those. Maybe, you can help me out.

Let's do a simple gedankenexperiment/thought experiment in the 1-dimensional
crystal case with unit cell length a, and desired information at resolution
d.

According to Braggs law, the resolution for a first order reflection (n=1)
is:

1/d = 2*sin(theta)/lambda

with 2*sin(theta)/lambda being the length of the scattering vector |S|,
which gives:

1/d = |S|

In the 1-dimensional crystal, we sample the continuous molecular transform
at discrete reciprocal lattice points according to the von Laue condition,
S*a = h, which gives |S| = h/a here. In other words, the unit cell with
length a is subdivided into h evenly spaced crystallographic planes with
distance d = a/h.

Now, the discrete sampling by the crystallographic planes a/h is only 1x the
resolution d. According to the Nyquist-Shannon sampling theorem in Fourier
transformation, in order to get a desired information at a given frequency,
we would need a discrete sampling frequency of *twice* that frequency (the
Nyquist frequency).

In crystallography, this Nyquist frequency is also used, for instance, in
the calculation of electron density maps on a discrete grid, where the grid
spacing for an electron density map at resolution d should be= d/2. For
calculating that electron density map by Fourier transformation, all
coefficients from -h to +h would be used, which gives twice the number of
Fourier coefficients, but the underlying sampling of the unit cell along a
with maximum index |h| is still only a/h!

This leads to my seeming paradox: according to Braggs law and the von Laue
conditions, I get the information at resolution d already with a 1x sampling
a/h, but according to the Nyquist-Shannon sampling theory, I would need a 2x
sampling a/(2h).

So what is the argument again, that the sampling of the continuous molecular
transform imposed by the crystal lattice is sufficient to get the desired
information at a given resolution?

I would be very grateful for your help!

Best regards,

Dirk.

--

***
Dirk Kostrewa
Gene Center Munich, A5.07
Department of Biochemistry
Ludwig-Maximilians-Universität München
Feodor-Lynen-Str. 25
D-81377 Munich
Germany
Phone:  +49-89-2180-76845
Fax:+49-89-2180-76999
E-mail: kostr...@genzentrum.lmu.de
WWW:www.genzentrum.lmu.de
***



--

***
Dirk Kostrewa
Gene Center Munich, A5.07
Department of Biochemistry
Ludwig-Maximilians-Universität München
Feodor-Lynen-Str. 25
D-81377 Munich
Germany
Phone:  +49-89-2180-76845
Fax:+49-89-2180-76999
E-mail: kostr...@genzentrum.lmu.de
WWW:www.genzentrum.lmu.de
***


Re: [ccp4bb] Lattice sampling and resolution - a seeming paradox?

2011-04-15 Thread Dirk Kostrewa

Dear colleagues of the CCP4BB,

many thanks for all your replies - I really got lost in the trees (or 
wood?) and you helped me out with all your kind responses!


I should really leave for the weekend ...

Have a nice weekend, too!

Best regards,

Dirk.

Am 15.04.11 13:20, schrieb Dirk Kostrewa:

Dear colleagues,

I just stumbled across a simple question and a seeming paradox for me 
in crystallography, that puzzles me. Maybe, it is also interesting for 
you.


The simple question is: is the discrete sampling of the continuous 
molecular Fourier transform imposed by the crystal lattice sufficient 
to get the desired information at a given resolution?


From my old lectures in Biophysics at the University, I know it has 
been theoretically proven, but I don't recall the argument, anymore. I 
looked into a couple of crystallography books and I couldn't find the 
answer in any of those. Maybe, you can help me out.


Let's do a simple gedankenexperiment/thought experiment in the 
1-dimensional crystal case with unit cell length a, and desired 
information at resolution d.


According to Braggs law, the resolution for a first order reflection 
(n=1) is:


1/d = 2*sin(theta)/lambda

with 2*sin(theta)/lambda being the length of the scattering vector 
|S|, which gives:


1/d = |S|

In the 1-dimensional crystal, we sample the continuous molecular 
transform at discrete reciprocal lattice points according to the von 
Laue condition, S*a = h, which gives |S| = h/a here. In other words, 
the unit cell with length a is subdivided into h evenly spaced 
crystallographic planes with distance d = a/h.


Now, the discrete sampling by the crystallographic planes a/h is only 
1x the resolution d. According to the Nyquist-Shannon sampling theorem 
in Fourier transformation, in order to get a desired information at a 
given frequency, we would need a discrete sampling frequency of 
*twice* that frequency (the Nyquist frequency).


In crystallography, this Nyquist frequency is also used, for instance, 
in the calculation of electron density maps on a discrete grid, where 
the grid spacing for an electron density map at resolution d should be 
= d/2. For calculating that electron density map by Fourier 
transformation, all coefficients from -h to +h would be used, which 
gives twice the number of Fourier coefficients, but the underlying 
sampling of the unit cell along a with maximum index |h| is still only 
a/h!


This leads to my seeming paradox: according to Braggs law and the von 
Laue conditions, I get the information at resolution d already with a 
1x sampling a/h, but according to the Nyquist-Shannon sampling theory, 
I would need a 2x sampling a/(2h).


So what is the argument again, that the sampling of the continuous 
molecular transform imposed by the crystal lattice is sufficient to 
get the desired information at a given resolution?


I would be very grateful for your help!

Best regards,

Dirk.



--

***
Dirk Kostrewa
Gene Center Munich, A5.07
Department of Biochemistry
Ludwig-Maximilians-Universität München
Feodor-Lynen-Str. 25
D-81377 Munich
Germany
Phone:  +49-89-2180-76845
Fax:+49-89-2180-76999
E-mail: kostr...@genzentrum.lmu.de
WWW:www.genzentrum.lmu.de
***


Re: [ccp4bb] Crystallographic Breakthrough - DarkMatter Version 1.0

2011-04-01 Thread Dirk Kostrewa

Hi Ethan,

many thanks for that - your Dark Matter really (en)lightened my day! I 
wonder, how many pdb records in the future will contain the 
corresponding remark lines that your incredible perl script produces :-)


Best regards,

Dirk.

Am 01.04.11 08:06, schrieb Ethan Merritt:

Hi to all on ccp4bb:

What better day to announce the availability of a breakthrough technique
in macromolecular crystallography?

Given recent discussion and in particular James Holton's suggestion that
the problem of disordered sidechains is a problem akin to the difficulty
of describing dark matter and dark energy...

I am happy to announce a new crystallographic tool that can improve your
model by accounting for an often-neglected physical property. A detailed
explanation, references, and a preliminary implementation of the program
can be downloaded from

http://skuld.bmsc.washington.edu/DarkMatter



--

***
Dirk Kostrewa
Gene Center Munich, A5.07
Department of Biochemistry
Ludwig-Maximilians-Universität München
Feodor-Lynen-Str. 25
D-81377 Munich
Germany
Phone:  +49-89-2180-76845
Fax:+49-89-2180-76999
E-mail: kostr...@genzentrum.lmu.de
WWW:www.genzentrum.lmu.de
***


Re: [ccp4bb] Density sharpening with Truncate?

2011-02-28 Thread Dirk Kostrewa

Dear Randy,

thanks for your comment - a good point with the likelihood target 
estimated from E-values! So, in principle, there shouldn't be any 
difference in maximum-likelihood refinement using sharpened data or not. 
However, for curiosity, in one case at 4.3 A resolution and a sharpening 
B-factor of ~100 A**2, I compared ML refinement against the sharpened 
data with ML refinement against the original data and subsequent map 
sharpening: the R-factors were almost identical, and so were the 
electron density maps in most places. But in a some places, the maps 
were slightly different, with slightly less (!) model-bias and slightly 
clearer densities for the refinement against sharpened data. But those 
judgements were very subjective, and since a true structure at really 
high resolution is not available, I never could quantify this. Either, 
this was only anecdotal evidence, or there is still room for improvement 
in existing ML refinement programs.


Best regards,

Dirk.

Am 28.02.11 11:40, schrieb Randy Read:

Hi,

I'm on Garib's side here.  The way the maximum likelihood targets work, the 
variances are defined relative to the average intensity in a resolution shell, 
so if you change the falloff the variances will change in the same way.  In 
fact, one way to implement maximum likelihood refinement is in terms of 
E-values, from which the falloff has been removed.  If your B-factors didn't 
run into hard limits (which, as Garib points out, they will when you make the 
data non-physical) you would end up with the same model if you refined against 
sharpened data, except the B-factors would be lower.  The other thing that will 
change if you sharpen the data is that the R-factors will be higher, because 
the poorly-fit higher-resolution terms will contribute more to the sums.  And 
that's probably not what you want when you might already have a hard time 
getting a low resolution structure past the freeR police!

This is a case where intuition can lead you astray.  Intuition might suggest 
that, if you sharpen the data, the refinement program should pay more attention 
to fitting the high resolution detail, but the likelihood target doesn't look 
at the data the same way you do when you look at a map.  The fact that you can 
define the target in terms of E-values means that, if your model and data are 
both good, the likelihood target can be thought of as sharpening the data 
anyway.

Best wishes,

Randy Read

On 28 Feb 2011, at 09:02, Dirk Kostrewa wrote:


Dear CCP4ers,

I really would sharpen the structure factors, not only the electron density 
maps. The simple reason is: if sharpening emphasizes enough information at 
higher resolution to help interpreting the electron density maps, refinement 
will also benefit from this information.
Of course, the mean B-factor of the refined structure will be lower by the 
sharpening B-factor, but since B-factor sharpening is usually done with lower 
resolution data, the Wilson B-factor is usually very high, and thus far, I 
didn't run into problems with B-factors crashing at the lower limit.
The sharpening B-factor can easily reach values in the -100s A**2, not only -10 
to -50 A**2. Axel Brunger has published several papers about how to estimate a 
good sharpening B-factor (a recent one with references is Brunger et al. Acta 
Cryst D65, 128-133). He usually describes map sharpening, but B-factor 
sharpening of structure factors seems to be done routinely for virus structures 
in Steve Harrisons lab.

One word of caution: the B-factor sharpening should be correctly described not 
only in the publication but also in the PDB deposition (if refinement was done 
against sharpened structure factors, the refinement statistics can only be 
reproduced using these structure factors). The original structure factors can 
be easily reproduced by applying back the negative sharpening B-factor.

Best regards,

Dirk.

Am 26.02.11 01:09, schrieb Garib N Murshudov:

I would not sharpen structure factors before refinement. It may cause problems 
with B value refinement (a lot of B values may stuck around 2 or minimum B). 
One must remember that not all atoms in crystal have same Bvalue. There is a 
distribution of Bvalues.

However maps can be sharpened after refinement. It can be done directly in coot 
(I hope this version of coot is now widely available). Or if you are using 
refmac for refinement you can use:

mapc sharpen   #  regularised map sharpening. Bvalues and regularisation 
parameters are calculated automatically

or

mapc sharpenBvalue   # regularised map sharpening with specified Bvalue

or

mapc sharpenBvalue
mapc sharpen alphavalue=0.1#  regularisation paramater. alpha=0 is simple 
sharpening.


I am sure other programs have similar options. (I know CNS has and it has been 
used successfully by many people)

regards
Garib

P.S. These options available from refmac v5.6 available from; 
www.ysbl.york.ac.uk/refmac/data/refmac_experimental

Re: [ccp4bb] strange density

2011-02-24 Thread Dirk Kostrewa
An additional information would be to calculate an anomalous difference 
map: at typical synchrotron wavelenght of ~1 A, Ni would have ~2 
electrons f'', whereas Cl would have only ~0.2 electrons f''. So, a 
strong anomalous difference density peak would be more consistent with 
Ni than with Cl.
However, if the data set was collected on a home source with CuKalpha 
wavelength, such a map would be not be very helpful here, because the Ni 
signal is about as weak as the Cl signal.


Best regards,

Dirk.

Am 24.02.11 16:37, schrieb Gloria Borgstahl:

I'm voting with Roger this time.
If I were you I would model a nickel in there (unless you have a 
better candidate)
if it is right, the distances to the His should be like seen in a SOD 
active site.
Then you can model the bonds and waters.  You may need partial 
occupancy on the metal.
Reminds me of the time I found a 6th water in MnSOD as I was 
making the token electron denisty
figure of the active site.  Found myself doing more refinement and a 
much better paper.


On Thu, Feb 24, 2011 at 8:15 AM, Roger Rowlett rrowl...@colgate.edu 
mailto:rrowl...@colgate.edu wrote:


This looks suspiciously like a metal ion with 3 or more resolved
water ligands. It's hard to tell from the images provided, but it
looks like the metal could be close to octahedral, with 2 His and
3 water ligands well-defined. The estimated metal-nitrogen bond
distances might help narrow down the metal ion. For example,
tetrahedral Zn(II) has a Zn-N bond distance of around 2.0 A. I
suppose this could be a Mg(II) ion, since that is in your
crystallization mix, but I think that Mg(II) typically prefers
harder protein  ligands, e.g., carboxylates. Zn(II) is a very
common contaminant in solution, however, and should not
necessarily be discounted; indeed Zn(II) and other first row
transition metal ions would be expected to have a reasonable
affinity for medium hard/soft ligands such as vicinial His residues.

Cheers.

On 2/23/2011 7:34 PM, Alex Singer wrote:


cocrystallized in 2.5mM Glycero-3Phosphocholine and cryoprotected
by dipping in 
-- 


Roger S. Rowlett
Professor
Department of Chemistry
Colgate University
13 Oak Drive
Hamilton, NY 13346

tel: (315)-228-7245
ofc: (315)-228-7395
fax: (315)-228-7935
email: rrowl...@colgate.edu mailto:rrowl...@colgate.edu




--

***
Dirk Kostrewa
Gene Center Munich, A5.07
Department of Biochemistry
Ludwig-Maximilians-Universität München
Feodor-Lynen-Str. 25
D-81377 Munich
Germany
Phone:  +49-89-2180-76845
Fax:+49-89-2180-76999
E-mail: kostr...@genzentrum.lmu.de
WWW:www.genzentrum.lmu.de
***



[ccp4bb] Postdoc position at the Gene Center Munich

2011-02-21 Thread Dirk Kostrewa

Dear CCP4ers,

on behalf of Patrick Cramer, I send a Postdoc position offer, given 
below. Please, do not respond to me, but to the e-mail addresses given 
in the job description.


Best regards,

Dirk Kostrewa.

***

Applications are invited for a

RESEARCH SCIENTIST (POSTDOC) POSITION IN CRYSTALLOGRAPHY

to work on multi-component complexes and study the mechanisms of gene 
transcription in the lab of Patrick Cramer at the Gene Center of the 
University of Munich (www.LMB.uni-muenchen.de/cramer).


We look for a collaborative person with a background in X-ray 
crystallography, documented by at least one significant first-author 
publication. We offer a stimulating environment on a leading European 
life science campus, and a longer-term perspective (2-5 years). There 
are possibilities to join ongoing projects of high scientific 
significance, to participate in networks of excellence at the national 
and international level, and to contribute to teaching. Thus this 
position can prepare for an independent career.


Applications including a one-page CV, list of publications, and email 
addresses of two referees should be sent to R. Menacher 
(menac...@lmb.uni-muenchen.de).


Questions may be sent to Patrick Cramer (cra...@lmb.uni-muenchen.de).

Deadline for applications is March 1st, 2011.


[ccp4bb] PDB deposition ADIT without frames?

2011-02-15 Thread Dirk Kostrewa

Dear CCP4ers,

a colleague of mine is just going through the PDB deposition process 
using the usual ADIT website. In contrast to my experience and to the 
ADIT turorial, she has only one frame in the browser. The left frame 
with the overview is missing. So, there is no way to jump between the 
different deposition fields, which makes deposition a nightmare. Has 
anybody else noticed that?


Best regards,

Dirk.

--

***
Dirk Kostrewa
Gene Center Munich, A5.07
Department of Biochemistry
Ludwig-Maximilians-Universität München
Feodor-Lynen-Str. 25
D-81377 Munich
Germany
Phone:  +49-89-2180-76845
Fax:+49-89-2180-76999
E-mail: kostr...@genzentrum.lmu.de
WWW:www.genzentrum.lmu.de
***


Re: [ccp4bb] PDB deposition ADIT without frames?

2011-02-15 Thread Dirk Kostrewa
Thanks a lot for your suggestions! Meanwhile, my colleague entered the 
desired sequence information into the first website without frames, and 
after that, the usual frame layout re-appeared! I don't know whether 
this is a bug or intended ...


Best regards,

Dirk.

Am 15.02.11 17:00, schrieb Dirk Kostrewa:

Dear CCP4ers,

a colleague of mine is just going through the PDB deposition process 
using the usual ADIT website. In contrast to my experience and to the 
ADIT turorial, she has only one frame in the browser. The left frame 
with the overview is missing. So, there is no way to jump between the 
different deposition fields, which makes deposition a nightmare. Has 
anybody else noticed that?


Best regards,

Dirk.



--

***
Dirk Kostrewa
Gene Center Munich, A5.07
Department of Biochemistry
Ludwig-Maximilians-Universität München
Feodor-Lynen-Str. 25
D-81377 Munich
Germany
Phone:  +49-89-2180-76845
Fax:+49-89-2180-76999
E-mail: kostr...@genzentrum.lmu.de
WWW:www.genzentrum.lmu.de
***


[ccp4bb] Counting of geometrical restraints?

2011-01-31 Thread Dirk Kostrewa

Dear Ian  other CCP4ers,

I want to get a riddle about counting geometrical restraints solved, 
which emerged in my head after a recent discussion 
http://www.mail-archive.com/ccp4bb@jiscmail.ac.uk/msg17534.html on 
this board about the effect of NCS on the data:parameter ratio. This 
discussion quickly centered around the 1998 Acta Cryst paper about 
R-factor ratios [1]. So, here is my riddle:


On one hand, geometrical restraints can be counted as observations. 
Refinement programs use differences between model geometry and ideal 
geometry restraints as least-squares targets, in a similar way to 
differences between model structure factor amplitudes and observed 
structure factor amplitudes. Model refinement is possible using 
geometrical restraints only, in the complete absence of observed 
structure factor amplitudes (idealization; whether this makes sense, is 
a different question). Geometrical restraints are also counted as 
observations in [1], both in Table 1 and in the text (for example in 
formula 2).


On the other hand, it is shown in that paper, summarized in Table 2, 
that for the Rfree/Rwork ratios, geometrical restraints effectively 
reduce the number of refinement parameters, with a smooth transition 
from restraints to constraints via the residual term Drest. This implies 
that geometrical restraints can be counted as reducing the numbers of 
parameters, not as increasing the number of observations, which was also 
brought up as an argument in the aforementioned discussion.


Thus, on one hand, geometrical restraints can be counted as 
observations, on the other hand they can be counted as reducing the 
number of parameters. The riddle for me is, that these two ways of 
counting are mutually exclusive alternatives - so, which one is the 
right one?


I would be grateful, if you, Ian, or any other crystallographer on this 
board could help me (and maybe others) to solve this riddle.


Best regards,

Dirk.

[1] Tickle, Laskowski, Moss. Rfree and the rfree ratio. I. Derivation 
of expected values of cross-validation residuals used in macromolecular 
least-squares refinement, Acta Cryst., D54, 547-557 (1998)


--

***
Dirk Kostrewa
Gene Center Munich, A5.07
Department of Biochemistry
Ludwig-Maximilians-Universität München
Feodor-Lynen-Str. 25
D-81377 Munich
Germany
Phone:  +49-89-2180-76845
Fax:+49-89-2180-76999
E-mail: kostr...@genzentrum.lmu.de
WWW:www.genzentrum.lmu.de
***



Re: [ccp4bb] Merging data to increase multiplicity

2011-01-28 Thread Dirk Kostrewa

Hi Bert,

here is one anecdotal evidence: a couple of years ago, I had one real 
in-house 3 A data set from a crystal after a quick iodide soak and 
processed the images with denzo/scalepack, mosflm/scala and xds/xscale. 
I got lower Rsym, higher I/sig(I) and better anomalous signal with xds. 
More importantly, I could solve the iodide substructure easily with 
SHELXC/D at different high resolution limits up to 3.5 A with the xds 
data set. For the other data sets, I had to cut the higher resolution 
limit down to 4-5 A, and there were fewer solutions for the substructure.


Best regards,

Dirk.

Am 28.01.11 14:37, schrieb Van Den Berg, Bert:
I have heard this before. I'm wondering though, does anybody know of a 
systematic study where different data processing programs are compared 
with real-life, non-lysozyme data?


Bert


On 1/28/11 7:58 AM, Bosch, Juergen jubo...@jhsph.edu wrote:

I was a bit reductive with my statement (iPhone)
The equation below is suppose to read:
If you have bad data, then you need to process with XDS in order
to get the maximum out of your data.

Thanks Tim,

Jürgen

-
Jürgen Bosch
Johns Hopkins Bloomberg School of Public Health
Department of Biochemistry  Molecular Biology
Johns Hopkins Malaria Research Institute
615 North Wolfe Street, W8708
Baltimore, MD 21205
Phone: +1-410-614-4742
Lab:  +1-410-614-4894
Fax:  +1-410-955-3655
http://web.mac.com/bosch_lab/ http://web.me.com/bosch_lab/

On Jan 28, 2011, at 7:44 AM, Tim Gruene wrote:

Dear Jürgen,

is this an assignment operator or an equal sign? For if it's
the latter it could
read that the result of processing data with XDS are bad data,
which is rather
rude and probably not what you meant.

Tim

On Fri, Jan 28, 2011 at 06:55:43AM -0500, Jürgen Bosch wrote:

Bad data = processing with XDS

Jürgen

..
Jürgen Bosch
Johns Hopkins Bloomberg School of Public Health
Department of Biochemistry  Molecular Biology
Johns Hopkins Malaria Research Institute
615 North Wolfe Street, W8708
Baltimore, MD 21205
Phone: +1-410-614-4742
Lab:  +1-410-614-4894
Fax:  +1-410-955-3655
http://web.mac.com/bosch_lab/

On Jan 28, 2011, at 6:46, José Trincão
trin...@dq.fct.unl.pt wrote:

Hello all,
I have been trying to squeeze the most out of a bad
data set (P1, anisotropic, crystals not reproducible).
I had very incomplete data due to high mosaicity and
lots of overlaps. The completeness was about 80%
overall to ~3A. Yesterday I noticed that I could
process the data much better fixing the mosaicity to
0.5 in imosflm. I got about 95% complete up to 2.5A
but with a multiplicity of 1.7. I tried to integrate
the same data fixing the mosaicity at different values
ranging from 0.2 to 0.6 and saw the trend in
completeness, Rmerge and multiplicity.
Now, is there any reason why I should not just merge
all these together and feed them to scala in order to
increase multiplicity?
Am I missing something?

Thanks for any comments!

Jose


José Trincão, PhDCQFB@FCT-UNL
2829-516 Caparica, Portugal

It's very hard to make predictions... especially
about the future - Niels Bohr



--

***
Dirk Kostrewa
Gene Center Munich, A5.07
Department of Biochemistry
Ludwig-Maximilians-Universität München
Feodor-Lynen-Str. 25
D-81377 Munich
Germany
Phone:  +49-89-2180-76845
Fax:+49-89-2180-76999
E-mail: kostr...@genzentrum.lmu.de
WWW:www.genzentrum.lmu.de
***



Re: [ccp4bb] High Rmerge with thin frames

2010-11-05 Thread Dirk Kostrewa

Dear Sergei,

since your Rmerge is high at low resolution even in P1, my guess is, 
that there was a problem either with the crystal or with the data 
collection. Fine slicing should improve the data quality, because your 
get a better description of the reference profiles and reduce the 
background. Different merging of fine-sliced images into 
coarser-sliced images was already systematically done by Wolfgang 
Kabsch, with the result, that finer slices gave better results, although 
slices much finer than half the full mosaicity angle of a reflection 
didn't improve the results much further (I've heard a talk given by 
Wolfgang, but never found a publication about these results). There is a 
publication in 1999 about fine-slicing by Jim Pflugrath, that you might 
want to read about this (Acta Cryst D55, 1718-1725). So, merging 
fine-sliced images into coarse-sliced probably won't help.


Anyway, good luck!

Dirk.

Am 05.11.10 09:40, schrieb Sergei Strelkov:

Dear All,

I am processing a dataset collected (not by me) with 0.1 degree 
oscillations.
The diffraction is quite weak even though there is a clean diffraction 
pattern to about 3A.


Either Mosflm or XDS processes the data readily with +/- default settings
but both yield a high overall Rmerge of about 0.23 in the expected 
symmetry.
Processing in P1 yields an overall Rmerge of ~0.18, but what is 
especially disappointing

is that Rmerge is as high as 0.15 at ~5A resolution already.

The question is, how can we process the data so that the merging 
statistics

becomes more reasonable?

Apparent mosaicity turns out to be ~0.5A. My naive way of thinking is
to try treating each five consecutive frames as a single 0.5 degree 
frame.

Does anyone have experience with this?

Many thanks in advance,
Sergei


--

***
Dirk Kostrewa
Gene Center Munich, A5.07
Department of Biochemistry
Ludwig-Maximilians-Universität München
Feodor-Lynen-Str. 25
D-81377 Munich
Germany
Phone:  +49-89-2180-76845
Fax:+49-89-2180-76999
E-mail: kostr...@genzentrum.lmu.de
WWW:www.genzentrum.lmu.de
***


[ccp4bb] Off-Topic: CNS MAXLEV error

2010-11-05 Thread Dirk Kostrewa

Dear CCP4ers,

sorry for this off-topic question, but maybe, somebody can answer this:

I want to refine some self-defined dummy-atoms (scatter.lib, topology, 
parameter: all copypaste from water and modified) with CNS and get the 
following enigmatic error message:


%CONNE2 error encountered: MAXLEV exceeded

Does anyone could point me to a direction what that means?

Best regards,

Dirk.

--

***
Dirk Kostrewa
Gene Center Munich, A5.07
Department of Biochemistry
Ludwig-Maximilians-Universität München
Feodor-Lynen-Str. 25
D-81377 Munich
Germany
Phone:  +49-89-2180-76845
Fax:+49-89-2180-76999
E-mail: kostr...@genzentrum.lmu.de
WWW:www.genzentrum.lmu.de
***


Re: [ccp4bb] Against Method (R)

2010-10-29 Thread Dirk Kostrewa

Hi Robbie,

yes, the apparently larger radius of convergence in real space 
refinement impresses me, too. Therefore, I usually do local real space 
refinement after manually correcting errors, either with Moloc at lower 
resolution or with Coot at higher resolution, prior to reciprocal space 
refinement.


If I recall correctly, real space refinement was introduced by Robert 
Diamond in the 60s long before reciprocal space refinement. In the 90s 
Michael Chapman tried to revive it, but without much success, as far as 
I know. With the fast computers today, maybe the time has come again for 
real space refinement ...


Best regards,

Dirk.

Am 29.10.10 08:03, schrieb Robbie Joosten:

Hi Bart,

I agree with the building strategy you propose, but at some point it 
stops helping and a bit more attention to detail is needed. Reciprocal 
space refinement doesn't seem to do the fine details. It always 
surprises me how much atoms still move when you real-space refine a 
refined model, especially the waters. I admit this is not a fair 
comparison.


High resolution data helps, but better data makes it tempting to put 
too little effort in optimising the model. I've seen some horribly 
obvious errors in hi-res models (more than 10 sigma difference density 
peaks for misplaced side chains). At the same time there are quite a 
lot of low-res models that are exceptionally good.


Cheers,
Robbie

 Date: Thu, 28 Oct 2010 16:32:04 -0600
 From: bart.ha...@ualberta.ca
 Subject: Re: [ccp4bb] Against Method (R)
 To: CCP4BB@JISCMAIL.AC.UK

 On 10-10-28 04:09 PM, Ethan Merritt wrote:
  This I can answer based on experience. One can take the coordinates 
from a structure
  refined at near atomic resolution (~1.0A), including multiple 
conformations,
  partial occupancy waters, etc, and use it to calculate R factors 
against a lower
  resolution (say 2.5A) data set collected from an isomorphous 
crystal. The
  R factors from this total-rigid-body replacement will be better 
than anything you
  could get from refinement against the lower resolution data. In 
fact, refinement

  from this starting point will just make the R factors worse.
 
  What this tells us is that the crystallographic residuals can 
recognize a
  better model when they see one. But our refinement programs are not 
good
  enough to produce such a better model in the first place. Worsr, 
they are not

  even good enough to avoid degrading the model.
 
  That's essentially the same thing Bart said, perhaps a little more 
pessimistic :-)

 
  cheers,
 
  Ethan
 

 Not pessimistic at all, just realistic and perhaps even optimistic for
 methods developers as apparently there is still quite a bit of progress
 that can be made by improving the search strategy during refinement.

 During manual refinement I normally tell students not to bother about
 translating/rotating/torsioning atoms by just a tiny bit to make it fit
 better. Likewise there is no point in moving atoms a little bit to
 correct a distorted bond or bond length. If it needed to move that
 little bit the refinement program would have done it for you. Look for
 discreet errors in the problematic residue or its neighbors: peptide
 flips, 120 degree changes in side chain dihedrals, etc. If you can find
 and fix one of those errors a lot of the stereochemical distortions and
 non-ideal fit to density surrounding that residue will suddenly
 disappear as well.

 The benefit of high resolution is that it is much easier to pick up and
 fix such errors (or not make them in the first place)

 Bart

 --

 

 Bart Hazes (Associate Professor)
 Dept. of Medical Microbiology Immunology
 University of Alberta
 1-15 Medical Sciences Building
 Edmonton, Alberta
 Canada, T6G 2H7
 phone: 1-780-492-0042
 fax: 1-780-492-7521

 


--

***
Dirk Kostrewa
Gene Center Munich, A5.07
Department of Biochemistry
Ludwig-Maximilians-Universität München
Feodor-Lynen-Str. 25
D-81377 Munich
Germany
Phone:  +49-89-2180-76845
Fax:+49-89-2180-76999
E-mail: kostr...@genzentrum.lmu.de
WWW:www.genzentrum.lmu.de
***



Re: [ccp4bb] Against Method (R)

2010-10-29 Thread Dirk Kostrewa

Dear George,

thanks a lot! I see the point, that in reciprocal space refinement one 
could refine directly against the observed intensities and sigmas. But 
in principle, one could do iterative real space refinement, structure 
factor and intensity calculation for refinement statistics and weights, 
calculation of an improved electron density map (but that requires Fs 
again ...), and so forth until some convergence criterion is met. I 
wonder, which refinement scheme is more efficient.


The missing reflections in map calculation is something that we have to 
live with, and unless the data are severely incomplete, I must admit, 
that I don't worry too much.


The twinning problem is really severe! Here, I don't see how this could 
be done in a clever way in real space.


Interesting discussion ...

Best wishes,

Dirk.

Am 29.10.10 10:41, schrieb George M. Sheldrick:

Dear Dirk,

There are good reasons why real space refinement has never become popular.
With reciprocal space refinement, you refine directly against what you
measured, taking the standard uncertainly of each individual intensity
into account. In this context I was pleased to read in CCP4bb that REFMAC
will soon be refining against intensities (like SHELXL). Then the
assumptions made (e.g. no distortion of the expected intensity distribution
by e.g. NCS or twinning) and even 'bugs' in (c)truncate will no longer
matter. If for some reason a reflection wasn't measured, then simply
leaving it out it does not invalidate a recoprocal space refinement.
The same applies to reflections that are reserved for Rfree.

In contrast, the electron density is only theoretically correct if all
reflections between 0,0,0 and infinity are included in the Fourier
summation, For a twin it is even worse, because we don't know how to
partition the difference between Fo^2 and Fc^2 between the twin
components. None of the attempts to work around these problems are
entirely convincing. Maps and real space refinement are invaluable in
the intermediate stages of model building and correction, but the
final refinement should be performed in reciprocal space.

Best wishes, George

Prof. George M. Sheldrick FRS
Dept. Structural Chemistry,
University of Goettingen,
Tammannstr. 4,
D37077 Goettingen, Germany
Tel. +49-551-39-3021 or -3068
Fax. +49-551-39-22582


On Fri, 29 Oct 2010, Dirk Kostrewa wrote:


Hi Robbie,

yes, the apparently larger radius of convergence in real space refinement
impresses me, too. Therefore, I usually do local real space refinement after
manually correcting errors, either with Moloc at lower resolution or with Coot
at higher resolution, prior to reciprocal space refinement.

If I recall correctly, real space refinement was introduced by Robert Diamond
in the 60s long before reciprocal space refinement. In the 90s Michael Chapman
tried to revive it, but without much success, as far as I know. With the fast
computers today, maybe the time has come again for real space refinement ...

Best regards,

Dirk.

Am 29.10.10 08:03, schrieb Robbie Joosten:

Hi Bart,

I agree with the building strategy you propose, but at some point it stops
helping and a bit more attention to detail is needed. Reciprocal space
refinement doesn't seem to do the fine details. It always surprises me how
much atoms still move when you real-space refine a refined model, especially
the waters. I admit this is not a fair comparison.

High resolution data helps, but better data makes it tempting to put too
little effort in optimising the model. I've seen some horribly obvious
errors in hi-res models (more than 10 sigma difference density peaks for
misplaced side chains). At the same time there are quite a lot of low-res
models that are exceptionally good.

Cheers,
Robbie


Date: Thu, 28 Oct 2010 16:32:04 -0600
From: bart.ha...@ualberta.ca
Subject: Re: [ccp4bb] Against Method (R)
To: CCP4BB@JISCMAIL.AC.UK

On 10-10-28 04:09 PM, Ethan Merritt wrote:

This I can answer based on experience. One can take the coordinates

from a structure

refined at near atomic resolution (~1.0A), including multiple

conformations,

partial occupancy waters, etc, and use it to calculate R factors

against a lower

resolution (say 2.5A) data set collected from an isomorphous

crystal. The

R factors from this total-rigid-body replacement will be better

than anything you

could get from refinement against the lower resolution data. In

fact, refinement

from this starting point will just make the R factors worse.

What this tells us is that the crystallographic residuals can

recognize a

better model when they see one. But our refinement programs are not

good

enough to produce such a better model in the first place. Worsr,

they are not

even good enough to avoid degrading the model.

That's essentially the same thing Bart said, perhaps a little more

pessimistic :-)

cheers,

Ethan


Not pessimistic at all, just realistic and perhaps even optimistic for
methods developers as apparently there is still

Re: [ccp4bb] Babinet solvent correction [WAS: R-free flag problem]

2010-10-28 Thread Dirk Kostrewa

Hi Tim,

sorry for my late reply - I just came back to the lab.

In the Babinet bulk solvent correction, no bulk solvent phases are used, 
it is entirely based on amplitudes and strictly only valid if the phases 
of the bulk solvent are opposite to the ones of the protein. And as 
Sasha Urzhumtsev pointed out, this assumption is only valid at very low 
resolution.


The mask bulk solvent correction is a vector sum including the phases of 
the bulk solvent mask, which makes a difference at medium resolution (up 
to ~4.5 A, or so).


As far as I can see, your formulas given below do not distinguish 
between amplitude (modulus) and vector bulk solvent corrections.


Personally, I really don't see any physical sense in using both 
corrections together, except for compensating any potential scaling 
problems at low resolution.


If the model is basically complete and correct, the mask bulk solvent 
correction is usually superior to the Babinet bulk solvent correction 
(see, for example, my old and small CCP4 Newsletter contribution 
http://www.ccp4.ac.uk/newsletters/newsletter34/bsdk_text.html).


However, there are also good reasons for using the Babinet bulk solvent 
correction (it should be an option in ALL refinement programs!):

- it requires only two parameters and can be used in any case
- in rigid body refinement, the mask lags behind; here, I always use the 
Babinet BS correction
- channels could show false positive density, because the mask left them 
empty - this depends heavily on the choice of radii to determine/shrink 
the bulk solvent mask; in such cases, I always calculate a Babinet BS 
correction as a control


Best regards,

Dirk.

Am 23.10.10 22:14, schrieb Tim Fenn:

On Sat, 23 Oct 2010 10:05:15 -0700
Pavel Afoninepafon...@gmail.com  wrote:


Hi Tim,

  ...but I hope this answers the question:
Babinet's vs. the flat model?  Use them together!  ;)


thanks a lot for your reply.

Could you please explain the *physical* meaning of using both
models together?

I can try!  Typically, we model the bulk solvent using a real space
mask that is set to 1 in the bulk solvent region and 0 in the protein.
This gets Fourier transformed, symmetrized and added in to the
scattering factors from the molecule (Equation 1 in the paper, page 6
in your presentation):

Ftot = Fc + ks*Fs*exp(-Bs*s^2/4)

which works great and is how things are usually coded in most
macromolecular software, no problems or arguments there.  However,
we can come from the opposite - but equivalent! - direction of
Babinet's principle, which tells us the bulk solvent can also be
modeled by inverting everything: set the bulk solvent region to 0 and
the protein region to 1 in the real space mask, apply a Fourier
transform to that and then invert the phase:

Ftot = Fc - ks*Fm*exp(-Bs*s^2/4)

(I'm using Fm to distinguish it from Fs, due to the inversion of 0's
and 1's in the real space mask)  This is equation 2 in the paper.

So we're still using the flat model to compute Fm, and we're using
Babinet's principle to add it in to the structure factors - although
its better described as adding the inverse (thus the minus sign in the
second equation) of the complement (Fm rather than Fs). These two
equations are exactly equivalent, without any loss of generality. So, I
would argue the flat model and Babinet's are very much congruous.  Also
take a look at the description/discussion in the paper regarding Figure
2 (which helped me think about things at first).

The big difference is that Babinet's is usually applied as:

Ftot = Fc - ks*Fc*exp(-Bs*s^2/4)

which, I would argue, isn't quite right - the bulk solvent doesn't
scatter like protein, but it does get the shape right.  Which I think
is why Fokine and Urzhumtsev point out that at high resolution this
form would start to show disagreement with the data.  I haven't looked
at this explicitly though, so we still haven't answered that question!
We didn't want to spend much time on it in the paper, our main goal was
to try out the differentiable models we describe.  The Babinet trick
was a convenient way to make coding easier.

Anyway, I hope this helps explain it a bit more, and again: sorry for
the long-windedness.

Regards,
Tim



--

***
Dirk Kostrewa
Gene Center Munich, A5.07
Department of Biochemistry
Ludwig-Maximilians-Universität München
Feodor-Lynen-Str. 25
D-81377 Munich
Germany
Phone:  +49-89-2180-76845
Fax:+49-89-2180-76999
E-mail: kostr...@genzentrum.lmu.de
WWW:www.genzentrum.lmu.de
***



Re: [ccp4bb] Fill map/mask with dummy atoms?

2010-10-18 Thread Dirk Kostrewa

 Dear colleagues,

many thanks for all of your kind support, following my request about 
placing dummy atoms into en EM-map! Here is a short summary:
Frederic Vellieux kindly offered me to use his programs with clever 
positioning of atoms in a density.
Paul Emsley pointed to a program findwaters, that comes with Coot, 
with option --flood to fill a density with waters.
John Tanner pointed to a USF program FLOOD from the VOIDOO packages for 
filling cavities with water.
Victor Lamzin sent me a script for ARP/wARP for placing dummy atoms into 
a map.
Alex Shkumatov pointed to two SAXS programs, em2dam and vol2pdb, to 
convert low resolution maps into dummy atoms.


Now, I have plenty of options to play with!

Best regards,

Dirk.

Am 13.10.10 13:49, schrieb Dirk Kostrewa:
 ... maybe, to clarifiy my question a little bit: I want to fill an 
essentially flat cryo-EM-map with dummy atoms. So, a peak search 
doesn't work. I would need a program that fills this map with dummy 
atoms for a few things that I want to try with this atomic 
representation.


Best regards,

Dirk.

Am 13.10.10 13:00, schrieb Dirk Kostrewa:

 Dear CCP4ers,

is there a program around that allows to fill an input map or mask 
with dummy atoms?


Best regards,

Dirk.





--

***
Dirk Kostrewa
Gene Center Munich, A5.07
Department of Biochemistry
Ludwig-Maximilians-Universität München
Feodor-Lynen-Str. 25
D-81377 Munich
Germany
Phone:  +49-89-2180-76845
Fax:+49-89-2180-76999
E-mail: kostr...@genzentrum.lmu.de
WWW:www.genzentrum.lmu.de
***


Re: [ccp4bb] Question regarding S-SAD

2010-10-18 Thread Dirk Kostrewa

 Dear Kornelius,

a few thoughts that come to my mind:

- Are you sure about the space group P6? For proteins, P6_1, P6_2, ..., 
P6_5 are more usual.


- Did you try both hands of the Se-sites? In case of space group P6_n, 
you have to invert both the handedness of the sites _and_ of the space 
group, resulting in P6_(6-n) (i.e. P6_5 instead of P6_1).


- I wouldn't worry about the mosaicity.

Best regards,

Dirk.

Am 18.10.10 14:03, schrieb Kornelius Zeth:

Dear all,

we have collected S-SAD data (2x4000 Frames, 0.1 degrees, wedges of 40 Frames, 
Rf between 3-5% overall) and received a dataset to 2.5 A which is complete with 
a redundancy of 30-40. Space group is P6 and the AU 120 residues, 6 Mets. 
Native data are up to 1.9 A Sharp and Phenix both return the expected number of 
sites and given the phasing power to approx. 3.8 A after HA refinement I was 
hoping to get some maps which I could use for tracing the structure. However 
DM, Solomon and Resolve all fail to significantly improve the phases and 
densities look not as if they can be traced. There is some partial twinning of 
15%. What I noticed was that the spot profiles in XDS looked not as the are 
supposed to, presumably because the mosaicity of the spots are 0.4-0.6 and spot 
integration may be hampered. Still, merging Rfactors are brilliant.

Any hints + ideas are welcome!

Best wishes

Kornelius

  --
  Kornelius Zeth
  Max Planck Institute for Developmental Biology
  Dept. Protein Evolution
  Spemannstr. 35
  72076 Tuebingen, Germany
  kornelius.z...@tuebingen.mpg.de
  Tel -49 7071 601 323
  Fax -49 7071 601 349


--

***
Dirk Kostrewa
Gene Center Munich, A5.07
Department of Biochemistry
Ludwig-Maximilians-Universität München
Feodor-Lynen-Str. 25
D-81377 Munich
Germany
Phone:  +49-89-2180-76845
Fax:+49-89-2180-76999
E-mail: kostr...@genzentrum.lmu.de
WWW:www.genzentrum.lmu.de
***


[ccp4bb] Fill map/mask with dummy atoms?

2010-10-13 Thread Dirk Kostrewa

 Dear CCP4ers,

is there a program around that allows to fill an input map or mask with 
dummy atoms?


Best regards,

Dirk.

--

***
Dirk Kostrewa
Gene Center Munich, A5.07
Department of Biochemistry
Ludwig-Maximilians-Universität München
Feodor-Lynen-Str. 25
D-81377 Munich
Germany
Phone:  +49-89-2180-76845
Fax:+49-89-2180-76999
E-mail: kostr...@genzentrum.lmu.de
WWW:www.genzentrum.lmu.de
***


[ccp4bb] Fwd: [ccp4bb] Fill map/mask with dummy atoms?

2010-10-13 Thread Dirk Kostrewa
 ... maybe, to clarifiy my question a little bit: I want to fill an 
essentially flat cryo-EM-map with dummy atoms. So, a peak search doesn't 
work. I would need a program that fills this map with dummy atoms for a 
few things that I want to try with this atomic representation.


Best regards,

Dirk.

Am 13.10.10 13:00, schrieb Dirk Kostrewa:

 Dear CCP4ers,

is there a program around that allows to fill an input map or mask 
with dummy atoms?


Best regards,

Dirk.



--

***
Dirk Kostrewa
Gene Center Munich, A5.07
Department of Biochemistry
Ludwig-Maximilians-Universität München
Feodor-Lynen-Str. 25
D-81377 Munich
Germany
Phone:  +49-89-2180-76845
Fax:+49-89-2180-76999
E-mail: kostr...@genzentrum.lmu.de
WWW:www.genzentrum.lmu.de
***


Re: [ccp4bb] Difference map

2010-09-29 Thread Dirk Kostrewa

 Hi Intekhab Alam,

an Fobs-Fobs' map usually works only if the two crystals are 
isomorphous, which means that there are neither large cell constant 
changes nor any other larger structural changes (like overall rotations, 
domain movements, other rearrangements) than the bound compound (ligand, 
heavy atom, ...). Scaleit produces a plot of Riso against resolution 
which ideally should resemble the scattering curve of the bound compound 
(~ like an atomic scattering curve for instance), plus a mild increase 
at high resolution due to the increasing noise component at higher 
resolution. If the curve starts at high Riso values and increases 
steeply, this would indicate anisomorphism, and there is probably no 
chance to detect your compound signal.
All this is qualitative, but you could estimate the expected change with 
the Crick-Magdoff equation by replacing the heavy atoms with a sum over 
your compound atoms. The Crick-Magdoff equations has been recently 
discussed on this board:

http://www.mail-archive.com/ccp4bb@jiscmail.ac.uk/msg10039.html

Good luck,

Dirk.

Am 29.09.10 09:09, schrieb intekhab alam:

Hi Folks
I have a query regarding the difference map between the two structures 
ligand bound data (2.5A) and native (2.8A).
I tried to calculate the fourier difference map between two data sets 
ligand bound- native.

The protocol in CCP4 that i used is as:
1.merge the mtz file of native nad ligand bound using cad
2. scaling this combine file with scaleit program followed by map 
generation uisng fft.
I got the map but i did not find the fu;ll map of the ligand,i can 
only see small density nera the ligand binding site at 5 sigma level.

 I have calculated omit map that cleraly showed the ligand.
why is such discrepency in the two cases, is there is something 
missing from the calculation. kindly help me out.

Thanks and regards
Intekhab alam
--
INTEKHAB ALAM
LABORATORY OF STRUCTURAL BIOINFORMATICS
KOREA UNIVERSITY, SEOUL


--

***
Dirk Kostrewa
Gene Center Munich, A5.07
Department of Biochemistry
Ludwig-Maximilians-Universität München
Feodor-Lynen-Str. 25
D-81377 Munich
Germany
Phone:  +49-89-2180-76845
Fax:+49-89-2180-76999
E-mail: kostr...@genzentrum.lmu.de
WWW:www.genzentrum.lmu.de
***


Re: [ccp4bb] Effect of NCS on estimate of data:parameter ratio

2010-09-21 Thread Dirk Kostrewa

 Dear Ian,

many thanks for your explanations - they've changed my view! I was 
always a bit puzzled by the supposedly contradictory transition between 
restraints and constraints with increasing weight, which has been 
clarified by their effect on the number of parameters, and not on the 
number of observations.


Interestingly, in your Acta Cryst paper, restraints are also counted as 
observations (for instance, in Table 1 and §2.3), but in the derived 
residuals and ratios, it's clear that they reduce the effective number 
of parameters.


Best regards,

Dirk.

Am 20.09.10 13:22, schrieb Ian Tickle:

Hi Dirk

First, constraints are just a special case of restraints in the limit
of infinite weights, in fact one way of getting constraints is simply
to use restraints with very large weights (though not too large that
you get rounding problems). These 'pseudo-constraints' will be
indistinguishable in effect from the 'real thing'.  So why treat
restraints and constraints differently as far as the statistics are
concerned: the difference is purely one of implementation.

Second, restraints are not interchangeable 1-for-1 with X-ray data as
far as the statistics are concerned: N restraints cannot be considered
as equivalent to N X-ray data, which would be the implication of
adding together the number of restraints and the number of X-ray data.

This can be seen in the estimation of the expected values of the
residuals (chi-squared) for the working  test sets, which are used to
estimate the expected Rfree.  If you take a look at our 1998 AC paper
(D54, 547-557), Table 2 (p.551), the last row of the table (labelled
'RGfree/RG') shows the expected residuals for the working set
(denominator) and test set (numerator) for the cases of no restraints,
restrained and constrained refinement:

No restraints (or constraints):

Dwork  = f - m
Dfree   = f + m

Restrained:

Dwork  = f - (m - r + Drest)
Dfree   = f + (m - r + Drest)

Constrained:

Dwork  = f - (m - r)
Dfree   = f + (m - r)

where:

Dwork  = expected working set residual (chi-squared),
Dfree  = expected test set residual (chi-squared),
f   = no of reflections in working set,
m = no of parameters,
r   = no of restraints and/or constraints,
Drest = restraint residual (chi-squared).

The constrained case is obviously just a special case of the
restrained case with Drest = 0, i.e. in the constrained case the
difference between the refined and target values is zero, and the 'no
restraints' case is a special case of this with r = 0.  We can
generalise all of this by writing simply:

Dwork  = f - m'
Dfree   = f + m'

where m' is the effective no of parameters corrected for restraints
and/or constraints (m' = m - r + Drest); the effective no of
parameters is reduced whether you're using restraints or constraints.
In the case where you had both restraints and constraints r would be
the total no of restraints + constraints, however constraints
contribute nothing to Drest.  The 'effectiveness' of a restraint
depends on its contribution to Drest (Z^2), a smaller value means it's
more effective.  A contribution of Z^2 = 1 to Drest completely cancels
the effect of increasing r by 1 by adding the restraint (i.e. the
restraint has no effect).

This incidentally shows that the effect of over-fitting (adding
redundant effective parameters) is to reduce the working set and
increase the test set residuals.  If you consider the working set
residual in the general case:

Dwork  = f - (m - r + Drest) = f + r - m - Drest

it certainly appears from this that the number of X-ray data (f) and
the number of restraints (r) are being added.

However if you consider the test set residual:

Dfree   = f + (m - r + Drest) = f - r + m + Drest

this is clearly not the case.  All you can say is that the effective
number of parameters is reduced by the number of restraints +
constraints.

Cheers

-- Ian

On Mon, Sep 20, 2010 at 9:20 AM, Dirk Kostrewa
kostr...@genzentrum.lmu.de  wrote:

  Hi Ian,

Am 19.09.10 15:25, schrieb Ian Tickle:

Hi Florian,

Tight NCS restraints or NCS constraints (they are essentially the same
thing in effect if not in implementation) both reduce the effective
parameter count on a 1-for-1 basis.

Restraints should not be considered as being added to the pool of
X-ray observations in the calculation of the obs/param ratio, simply
because restraints and X-ray observations can in no way be regarded as
interchangeable (increasing the no of restraints by N is not
equivalent to increasing the no of reflections by N).  This becomes
apparent when you try to compute the expected Rfree: the effective
contribution of the restraints has to be subtracted from the parameter
count, not added to the observation count.

I always understood the difference between constraints and restraints such,
that a constraint reduces the number of parameters by fixing certain
parameters, whereas restraints are target values for parameters and as such
can be counted as observations, similarly

Re: [ccp4bb] Effect of NCS on estimate of data:parameter ratio

2010-09-20 Thread Dirk Kostrewa

 Hi Ian,

Am 19.09.10 15:25, schrieb Ian Tickle:

Hi Florian,

Tight NCS restraints or NCS constraints (they are essentially the same
thing in effect if not in implementation) both reduce the effective
parameter count on a 1-for-1 basis.

Restraints should not be considered as being added to the pool of
X-ray observations in the calculation of the obs/param ratio, simply
because restraints and X-ray observations can in no way be regarded as
interchangeable (increasing the no of restraints by N is not
equivalent to increasing the no of reflections by N).  This becomes
apparent when you try to compute the expected Rfree: the effective
contribution of the restraints has to be subtracted from the parameter
count, not added to the observation count.


I always understood the difference between constraints and restraints 
such, that a constraint reduces the number of parameters by fixing 
certain parameters, whereas restraints are target values for parameters 
and as such can be counted as observations, similarly to the Fobs, which 
are target values for the Fcalc (although with different weights). I 
don't see what is wrong with this view. Do I misunderstand something?


Best regards,

Dirk.


The complication is that a 'weak' restraint is equivalent to less than
1 parameter (I call it the 'effective no of restraints': it can be
calculated from the chi-squared for the restraint).  Obviously no
restraint is equivalent no parameter, so you can think of it as a
continuous sliding scale from no restraint (effective contribution to
be subtracted from parameter count = 0) through weak restraint (0
contribution  1) through tight restraint (count ~=1) to constraint
(count = 1).

Cheers

-- Ian

On Sat, Sep 18, 2010 at 9:23 PM, Florian Schmitzberger
schmitzber...@crystal.harvard.edu  wrote:

Dear All,

I would have a question regarding the effect of non-crystallographic
symmetry (NCS) on the data:parameter ratio in refinement.

I am working with X-ray data to a maximum resolution of 4.1-4.4 Angstroem,
79 % solvent content, in P6222 space group; with 22 300 unique reflections
and expected 1132 amino acid residues in the asymmetric unit, proper 2-fold
rotational NCS (SAD phased and no high-resolution molecular replacement or
homology model available).

Assuming refinement of x,y,z, B and a polyalanine model (i.e. ca. 5700
atoms), this would equal an observation:parameter ratio of roughly 1:1. This
I think would be equivalent to a normal protein with 50 % solvent content,
diffracting to better than 3 Angstroem resolution (from the statistics I
could find, at that resolution a mean data:parameter ratio of ca. 0.9:1 can
be expected for refinement of x,y,z, and individual isotropic B; ignoring
bond angle/length geometrical restraints at the moment).

My question is how I could factor in the 2-fold rotational NCS for the
estimate of the observations, assuming tight NCS restraints (or even
constraint). It is normally assumed NCS reduces the noise by a factor of the
square root of the NCS order, but I would be more interested how much it
adds on the observation side (used as a restraint) or reduction of the
parameters (used as a constraint). I don't suppose it would be correct to
assume that the 2-fold NCS would half the number of parameters to refine
(assuming an NCS constraint)?

Regards,

Florian

---
Florian Schmitzberger
Biological Chemistry and Molecular Pharmacology
Harvard Medical School
250 Longwood Avenue, SGM 130
Boston, MA 02115, US
Tel: 001 617 432 5602



--

***
Dirk Kostrewa
Gene Center Munich, A5.07
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Ludwig-Maximilians-Universität München
Feodor-Lynen-Str. 25
D-81377 Munich
Germany
Phone:  +49-89-2180-76845
Fax:+49-89-2180-76999
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***


Re: [ccp4bb] Deposition of riding H: R-factor is overrated

2010-09-17 Thread Dirk Kostrewa

 Hi Pavel,


Am 16.09.10 17:56, schrieb Pavel Afonine:

 Hi Dirk,

so, wouldn't be the deposition of the final model's Fcalc, Phic (and 
their weights) along with the final coordinates be the best solution? 
The final Fcalc are our best model and can be used to reproduce the 
final statistics (which would remove the sfcheck annoyance) and to 
reproduce the final electron density maps, and the coordinates can be 
used for what ever purpose they are needed, irrespective of adding 
riding hydrogens or not.


it is a great idea and if you look in PDB deposited structure factors 
there is a number of them (but certainly not the majority) that are 
accompanied by Fcalc. However, a few things to keep in mind:


- Imagine a (not very uncommon, unfortunately) situation when someone 
obtains the final model and Fcalc, and then, right before the PDB 
deposition does a final check in Coot, and moves/removes a few atoms 
(a few waters, or instance) here and there. Or may be does a 
real-space fit of a residue. Or removes H, if present. Or renames a 
ligand by request of PDB staff and accidentally change an atom 
parameter(s). All this in turn will invalidate the R-factors and make 
previously calculated Fcalc inconsistent with such a manipulated model.
So, the bottom-line is: having a model that you can use to reproduce 
the reported statistics is important (for validation and database 
sanity at least, if someones believe that such a minor things wouldn't 
impair the biological interpretation - ultimate goal of protein 
structures).
but this is exactly what one shouldn't do: manipulate the structure 
after the final refinement! And if you manipulate it for a good reason, 
do a last final refinement after that, before depositing coordinates 
and structure factors. Then, there will be no problems, as far as I can see.


Best regards,

Dirk

--

***
Dirk Kostrewa
Gene Center Munich, A5.07
Department of Biochemistry
Ludwig-Maximilians-Universität München
Feodor-Lynen-Str. 25
D-81377 Munich
Germany
Phone:  +49-89-2180-76845
Fax:+49-89-2180-76999
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***


Re: [ccp4bb] Deposition of riding H: R-factor is overrated

2010-09-16 Thread Dirk Kostrewa

 Dear Ian and contributors to this interesting thread,

(please, scroll down a little bit)

Am 15.09.10 23:34, schrieb Ian Tickle:

I should just like to point out that the main source of the
disagreement here seems to be that people have very different ideas
about what a 'model' is or should be.  Strictly a model is a purely
mathematical construct, in this case it consists of the appropriate
equation for the calculated structure factor and the best-fit values
of the various parameters (scattering factors, atomic positions,
occupancies, B factors, TLS parameters etc.) that appear in it. A
mathematical model is inevitably going to be an imperfect
representation of reality, but hopefully it's the best one we can come
up with, in the sense of best explaining the data without significant
overfitting.

The problem arises because many users of the PDB, and I suspect many
contributors to this BB, particularly non-crystallographers, don't see
it like that, because they view a PDB file as a physical model, i.e.
not as the best fit to the data (assuming that the
non-crystallographers even know what the data are!), but the closest
representation of reality.  The difference between the N-H bond
lengths that Ed referred to illustrates the distinction between the
mathematical and the physical model.  The mathematical model requires
that the bond length is 0.86 Ang because that value gives the best fit
of the assumed spherical scattering factor of H to the deformation
density of the X-H covalent bond.  The physical model requires that it
be 1.00 Ang because that is the internuclear distance found by
spectroscopic methods  predicted by QM calculations.  The same goes
for B factors and TLS: to a large extent they are a mathematical
construct whose purpose is to provide an optimal fit to the data.  The
connection of Bs  TLS with reality is tenuous at best, nevertheless
people obviously would like to have a physical interpretation such as
rigid-body correlated motion.  The fact that Bragg scattering provides
no information about correlated motion (you need to measure the
diffuse scattering for that) doesn't seem to deter them!

I have no doubt in my mind that it is the mathematical model that
should be published, because hopefully it's the best available
interpretation of the data.  Whether that involves publishing the
riding H atoms explicitly, or alternatively the formulae and
parameters that were used to calculate their positions I don't mind,
as long as I can faithfully reproduce the Fcalcs to check the validity
of the model.  Then users of the PDB are free to *interpret* the
mathematical models as physical models in a appropriate manner (e.g.
by adjusting the bond lengths to H), and crystallographers have the
untainted mathematical models needed to reproduce the Fcalcs.


so, wouldn't be the deposition of the final model's Fcalc, Phic (and 
their weights) along with the final coordinates be the best solution? 
The final Fcalc are our best model and can be used to reproduce the 
final statistics (which would remove the sfcheck annoyance) and to 
reproduce the final electron density maps, and the coordinates can be 
used for what ever purpose they are needed, irrespective of adding 
riding hydrogens or not.


Best regards,

Dirk.

--

***
Dirk Kostrewa
Gene Center Munich, A5.07
Department of Biochemistry
Ludwig-Maximilians-Universität München
Feodor-Lynen-Str. 25
D-81377 Munich
Germany
Phone:  +49-89-2180-76845
Fax:+49-89-2180-76999
E-mail: kostr...@genzentrum.lmu.de
WWW:www.genzentrum.lmu.de
***


Re: [ccp4bb] Molecular replacement question

2010-09-14 Thread Dirk Kostrewa

 Dear Paul Holland,

I would spend some time in improving the search model, first. If there 
are more than one possible search molecules in the PDB, I usually do a 
structural alignment (ssm superposition) to get an idea about the 
flexibility of the search molecules. Then I remove all parts that I 
suspect to be flexible (usually N- and C-termini, long loops), until I 
get a very compact search model. You may try a model with no side-chain 
truncation, since in the hydrophobic core, there might be a similar 
isosteric packing of atoms. In addition, I would truncate the side 
chains either to the longest common chain (with ctruncate) if there is a 
good sequence alignment, or to poly-Ser or even poly-Ala. I would try 
these core-models as search models, with the idea that missing atoms 
lower the signal, but wrong atoms raise the noise and may produce wrong 
clashes. In case of several search models, where each individual model 
fails, you may try to run Phaser using all of them simultaneously as a 
search ensemble.
This model-pruning together with a search-ensemble of several PDB 
entries worked recently in a project, where otherwise all molecular 
replacement trials failed.


Good luck,

Dirk.

Am 13.09.10 16:52, schrieb Paul Holland:

Hello fellow crystallographers,

I am trying molecular replacement for a protein crystal dataset that has very 
high sequence similarity to the search model with several predicted flexible 
loop regions; however, all attempts at finding a solution have not produce very 
ideal starting solutions using Phaser and Molrep (CC = 0.3 and Z-score = 5).  I 
am very confident that the unit cell parameters are C2 84.027  120.565  108.272 
 90.00 104.71  90.00, and there appears to be no evidence of twinning.  The 
Matthews calculation predicts from anywhere from 2-4 monomers in the ASU, and 
calculation of the SRF in Molrep does not identify any peaks in higher order 
symmetry except for the expected crystallographic two-fold for C2.  Below is 
the table from the calculated SRF in molrep.  Any advice would be greatly 
appreciated.

#thetaphichi alpha   beta  gamma Rf 
Rf/sigma
Sol_RF   1 0.000.000.000.000.000.00 870.5   
   21.59
Sol_RF   258.61  -10.17  180.00  169.83 -117.23   10.17 162.5  4.03
Sol_RF   366.02   -0.00  180.00  180.00 -132.030.00 161.1  4.00
Sol_RF   458.42   -9.54  180.00  170.46 -116.859.54 159.8  3.96
Sol_RF   5   149.840.00  180.00 -180.00   60.320.00 156.0  3.87
Sol_RF   658.96   -5.52  180.00  174.48 -117.915.52 151.5  3.76
Sol_RF   765.59   20.95  180.00   20.95  131.18  159.05 143.9  3.57
Sol_RF   890.00  -98.96  180.000.00  180.00   17.92 142.9  3.55
Sol_RF   956.53   15.78  180.00   15.78  113.07  164.22 142.0  3.52
Sol_RF  1071.10  -19.94  180.00  160.06 -142.20   19.94 141.6  3.51
Sol_RF  1171.28   29.78  180.00   29.78  142.55  150.22 140.4  3.48
Sol_RF  1265.22  -15.88  180.00  164.12 -130.44   15.88 139.2  3.45
Sol_RF  1368.84   -0.00  180.00  180.00 -137.670.00 138.0  3.42
Sol_RF  1432.51 -180.00  180.00 -180.00   65.02   -0.00 137.9  3.42
Sol_RF  1575.02  -28.84  180.00  151.16 -150.04   28.84 134.7  3.34
Sol_RF  1671.69  -20.99  180.00  159.01 -143.37   20.99 133.0  3.30
Sol_RF  1792.13  101.46  179.93  102.35 -175.74   79.42 130.9  3.25
Sol_RF  18   107.89  144.73  179.79  145.06 -144.22   35.61 128.8  3.19
Sol_RF  1987.45  -78.19  180.00  101.81 -174.90   78.19 128.1  3.18
Sol_RF  2038.570.69   30.36  102.66  -18.79  -78.71 122.4  3.04
Sol_RF  2126.77  174.59  176.58  172.68   53.523.49 120.5  2.99
Sol_RF  22   116.66  178.08  175.143.49  126.48  187.32 120.5  2.99
Sol_RF  2375.56  -41.35  180.00  138.65 -151.12   41.35 119.8  2.97
Sol_RF  2466.12   36.35  180.00   36.35  132.24  143.65 116.6  2.89
Sol_RF  2583.87   71.62  180.00   71.62  167.74  108.38 114.7  2.85
Sol_RF  2669.24  -12.37  180.00  167.63 -138.48   12.37 112.3  2.79
Sol_RF  2759.75   15.26  172.297.64  119.07  157.12 112.2  2.78
Sol_RF  28   120.25 -164.74  172.29   22.88  119.07  172.36 112.2  2.78
Sol_RF  2996.68  -70.99  180.00  109.01 -166.63   70.99 110.9  2.75
Sol_RF  3063.23  -44.73  180.00  135.27 -126.47   44.73 108.9  2.70

Cheers,

Paul Holland




--

***
Dirk Kostrewa
Gene Center Munich, A5.07
Department of Biochemistry
Ludwig-Maximilians-Universität München
Feodor-Lynen-Str. 25
D-81377 Munich
Germany
Phone:  +49-89-2180-76845
Fax:+49-89-2180-76999
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***


Re: [ccp4bb] Practical MR advice

2010-09-01 Thread Dirk Kostrewa

 Hi Roger,

personally, I would take the four dimers from Phaser, strip off all side 
chains (make a poly-ala/gly), do a ML refinement with tight NCS 
restraints. The resulting map could then be on-the-fly 
real-space-averaged with Coot. At your resolution, I would expect to see 
the real register of at least some side chains either in the 2mfodfc-map 
or in one of the real-space-averaged 2mfodfc-maps.


Good luck,

Dirk.

Am 01.09.10 17:12, schrieb Roger Rowlett:
I am trying to find a MR solution for a large unit cell (R3:H, 
158x158x196) with a relatively poor, but I think workable search model 
(30% identity, 50% similarity). The data set is decent to 2.4 A. I 
might be able to get better if necessary. I submitted the  sequence of 
the target to the Phyre server, and it returned a PDB file derived 
from what I had already identified as the most likely successful 
search model. Phaser finds a reasonable solution with four dimers 
(Z=9-15 depending on the data set) for which the unit cell packing 
looks good. Phaser even assembles what looks like correct biological 
tetramers in the ASU and across the symmetry interfaces. The main 
chain appears to be mostly traceable, but the side chains are not all 
well-resolved, and I suspect from the better-defined regions, that the 
chain is misregistered by a residue or two throughout most of the 
structure.


Assuming that an MR solution is possible, what is a good approach from 
here? FWIW, Phaser does not correctly place a poly-Ala/Gly model, 
although it may place three chains similarly to the MR solution I have 
with the Phyre model. My first thought is to:


1. Chainsaw the currrent solution, and attempt to identify and build 
in the correct register of the side chains. after refinement.
2. Do a low resolution refinement of the poly-Ala/Gly model to better 
thread the main chain?

3. Try EPMR with the Phyre model or the poly-Ala/Gly model
4. Give up and get real phases (but I'm so close now!?)

Thanks in advance.

--
Roger S. Rowlett
Professor
Department of Chemistry
Colgate University
13 Oak Drive
Hamilton, NY 13346

tel: (315)-228-7245
ofc: (315)-228-7395
fax: (315)-228-7935
email: rrowl...@mail.colgate.edu mailto:rrowl...@mail.colgate.edu


--

***
Dirk Kostrewa
Gene Center Munich, A5.07
Department of Biochemistry
Ludwig-Maximilians-Universität München
Feodor-Lynen-Str. 25
D-81377 Munich
Germany
Phone:  +49-89-2180-76845
Fax:+49-89-2180-76999
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***



Re: [ccp4bb] which software can calculate binding energy

2010-07-23 Thread Dirk Kostrewa

 Dear Min,

in addition to what Greg Warren wrote, to my knowledge, there is still a 
big uncertainty in the calculation of desolvation energies. A colleague 
of mine, a theoretical physicist, when I was at Hoffmann-La Roche, tried 
to calulcate the desolvation energy contribution to the total binding 
energy of drug compounds to protein active sites, and estimated that the 
errors in the desolvation energies had about the same magnitude as the 
total net binding energy. So, this is another big source of inaccuracy, 
especially with very different drug compounds.


Best regards,

Dirk.

Am 22.07.10 23:13, schrieb Greg Warren:


Dear Min,

There is no software that can accurately calculate the binding energy 
of a predicted (docking) or solved (X-ray structure) protein-ligand 
complex particularly for ligands that are different chemically -- not 
part of a congeneric  series.While there are a number of 
publications on methods (LIE, FEP, MD, MMPB(GB)SA, QM/MM, even 
semi-empirical QM methods) for predicting binding energy, most of 
these publication show results for congeneric series compounds not 
chemically diverse ligands which is the result you will get from 
screening a chemical database with Autodock.  There are publications 
by SP Brown J Chem Inf Model. 2007 Jul-Aug;47(4):1493-503, J Chem Inf 
Model. 2006 May-Jun;46(3):999-1005 using MMPBSA showing a correlation 
between predicted and measured binding energy of around 0.8.  The 0.8 
correlation may not be in the papers but might have only been shown in 
presentations given by Scott.  If you are looking for accurate 
predictions a 0.8 correlation is not very accurate.  If you were 
thinking about using docking scores, a publication that looked at 
using docking scores to predict binding energy is Warren et al. J Med 
Chem 2006, 49, 5912.  The last third of this publication showed that 
using docking scores to predict binding energy was a very bad idea 
even for congeneric series.


Regards,

Greg

*From:* CCP4 bulletin board [mailto:ccp...@jiscmail.ac.uk] *On Behalf 
Of *WEI MIN

*Sent:* Thursday, July 22, 2010 1:51 PM
*To:* CCP4BB@JISCMAIL.AC.UK
*Subject:* [ccp4bb] which software can calculate binding energy

Dear All

I have been using the Autodock software for docking the drug candidate 
compounds into the receptor structures. I would like to calculate 
accurately the binding energy. Would anyone introduce me a software?


Any help would be greatly appreciated.

Best

Min



--

***
Dirk Kostrewa
Gene Center Munich, A5.07
Department of Biochemistry
Ludwig-Maximilians-Universität München
Feodor-Lynen-Str. 25
D-81377 Munich
Germany
Phone:  +49-89-2180-76845
Fax:+49-89-2180-76999
E-mail: kostr...@genzentrum.lmu.de
WWW:www.genzentrum.lmu.de
***



Re: [ccp4bb] differences Rfactor calculations

2010-07-14 Thread Dirk Kostrewa
 ... yes, and this is the reason why sfcheck should be replaced by a 
more modern program at the Protein Data Bank!


Best regards,

Dirk.

Am 13.07.10 22:15, schrieb Ethan Merritt:

Should be in an FAQ somewhere:
Q: Why does sfcheck not reproduce my original R factors?
A: Because instead of using the Fc in your file, sfcheck tries to
re-calculate Fc using only your atom names, coordinates and isotropic
B factors.  This is bad, because it ignores any contributions to your
original Fc from things like F_partial, Anisotropic corrections,
TLS models, scattering factor corrections, riding hydrogens, etc.

My advice is to use sfcheck only to evaluate the Fobs file resulting from
your data collection. It is not a suitable tool for validating a refined
model.



The same happened when I used this final model as starting model for a
refinement with Refmac5. Again I got an Rfactor of 20.8%.

Probably you failed to describe the full model to refmac.
Refmac and phenix.refine can both handle all the contributing factors
listed above, but it may take some work to pick a the correct
corresponding set of options.


Ethan



As far as I know, Phenix uses different algorithms for the refinement
than other programs, which in some cases can make Phenix gets better
Rfactors. Could these differences be the reason for this large
difference in the calculated Rfactors? Or I have to recheck my procedure
for mistakes?

Thanks a lot in advanced.
Looking forward to hearing form you.

Cheers,
Ariel



--

***
Dirk Kostrewa
Gene Center Munich, A5.07
Department of Biochemistry
Ludwig-Maximilians-Universität München
Feodor-Lynen-Str. 25
D-81377 Munich
Germany
Phone:  +49-89-2180-76845
Fax:+49-89-2180-76999
E-mail: kostr...@genzentrum.lmu.de
WWW:www.genzentrum.lmu.de
***


Re: [ccp4bb] conversion of cyroEM reconstruction from MRC to CCP4 format

2010-07-13 Thread Dirk Kostrewa

 Hi James,

I had similar problems with MRC maps. As a solution, a colleague of 
mine, working with EM, read the MRC map into SPIDER and saved it as a 
CCP4 map. That worked for me. Unfortunately, my colleague is absent for 
some time, and I'm still not familiar with EM software. But maybe, you 
find a colleague at your institute to help you with that.


Good luck,

Dirk.

Am 13.07.10 14:32, schrieb James Whittle:

Hi all-

I'm trying to convert a cryoEM map from FREALIGN for use with various 
CCP4 programs, or with MAPMAN. Even though the MRC format is derived 
from the CCP4 map file format, every program I've tried fails to open 
it, (except for Chimera which displays the map but cannot save it to 
another format for lack of memory).


For example, in MAPMASK I get the error:

 CCP4 library signal ccp4_map:No associated header (Error)
 raised in ccp4_cmap_open 
 CCP4 library signal ccp4_map:Cannot open file (Error)
 raised in MRDHDS 

or with MAPMAN:

 **CCPOPN ERROR**  FORMATTED  OLD file open failure on unit   1
 Logical name: DLP_100.map, File name: DLP_100.map
 Cannot send after transport endpoint shutdown

 ERROR --- While reading map header. Sorry !
 ERROR --- While opening map file



Is there a way to re-write the header to be compatible with CCP4?

--James


--

***
Dirk Kostrewa
Gene Center Munich, A5.07
Department of Biochemistry
Ludwig-Maximilians-Universität München
Feodor-Lynen-Str. 25
D-81377 Munich
Germany
Phone:  +49-89-2180-76845
Fax:+49-89-2180-76999
E-mail: kostr...@genzentrum.lmu.de
WWW:www.genzentrum.lmu.de
***


Re: [ccp4bb] Question about R/Rfree value difference

2010-07-09 Thread Dirk Kostrewa

 Hi Tom,

very nice tool! It would be good to get numerical values of the plotted 
distributions as well, like mean, median, standard deviation and so on.


Best regards,

Dirk.

Am 08.07.10 15:20, schrieb Tom Oldfield:

Sampath

With regard to your question on what sort of statistics you should get 
within

structure determination you might find this service at the PDBe useful :
http://www.ebi.ac.uk/pdbe-as/pdbestatistics/PDBeStatistics.jsp

You can view and manipulate distributions of R, Rfree and R-Rfree along
within many other data distributions from Xray (also NMR/EM) during
structure determination.  There are also links (clicking the graph) 
that list

all the depositions that have a particular value within the distribution.

I agree with Pavel that from your quoted statistics that it would be 
un-wise to deposit
the structure in the current state of refinement as there is clearly 
an issue.


Regards
Tom Oldfield


Hi Sampath,

this is how the distribution of Rwork, Rfree and Rfree-Rwork look 
like for 'all' PDB structures refined at around 2A resolution. The 
 indicates where your structure stands with respect to this 
distribution.


Histogram of Rwork for models in PDB at resolution 1.90-2.10 A:
 0.093 - 0.118  : 2
 0.118 - 0.143  : 35
 0.143 - 0.168  : 390
 0.168 - 0.193  : 1439
 0.193 - 0.218  : 1802  your structure
 0.218 - 0.242  : 785
 0.242 - 0.267  : 159
 0.267 - 0.292  : 14
 0.292 - 0.317  : 1
 0.317 - 0.342  : 1
Histogram of Rfree for models in PDB at resolution 1.90-2.10 A:
 0.149 - 0.170  : 10
 0.170 - 0.191  : 116
 0.191 - 0.213  : 534
 0.213 - 0.234  : 1166
 0.234 - 0.255  : 1417
 0.255 - 0.276  : 942
 0.276 - 0.297  : 343
 0.297 - 0.319  : 78
 0.319 - 0.340  : 17  your structure
 0.340 - 0.361  : 5
Histogram of Rfree-Rwork for all model in PDB at resolution 1.90-2.10 A:
 0.001 - 0.011  : 41
 0.011 - 0.021  : 230
 0.021 - 0.031  : 724
 0.031 - 0.041  : 1210
 0.041 - 0.050  : 1206
 0.050 - 0.060  : 654
 0.060 - 0.070  : 318
 0.070 - 0.080  : 160
 0.080 - 0.090  : 56
 0.090 - 0.100  : 29

So, it seems your case is the example of typical overfitting, which 
means the model parameterization or/and the refinement strategy is 
not good for your data and model.


If you send me the data and model files then I will be able 
(hopefully) to suggest a better refinement strategy or explaine why 
it's not feasible with available tools. All files will be kept 
confidentially.


The histograms above are obtained using this command from PHENIX family:

phenix.r_factor_statistics 2.0

Good luck!
Pavel.


On 7/7/10 10:17 PM, Sampath Natarajan wrote:

Dear all,

I have a question about the R free value. I refined a structure with 
2A resolution. After model building and restraint refinement using 
Refmac program, the average B factor was around 50 for all atoms. 
The R/Rfree were around 22/34. Then used the TLS refinement choosing 
entire molecule. Then R/Rfree reduced as 20/32. But the average B 
factor was reduced as 30. The R/Rfree difference is about 12% in 
final refinement. I feel it is significantly higher.


Could any one suggest me to reduce the Rfree value more? or is it 
good to submit the data in the PDB database with this 12% difference?


Thanks for the suggestions.

Sincerely,
Sampath N


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Re: [ccp4bb] R values are higher in SF-CHECK

2010-07-06 Thread Dirk Kostrewa

 Hello Rakesh,

yes, you are right. In contrast to all modern refinement programs, 
sfcheck neither applies TLS nor the superior mask bulk solvent 
correction (it applies the Babinet bulk solvent correction by 
double-exponential scaling). As a result, the R-factors from sfcheck are 
higher than those from the refinement program.
Annoyingly, I have to discuss/explain this discrepancy in R-factors 
every time when I want to deposit a refined X-ray structure with the 
Protein Data Bank ...


Best regards,

Dirk.

Am 06.07.10 17:05, schrieb Rakesh Joshi:

Hello,

I refined my structures using REFMAC5 ( using TLS in combination ). When i used 
the SF-Check
program, my R-values are ~5% higher than in those reported by refmac. Is this
due to the fact that SF-check does bulk solvent calculations differently and
does not account for TLS refinement?

Also, when i used TLSANL to put in my total B factor in the pdb file I only get
3 sets of numbers instead of( what i expected) 6 sets(ie. last three entries have 
values=0).

For example:

ATOM246  C6   DA C  13 -29.692  15.902  14.379  1.00 36.42   C
ANISOU  246  C6   DA C  13 3267   5459   5110  0  0  0   C



Cheers
Rakesh

Graduate student
Purdue University


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Feodor-Lynen-Str. 25
D-81377 Munich
Germany
Phone:  +49-89-2180-76845
Fax:+49-89-2180-76999
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***


Re: [ccp4bb] Wilson B and Mean B factors

2010-07-01 Thread Dirk Kostrewa

 Dear Murugan,

at higher resolution, the Wilson plot captures mainly the contribution 
of atoms with lower B-factors which leads to a systematic 
underestimation of the true B-factor distribution. Accordingly, the 
average B-factor of refined structures tend to be higher then the Wilson 
B-factor, at least in my experience. In your case, it is the other way 
around. One possible problem could be, apart from the fit of the Wilson 
plot as James Holton suggested, that you have reflections at very low 
resolution with underestimated intensities due to cut overloads or 
measurement in the half-shadow of the beamstop. This would result in a 
too low overall B-factor for the model in order to try to fit the 
usually stronger low resolution reflections at the cost of the weaker 
high resolution data. One quick check of this hypothesis is to cut the 
low resolution at, say, 10 A instead of 50 A and run a test-refinement. 
If this results in more realistic model B-factors, you should have a 
closer look at the low resolution data and exclude the ill-measured ones.


Best regards,

Dirk.

Am 30.06.10 19:31, schrieb Vandu Murugan:

Dear all,
 If one could find a difference of more than 15  between Wilson B 
factor of the data ( 55) and Mean B factor of the structure, (30) what 
could be the possible reasons?  I am seeing it in my structure.  Could 
someone tell me why it could be?? Thanks in advance.


Yours faithfully,
Murugan


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Ludwig-Maximilians-Universität München
Feodor-Lynen-Str. 25
D-81377 Munich
Germany
Phone:  +49-89-2180-76845
Fax:+49-89-2180-76999
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Re: [ccp4bb] problem with coot

2010-06-30 Thread Dirk Kostrewa

 Dear Munan,

this is a question that should better go to the Coot mailing list. 
Anyway - it is difficult to say what the problem is, without more 
informations. It could be an X11 problem or a Coot installation problem. 
Generally, on Mac OS X, you don't have to start X11 manually or at login 
- there is a launchd daemon that automatically starts X11 if it is 
required. Also, you must not set any DISPLAY variable in your .bashrc, 
.bash_proflie or elsewhere.
The following works for me on Mac OS X: I've installed the precompiled 
Coot version for Mac OS X, kindly provided by Bill Scott (-Google), and 
I've installed the more up-to-date X11 from xquartz.macosforge.org (but 
this is not necessary). You may want to try this.


Good luck,

Dirk.

Am 30.06.10 10:48, schrieb Md. Munan Shaik:

Dear BB
I have a problem with coot opening, i tried to open but its not opended.
Then I found some other problem, X11 terminal is not opened on login 
(even its in the list on login items), if I open X11 and then tried to 
open coot still not working, I am using Macbook and the OS X is 
10.6.1. (coot is install to Applications and not source to tcsh 
terminal, as i preferred not to open from terminal).


if anybody have suggestion, please .

 thanking you all,
===
Md. Munan Shaik
Department of Biotehnology
School of Bioscience and Biotechnology
via G. Colombo 03
Padova 35131, Italy





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***
Dirk Kostrewa
Gene Center Munich, A5.07
Department of Biochemistry
Ludwig-Maximilians-Universität München
Feodor-Lynen-Str. 25
D-81377 Munich
Germany
Phone:  +49-89-2180-76845
Fax:+49-89-2180-76999
E-mail: kostr...@genzentrum.lmu.de
WWW:www.genzentrum.lmu.de
***



Re: [ccp4bb] measure of anamolous signal

2010-06-29 Thread Dirk Kostrewa

 Dear Murugan,

Am 29.06.10 11:05, schrieb Vandu Murugan:

Dear all,
   I have collected a 2.7 angstrom home source data with Cu-Kalpha 
source for a protein with 6 cysteines, with a multiplicity of around 
23.  I need to know, is there any significant anamolous signal present 
in the data set, since there is no good model for my protein.  Can any 
one tell, which program to run, and what parameter to see?  Thanks in 
advance.


cheers,
Murugan
estimating the quality of the anomalous signal is not trivial, and 
several quality indicators have been discussed (see for example Fu, Rose 
 Wang, Acta Cryst D60, 499-506 (2004), or Zwart, Acta Cryst D61, 
1437-1444 (2005)).


If you process your data with XDS, there are two quality indicators for 
the anomalous signal, given both in the CORRECT.LP and in the XSCALE.LP 
file. One is the correlation of anomalous differences between two 
randomly chosen subsets that should have the same anomalous difference 
due to crystallographic symmetry, called RANOM. The other describes the 
absolute anomalous difference divided by their standard deviation, 
called SIGANO. A typical rule of thumb (and the one that I use) is, that 
RANOM should be ~ 30%, and SIGANO should be ~ 1.2. However, these 
indicators might not be realistic (see references above) and therefore 
should be taken with a grain of salt.


Good luck,

Dirk.

--

***
Dirk Kostrewa
Gene Center Munich, A5.07
Department of Biochemistry
Ludwig-Maximilians-Universität München
Feodor-Lynen-Str. 25
D-81377 Munich
Germany
Phone:  +49-89-2180-76845
Fax:+49-89-2180-76999
E-mail: kostr...@genzentrum.lmu.de
WWW:www.genzentrum.lmu.de
***


Re: [ccp4bb] Snow leopard + NVidia quadro FX4500

2010-06-15 Thread Dirk Kostrewa

Dear Deena,

yes, I have a Mac Pro with an Nvidia FX 4500 running under 10.6.3. For 
me, all programs work more or less fine in hardware stereo (Pymol, Coot, 
Moloc, Chimera). I've done the following to get it working:


1. Connect the CRT monitor to the first DVI socket of the graphics card 
(the one further away from the 3-pin Mini-DIN)

2. Connect the TFT to the second DVI socket (in the middle)
3. Connect the emitter to the 3-pin Mini-DIN socket
4. Choose a resolution for the CRT that allows a refresh rate of 120 Hz
5. I've arranged the monitors such that the menu bar is on the TFT (you 
might want to change this, if you like)
6. Not necessary since 10.6, but I've installed the most recent X11 from 
xquartz.macosforge.org


You can start MacPyMOL or PyMOLX11Hybrid with the parameters -X 1800 -Y 
200 -S (you might want to play with the X,Y position) and switch pymol 
to stereo in the application (still required despite -S).
For me, it is necessary to start pymol on the CRT monitor with suitable 
X,Y parameters, since dragging a X11 stereo window from the TFT to the 
CRT could lead to a crash of your whole session.


Good luck,

Dirk.

Am 14.06.10 21:35, schrieb Deena Oren:

Hi all,

Does anyone have this combination of Nvidia FX4500 in a mac machine 
running 10.6 and if so is stereo working?
I am getting a messed up screen when using either coot in hardware 
stereo or pymol -S even without invoking the stereo command. Yet 
ccp4mg is working fine in stereo.


Thanks,

Deena
Deena Abells Oren, PhD
Manager, Structural Biology Resource Center
Rockefeller University
1230 York Avenue, Box 295
New York, NY 10065-6399
phone: 212- 327-7429
fax: 212-327-7389






--

***
Dirk Kostrewa
Gene Center Munich, A5.07
Department of Biochemistry
Ludwig-Maximilians-Universität München
Feodor-Lynen-Str. 25
D-81377 Munich
Germany
Phone:  +49-89-2180-76845
Fax:+49-89-2180-76999
E-mail: kostr...@genzentrum.lmu.de
WWW:www.genzentrum.lmu.de
***



Re: [ccp4bb] sigma cutoff for fitting waters in model

2010-04-21 Thread Dirk Kostrewa

Dear Tassos,

Am 19.04.10 17:31, schrieb Anastassis Perrakis:
snip

The sigma issue a bit more complicated.

What we call usually sigma is the root mean square deviation (rmsd) of 
the map.


Lets first recall, that the variation within the protein region is 
quite large, while the solvent is rather flat.


Now, lets take an 'extreme' example, of a protein with 80% solvent. 
The rmsd for that will be quite low,
since most of the AU is flat. Thus, I would argue that you might want 
to consider waters in relatively 'low sigma'levels.
Of course 80% solvent will also mean that most likely this protein 
will only diffract to low resolution,

so you should maybe not be putting any waters.

The inverse case argument also applies.

Similar issues, maybe more severe, come up for atom removal.

/snip

regarding fitting electron density maps: isn't it the other way around? 
Assume, that we have the same protein with the same absolute noise level 
(without F000/V) in the protein region and the same loop that's missing 
in the model with the same absolute density well above the protein 
region's noise level, and this protein crystallizes in two crystal 
forms, one with low solvent content and one with high solvent content. 
Let's also assume that the solvent regions are absolutely flat. Then, 
the rmsd of the total electron density in the unit cell will be lower 
for the crystal form with high solvent content and higher for the 
crystal form with low solvent content, as you said. However, if we want 
to interprete that missing loop above the noise level in the protein 
region, we would then have to contour the electron density map in the 
high solvent crystal form at a higher multiple of its rmsd value than in 
the low solvent crystal form to get to the same absolute electron 
density level. Is this true or did I misunderstand something?


Best regards,

Dirk.

--

***
Dirk Kostrewa
Gene Center Munich, A5.07
Department of Biochemistry
Ludwig-Maximilians-Universität München
Feodor-Lynen-Str. 25
D-81377 Munich
Germany
Phone:  +49-89-2180-76845
Fax:+49-89-2180-76999
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***


Re: [ccp4bb] Hydrogen Bond Restraints

2010-04-14 Thread Dirk Kostrewa

Dear Bradley,

a recent refinement of a protein complex at 4.3 A was stabilized by 
using hydrogen bond restraints in secondary structures [1] (described in 
the supplementary material). Subjectively, the additional restraints had 
a small positive effect on the electron density interpretability of 
parts that were missing in the model. Irrespective of that, the hydrogen 
bonds stabilized the known/expected secondary structural elements during 
refinement and had a positive effect on the Ramachandran plot (which is 
not an independent quality control anymore, as with all restraints).


Good luck,

Dirk.

[1] Nature 462, 323-330 (2009)

Am 14.04.10 15:41, schrieb Bradley Hintze:

I am looking for published examples where hydrogen bond restraints
were helpful in refinement. Can anyone point me to some papers?

   


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***
Dirk Kostrewa
Gene Center, A 5.07
Ludwig-Maximilians-University
Feodor-Lynen-Str. 25
81377 Munich
Germany
Phone:  +49-89-2180-76845
Fax:+49-89-2180-76999
E-mail: kostr...@genzentrum.lmu.de
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***


Re: [ccp4bb] How to show electron density map for my ligand in pymol, which is bound in the active site..??/

2010-04-13 Thread Dirk Kostrewa

Dear Hussain,

in the electron density example of this tutorial, the parameter 
carve=1.6 is used, which means that density is only shown within a 
radius of 1.6 A around atoms. This is usually done for clarity, but may 
give an unrealistic impression of the density quality. Here, you should 
carefully choose a radius that shows the density similar as in a plot 
without any carve parameter, while cutting away the density from the 
surrounding atoms that you don't want to show. I've made good 
experiences choosing a radius similar to the maximum resolution of your 
data as a starting point. The carve-radius should then be reported in 
the figure.


Good luck,

Dirk.

Am 13.04.10 15:40, schrieb Ed Pozharski:

Hussain,

http://137.189.50.96/kbwong/teaching/pymol/pymol_tutorial.html

which is the top hit when you google pymol electron density.  Using
google (and not to appear biased, other available search engines) is the
most valuable advice (per word) that you may possible get.

On Tue, 2010-04-13 at 18:33 +0530, Hussain Bhukyagps wrote:
   

Dear all,

How can i show electron density map for my ligand in pymol, which is
bound in the active site.
i uploaded map as .xplor extension to the map file..

thank u

Hussain


Send free SMS to your Friends on Mobile from your Yahoo! Messenger.
Download Now! http://messenger.yahoo.com/download.php
 


   


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Re: [ccp4bb] Phasing statistics

2010-04-12 Thread Dirk Kostrewa

Hi Tassos,

my personal opinion is, that I would like to see the usual phasing 
statistics. At least to me, they provide hints how well the structure 
was determined, analogous to the R-factor/Free-R-factor providing hints 
how well the structure was refined.


It would be good if SHELXE would print out those statistics before any 
density modification.


Best regards,

Dirk.

Am 12.04.10 13:10, schrieb Anastassis Perrakis:

Hi -

A year or so ago, I have asked as a referee somebody to provide for a 
paper the statistics for their heavy atom derivative dataset,
and for the phasing statistics. For some good reasons, they were 
unable to do that, and they (politely) asked me
'what would it change if you knew these, isn't the structure we 
present impeccable?'. Well, I think they were right.
Their structure was surely correct, surely high quality. After that 
incident and giving it some thought,
I fail to see why should one report e.g. PP or Rcullis, or why will I 
care what they were if the structure has a convincing Rfree and is 
properly validated.
If someone wants to cheat at the end of the day, its easy to provide 
two numbers, but its hard to provide a good validated model that 
agrees with the data.
(and, yes, you can also make up the data, but we have been there, 
haven't we?!?)


So, my question to that referee, likely being a ccp4bb aficionado that 
is reading this email, or to anyone else really, is:


What would it help to judge the quality of the structure or the paper 
if you know PP, Rcullis and FOM?


Best -

A.

PS Especially since you used SHELXE for phasing these statistics are 
utterly irrelevant, and possibly you could advice the referee to read 
a bit about how SHELXE works ... or go to one of the nice courses that 
George teaches ...


On Apr 12, 2010, at 10:37, Eleanor Dodson wrote:


You can feed the SHELX sites into phaser_er or CRANK both of which will
give this sort of information.

Or mlphare if you know how to set it up..

Eleanor


Harmer, Nicholas wrote:

Dear CCP4ers,

I've been asked by a referee to provide the phasing statistics for a 
SAD dataset that I used to solve a recent structure. Whilst I have 
been able to find a figure-of-merit for the data after phasing, I 
can't work out how to get any other statistics (e.g. phasing power 
or an equivalent or Rcullis). Does anyone know a good route to 
obtaining useful statistics to put in the paper for SAD data?


The structure solution was carried out using SHELX C/D/E and then 
ARP/wARP.


Thanks in advance,

Nic Harmer

=
Dr. Nic Harmer
School of Biosciences
University of Exeter
tel: +44 1392 725179



*P** **please don't print this e-mail unless you really need to*
Anastassis (Tassos) Perrakis, Principal Investigator / Staff Member
Department of Biochemistry (B8)
Netherlands Cancer Institute,
Dept. B8, 1066 CX Amsterdam, The Netherlands
Tel: +31 20 512 1951 Fax: +31 20 512 1954 Mobile / SMS: +31 6 28 597791






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Feodor-Lynen-Str. 25
81377 Munich
Germany
Phone:  +49-89-2180-76845
Fax:+49-89-2180-76999
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***



Re: [ccp4bb] Phenix version 1.6.1 released

2010-03-31 Thread Dirk Kostrewa

Dear Paul,

this is very interesting! From the list of changes, it appears that in 
version 1.6.1, you use a similar idea to implement hydrogen bonds via 
DSSP during refinement that I used to stabilize the 4.3 A refinement of 
Pol II in complex with TFIIB [1]:


CHANGE LOG for PHENIX distribution
==

Version 1.6.1
=
snip
- phenix.refine
  - much faster rotamer fixing
  - initial implementation of secondary structure restraints (hydrogen 
bonds)

- automatic assignment of sec. str. using KSDSSP (from UCSF CGL)
  - proper treatment of charges on metal ions for scattering factors
/snip

Could you please give more details of how this is implemented? What are 
your hydrogen bond target distances and sigmas? Do you update this list 
during refinement?
I used a simple list of additional 2.9 A target-bond-distances between 
N and O with a target sigma of 0.05 A. This list was determined with 
DSSP and a self-made Fortran95 program using a user-defined 
energy-threshold prior to refinement and was kept constant during 
refinement.


Personally, I think, using secondary structure hydrogen bonds should be 
an option in every refinement program, especially at lower resolution!!! 
The BUSTER Wiki describes the procedure that I used. For REFMAC, I 
haven't seen anything similar, yet.


Very exciting!

Best regards,

Dirk.

[1] Nature 462, 323-330, (2009)

Am 31.03.10 04:41, schrieb Paul Adams:
The Phenix developers are pleased to announce that version 1.6.1 of 
Phenix is now available. Binary installers for Linux, and Mac OSX 
platforms are available at the download site:


http://phenix-online.org/download/

Just some of the new features in this version (1.6.1) are:

- Fast automated rotamer fixing in phenix.refine
- Use of atomic charge in calculation of scattering factors
- New Graphical User Interfaces for phenix.superpose_pdbs, 
phenix.get_cc_mtz_mtz,

  phenix.get_cc_mtz_pdb, and phenix.fmodel
- Consolidated validation tool in GUI
- New map calculation tool, phenix.maps (also used in GUI)
- Rapid loading of structures in GUI selection editor
- Improved geometry restraints to maintain amino acid rotameric states
- Alpha version of secondary structure restraints
- Automated secondary structure analysis with KSDSSP (code from UCSF CGL)

For a full list of changes see:

http://www.phenix-online.org/documentation/CHANGES

Please note that there is a new publication that should be used to 
cite use of Phenix:


PHENIX: a comprehensive Python-based system for macromolecular 
structure solution. P. D. Adams, P. V. Afonine, G. Bunkóczi, V. B. 
Chen, I. W. Davis, N. Echols, J. J. Headd, L.-W. Hung, G. J. Kapral, 
R. W. Grosse-Kunstleve, A. J. McCoy, N. W. Moriarty, R. Oeffner, R. J. 
Read, D. C. Richardson, J. S. Richardson, T. C. Terwilliger and P. H. 
Zwart. Acta Cryst. D66, 213-221 (2010).


Full documentation is available here:

http://www.phenix-online.org/documentation/

There is a Phenix bulletin board:

http://www.phenix-online.org/mailman/listinfo/phenixbb/

Please consult the installer README file or online documentation for
installation instructions.

Direct questions and problem reports to the bulletin board or:

h...@phenix-online.org and b...@phenix-online.org

Commercial users interested in obtaining access to Phenix should visit 
the

Phenix website for information about the Phenix Industrial Consortium.

The development of Phenix is principally funded by the National 
Institute of
General Medical Sciences (NIH) under grant P01-GM063210. We also 
acknowledge

the generous support of the members of the Phenix Industrial Consortium.



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***
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Feodor-Lynen-Str. 25
81377 Munich
Germany
Phone:  +49-89-2180-76845
Fax:+49-89-2180-76999
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***


Re: [ccp4bb] self rotation education

2010-03-19 Thread Dirk Kostrewa

Dear Francis Reyes,

from the self-rotation function at kappa=120 degrees, you can see that 
one threefold NCS axis is perpendicular to a crystallographic twofold 
axis. I haven't worked this out for your particular case, but the 
combination of a threefold (n-fold) NCS axis perpendicular to a 
crystallographic twofold axis creates three (n) NCS twofold axes (that 
can be viewed from both directions and in case of an uneven NCS axis 
appear twice). I've appended a schematic stereographic projection to 
make this a bit clearer (full dyad symbol crystallographic, open dyad 
and triangle symbols NCS, green circles positions above plane, red 
circles positions below plane created by crystallographic dyad, dashed 
lines help to visualize the NCS threefold, thick solid line 
crystallographic twofold, thin solid lines NCS twofolds).


Good luck,

Dirk.

Am 18.03.10 16:03, schrieb Francis E Reyes:

Hi all

I have a solved structure that crystallizes as a trimer to a reasonable 
R/Rfree, but I'm trying to rationalize the peaks in my self rotation. The space 
group is P212121, calculating my self rotations from 50-3A, integration radius 
of 22 (the radius of my molecule is about 44). I can see the three fold NCS 
from my structure on the 120 slice, but I'm trying to rationalize apparent two 
folds in my kappa=180. A picture of both slices is enclosed. The non 
crystallographic peaks for kappa=180, P222 begin to appear at kappa=150 and are 
strongest on the 180 slice.

My molecule looks close to a bagel (44A wide and 28A tall). The three fold NCS 
is down the axis of looking down on the bagel hole. I'm trying to find the two 
fold. I imagine it could be slicing the bagel in half (like to eat it for 
yourself) or slicing it vertically (like to share amongst kids) but I'm not 
exactly sure what's the best way to visualize this. Is there something easier 
than correlation maps with getax (since I have the rotation (polarrfn) and 
translation?). If you have an eye for spotting symmetry, Ill send the pdb in 
confidence.
  Thanks!

FR


   




-
Francis Reyes M.Sc.
215 UCB
University of Colorado at Boulder

gpg --keyserver pgp.mit.edu --recv-keys 67BA8D5D

8AE2 F2F4 90F7 9640 28BC  686F 78FD 6669 67BA 8D5D



   


--

***
Dirk Kostrewa
Gene Center, A 5.07
Ludwig-Maximilians-University
Feodor-Lynen-Str. 25
81377 Munich
Germany
Phone:  +49-89-2180-76845
Fax:+49-89-2180-76999
E-mail: kostr...@genzentrum.lmu.de
WWW:www.genzentrum.lmu.de
***



Combination-Crystallographic-NCS.pdf
Description: Adobe PDF document


Re: [ccp4bb] self rotation education

2010-03-19 Thread Dirk Kostrewa
... and here a slightly clearer version where I numbered the NCS-related 
positions 1,2,3 and their crystallographic equivalent positions 
1',2',3', which makes the NCS dyads a bit easier to understand ...


Sorry for sending two pictures.

Best regards,

Dirk.

Am 19.03.10 10:31, schrieb Dirk Kostrewa:

Dear Francis Reyes,

from the self-rotation function at kappa=120 degrees, you can see that 
one threefold NCS axis is perpendicular to a crystallographic twofold 
axis. I haven't worked this out for your particular case, but the 
combination of a threefold (n-fold) NCS axis perpendicular to a 
crystallographic twofold axis creates three (n) NCS twofold axes (that 
can be viewed from both directions and in case of an uneven NCS axis 
appear twice). I've appended a schematic stereographic projection to 
make this a bit clearer (full dyad symbol crystallographic, open dyad 
and triangle symbols NCS, green circles positions above plane, red 
circles positions below plane created by crystallographic dyad, dashed 
lines help to visualize the NCS threefold, thick solid line 
crystallographic twofold, thin solid lines NCS twofolds).


Good luck,

Dirk.

Am 18.03.10 16:03, schrieb Francis E Reyes:

Hi all

I have a solved structure that crystallizes as a trimer to a reasonable 
R/Rfree, but I'm trying to rationalize the peaks in my self rotation. The space 
group is P212121, calculating my self rotations from 50-3A, integration radius 
of 22 (the radius of my molecule is about 44). I can see the three fold NCS 
from my structure on the 120 slice, but I'm trying to rationalize apparent two 
folds in my kappa=180. A picture of both slices is enclosed. The non 
crystallographic peaks for kappa=180, P222 begin to appear at kappa=150 and are 
strongest on the 180 slice.

My molecule looks close to a bagel (44A wide and 28A tall). The three fold NCS 
is down the axis of looking down on the bagel hole. I'm trying to find the two 
fold. I imagine it could be slicing the bagel in half (like to eat it for 
yourself) or slicing it vertically (like to share amongst kids) but I'm not 
exactly sure what's the best way to visualize this. Is there something easier 
than correlation maps with getax (since I have the rotation (polarrfn) and 
translation?). If you have an eye for spotting symmetry, Ill send the pdb in 
confidence.
  Thanks!

FR


   




-
Francis Reyes M.Sc.
215 UCB
University of Colorado at Boulder

gpg --keyserver pgp.mit.edu --recv-keys 67BA8D5D

8AE2 F2F4 90F7 9640 28BC  686F 78FD 6669 67BA 8D5D



   


--

***
Dirk Kostrewa
Gene Center, A 5.07
Ludwig-Maximilians-University
Feodor-Lynen-Str. 25
81377 Munich
Germany
Phone:  +49-89-2180-76845
Fax:+49-89-2180-76999
E-mail: kostr...@genzentrum.lmu.de
WWW:www.genzentrum.lmu.de
***
   


--

***
Dirk Kostrewa
Gene Center, A 5.07
Ludwig-Maximilians-University
Feodor-Lynen-Str. 25
81377 Munich
Germany
Phone:  +49-89-2180-76845
Fax:+49-89-2180-76999
E-mail: kostr...@genzentrum.lmu.de
WWW:www.genzentrum.lmu.de
***



Combination-Crystallographic-NCS.pdf
Description: Adobe PDF document


Re: [ccp4bb] about comparing Rwork and Rfree factors of different refinement trials

2010-02-26 Thread Dirk Kostrewa
Could this be a long-standing bug in the ccp4i Refmac GUI? Some time 
ago, I sent a bug report to the ccp4 developers: if you did TLS 
refinement, you got an additional tab where you should set the B-factor 
to a uniform value. In the next round of refinement, where you read in 
the refined TLS parameters from the previous run, this tab vanished, but 
the B-factor was nevertheless still set to the same uniform value, which 
resulted in high starting R-factors for the first cycle!


I haven't tested this recently, but if you display the actual Refmac 
command script from the GUI, it should be obvious whether this bug is 
still there or not.


Best regards,

Dirk.

Am 25.02.10 17:54, schrieb Jan Schoepe:

What I tried for instance was in refmac:
1.) 20 cycles TLS followed by 10 cycles restrained refinement which 
gave Rwork=24%/Rfree=33%.
Afterwards I did 0-1 cycles restrained refinement with output from 
prev. run (pdb file, mtz file, tls file) as input for that. Result: 
33%/44%.
2.) I omitted the restrained refinement, else same as above. Result 
was 26%/32% after TLS and 31%/38% after restrained refinement...




--- gbirr...@bidmc.harvard.edu /gbirr...@bidmc.harvard.edu/ schrieb 
am *Do, 25.2.2010:

*

*
Von: gbirr...@bidmc.harvard.edu gbirr...@bidmc.harvard.edu
Betreff: RE: [ccp4bb] about comparing Rwork and Rfree factors of
different refinement trials
An: j.scho...@yahoo.de
Datum: Donnerstag, 25. Februar, 2010 17:12 Uhr

*
* *
*You can fix the TLS parameters as well. *
*Zero cycles of Refmac and fixed TLS*
*Will this work in your case?*
* *
* *
* *

*Gabriel Birrane**
Beth Israel Deaconess Medical Center
RN348
99 Brookline Ave
Boston, MA 02215 *

* *
*
*

**From:* Jan Schoepe [mailto:j.scho...@yahoo.de]
*Sent:* Thursday, February 25, 2010 11:06 AM
*To:* Birrane,Gabriel (Bidmc-Research Fellow)
*Subject:* RE: [ccp4bb] about comparing Rwork and Rfree factors of
different refinement trials

*
In principle yes, but I doubt that this works properly, especially
after TLS refinement.

--- gbirr...@bidmc.harvard.edu /gbirr...@bidmc.harvard.edu/
schrieb am *Do, 25.2.2010:
*

*
Von: gbirr...@bidmc.harvard.edu gbirr...@bidmc.harvard.edu
Betreff: RE: [ccp4bb] about comparing Rwork and Rfree factors
of different refinement trials
An: j.scho...@yahoo.de
Datum: Donnerstag, 25. Februar, 2010 16:04 Uhr

*
*


You can do zero cycles of refinement in Refmac. This will just
give you the statistics as Refmac calculates them without
any refinement. Is this what you are looking for?



From: CCP4 bulletin board [ccp...@jiscmail.ac.uk] On Behalf Of
Jan Schoepe [j.scho...@yahoo.de]
Sent: Thursday, February 25, 2010 9:38 AM
To: CCP4BB@JISCMAIL.AC.UK
Subject: [ccp4bb] about comparing Rwork and Rfree factors of
different refinement trials

Dear all,

I do have a question about comparing Rfree and Rwork factors
of different refinement trials whereas I always started with
the same pdb file and structure factors (phasing by MR).
Means I had a protein structure which was (not just by me)
refined several times in different ways also with different
programs and also accordingly got different R factors for each
finally refined structure.
Could anyone suggest if there is something like a standard
run which makes all these R factors (or derivatives since
this run should change the R factors) better comparable?
(E.g. it did not work for me to do a 1 cycle rigid body
refinement in refmac hoping that the R factors are measured
well and the structure does not change much. In fact, the R
factors increased dramatically, lets say Rfree from 30% to 40%.)

Many thanks for your suggestions!
Jan


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*

*
__
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Schutz gegen Massenmails.
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__
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--

***
Dirk Kostrewa
Gene Center, A 5.07
Ludwig-Maximilians-University
Feodor-Lynen-Str. 25
81377 Munich
Germany
Phone:  +49-89-2180-76845
Fax:+49-89-2180-76999
E-mail

[ccp4bb] Research Scientist / Postdoc Position at the Gene Center, University of Munich

2010-02-25 Thread Dirk Kostrewa

Dear CCP4ers,

on behalf of Patrick Cramer, I would like to draw your attention to the 
following open position at the Gene Center, University of Munich. 
Please, do not reply directly to me, but to the e-mail addresses given 
at the end of this job offer.


Best regards,

Dirk Kostrewa.

---

Applications are invited for a

RESEARCH SCIENTIST / POSTDOC (Multiprotein complex structure)

in the lab of Patrick Cramer at the Gene Center Munich.

Project: Crystal structure analysis of RNA polymerase I, the 14-subunit 
600 kDa central enzyme that makes rRNA. Initial crystals are available.


We study the mechanisms of transcription by an interdisciplinary 
structural, biochemical and genetic analysis of multi-component 
complexes. For details please visit:


http://www.LMB.uni-muenchen.de/cramer/index.html

We look for a collaborative person with a background in biochemistry and 
X-ray crystallography, documented by at least one significant 
first-author publication. We offer a stimulating environment on a 
leading European life science campus, and a longer-term perspective. 
There are possibilities to join ongoing projects of high scientific 
significance, to participate in networks of excellence at the national 
and international level, and to contribute to teaching.


Applications including a one-page CV, list of publications, and email 
addresses of 2-3 referees should be sent to R. Menacher 
(menac...@lmb.uni-muenchen.de). Informal enquiries may be sent to P. 
Cramer (cra...@lmb.uni-muenchen.de).


Deadline for applications is March 15, 2010.


Re: [ccp4bb] about comparing Rwork and Rfree factors of different refinement trials

2010-02-25 Thread Dirk Kostrewa

Dear Jan,

an initial increase in Rfree usually means, that either, in case of 
isomorphous crystal forms, the structure was refined before against a 
different test set, or, in case of completely different crystal forms, 
that you have a new test set. In both cases, Rwork and Rfree for the 
initial model start at very similar values and de-couple during 
refinement, resulting in decreasing Rwork and increasing Rfree values.
If you have similar resolution ranges, you should define your own 
standard refinement protocol; for instance, rigid body - TLS - xyzB, 
such that the rmsd in bond lengths converge at similar values, and then 
compare the R-values afterwards.
This can be done with all modern refinement programs, such as REFMAC, 
PHENIX, BUSTER and CNS.


Good luck,

Dirk.

Am 25.02.10 15:38, schrieb Jan Schoepe:

Dear all,

I do have a question about comparing Rfree and Rwork factors of 
different refinement trials whereas I always started with the same pdb 
file and structure factors (phasing by MR).
Means I had a protein structure which was (not just by me) refined 
several times in different ways also with different programs and also 
accordingly got different R factors for each finally refined structure.
Could anyone suggest if there is something like a standard run which 
makes all these R factors (or derivatives since this run should 
change the R factors) better comparable?
(E.g. it did not work for me to do a 1 cycle rigid body refinement in 
refmac hoping that the R factors are measured well and the structure 
does not change much. In fact, the R factors increased dramatically, 
lets say Rfree from 30% to 40%.)


Many thanks for your suggestions!
Jan


__
Do You Yahoo!?
Sie sind Spam leid? Yahoo! Mail verfügt über einen herausragenden 
Schutz gegen Massenmails.
http://mail.yahoo.com 


--

***
Dirk Kostrewa
Gene Center, A 5.07
Ludwig-Maximilians-University
Feodor-Lynen-Str. 25
81377 Munich
Germany
Phone:  +49-89-2180-76845
Fax:+49-89-2180-76999
E-mail: kostr...@genzentrum.lmu.de
WWW:www.genzentrum.lmu.de
***



Re: [ccp4bb] anomalous difference fourier maps

2010-02-19 Thread Dirk Kostrewa

Dear Gerard,

I can only agree with you - I've also noticed a growing and sometimes 
irritating cross-advertisement of non-CCP4 programs on the CCP4BB over 
the last months (mainly Phenix). Unless, the specific task that was 
asked for, can only be (reasonably) solved with non-CCP4 programs, such 
replies leave a somewhat bad aftertaste.
Personally, I think, it would be perfectly acceptable if both solutions 
with CCP4 programs and other programs would be given, so that the user 
may choose, or try them all.


Best wishes,

Dirk.

Am 19.02.10 15:04, schrieb Gerard Bricogne:

Dear all,

  This is a remark I have wanted to make for a long time but managed so
far to repress. However, this case is absolutely clear: Ivan was not asking
for general advice on how to carry out a general task, but how to perform a
specific task with the CCP4 software.

  In response we get (surprise, surprise, ...) another instance of the
relentless touting for Phenix on the CCP4BB, which has long been an
expected (or tolerated?) feature of this BB. Contributions from Phenix
developers are of course much appreciated when questions are about general
crystallographic matters where their expertise and experience is valuable;
but when people ask specifically how to do something with CCP4 programs,
could they please not be grabbed by the sleeve and enticed to buy their
sweets from the shop next door?

  In this case, for instance, Ivan thanks guys (plural) for the answers
he got (All of your suggestions were great). Perhaps one of those was a
CCP4-based answer, but if so it has not even been communicated to the rest
of the CCP4BB subscribers - so not only is this touting in bad taste after a
while: it even interferes with the sharing of expertise in using the CCP4
software, which after all must be one of the main missions of this BB.

  I have long wondered whether anyone on the CCP4 side been assigned the
task of answering every question to the Phenix BB by describing how to do it
with CCP4 programs ... .


  With best wishes,

   Gerard.

--
On Thu, Feb 18, 2010 at 03:53:02PM -0800, Pavel Afonine wrote:
   

Hi Ivan,

two ways (at least) to do it in PHENIX:

- phenix.refine always computes anomalous difference Fourier map (provided
that your input data file contains Fobs(+) and Fobs(-)). The command below
will do it:

phenix.refine model.pdb data.mtz strategy=none
main.number_of_macro_cycles=0 output.prefix=maps_only

- you can use phenix.maps that is a general tool to compute a broad variety
of maps. Type phenix.maps from the command line for usage instructions.
You need to have the latest development (or one of) PHENIX nightly build
for this.

All this is available from the GUI too.

Pavel.


On 2/18/10 3:34 PM, xaravich ivan wrote:
 

Hello,


I wanted to make an anomalous difference fourier map of a structure with
zinc bound to it. However I have not been successful in making the map and
I would really appreciate your help if anyone could suggest me where I am
going wrong.

I solved this zinc bound structure, by molecular replacement from a
calcium bound structure (1.4 angstrom) that I solved. I want to show that
the zinc binds to the identical site by the anomalous difference fourier
map.

I am using CCP4i and the steps that I have been taking are, (names of the
files are arbitrary)

1) generating structure factors and phases from the solved coordinates by
SFALL

   Input files
   zinc bound pdb
   original zinc .mtz data from synchrotron

  output file
sfall.mtz

2)merging the sfall.mtz containing the PHICalc and FCalc columns with
the original synchrotron .mtz file containing DANO and SIGDANO by running
CAD.

  input files
sfall.mtz and zinc synchrtron .mtz

output file
CAD.mtz

3) Running FFT to make anomalous map, selecting labels from CAD.mtz as
input files.

There is an output map file but nothing in it. all the values are 0 and
the map is not recognized by coot. There is no error message in the log
file.


I must be missing something or doing something wrong/stupid.


Thanks,

Ivan

   
   


--

***
Dirk Kostrewa
Gene Center, A 5.07
Ludwig-Maximilians-University
Feodor-Lynen-Str. 25
81377 Munich
Germany
Phone:  +49-89-2180-76845
Fax:+49-89-2180-76999
E-mail: kostr...@genzentrum.lmu.de
WWW:www.genzentrum.lmu.de
***


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