[ccp4bb] Lousy diffraction at home but fantastic at the synchrotron?

2010-10-18 Thread Marcus Winter






Dear Klaus,





With extensive travel in the meantime, we're sorry that it took us so long to 
get

back to you on this.



Well, the true answer is that any resolution might be expected on the PX 
Scanner.

Thus, sometimes we have observed higher resolutions on the PX Scanner than

observed from the 'same' protein crystals using a third generation synchrotron 
source.

The point is that as well as determining the 'native' diffraction qualities 
(resolution limit,

mosaicity and unit cell, etc.) of the chosen crystal, using the PX Scanner one 
can also

establish the efficacy of the cryo-protection and the further 'handling' stages 
of the

crystal workflow, etc.  (So, in the cases above, perhaps the cryo-conditions 
were

'wrong', etc...).



Moreover, using the PX Scanner, one can unambiguously identify the 
best-diffracting

individual crystal in any droplet across the whole crystallisation plate: most 
importantly

in situ without any kind of 'disturbance'...  And even if the crystals do indeed

diffract - on the PX Scanner, to lower resolution than they do on a more 
powerful

source, of course you can still rank them and then pick up the clearly 'best' 
ones for further

analysis.  As experienced by many researchers: there can be very significant 
differences

between crystals, even grown in the same drop.



You, all, are most welcome to visit our labs, bringing your plates, in order to 
collect

in situ crystal diffraction data: as an evaluation both of your crystals and the

PX Scanner instrument.  We look forward to this !





Yours,



Tadeusz Skarzynski

Marcus Winter



(Oxford Diffraction Ltd. - now Agilent Technologies)







-Original Message-
From: Klaus Fütterer [mailto:k.futte...@bham.ac.uk]
Sent: 30 September 2010 11:00
To: WINTER,MARCUS (A-Varian,ex1)
Cc: CCP4BB@JISCMAIL.AC.UK
Subject: Re: [ccp4bb] Lousy diffraction at home but fantastic at the 
synchrotron?



Marcus,



May I ask the following: assuming 8 A is obtained from a single

crystal on the home source, what diffraction limit would one expect

on the PX scanner?



Best regards,



Klaus





===



 Klaus Fütterer, Ph.D.

 Reader in Structural Biology

   Undergraduate Admissions



School of Biosciences   P: +44-(0)-121-414 5895

University of Birmingham   F: +44-(0)-121-414 5925

Edgbaston E: k.futte...@bham.ac.uk

Birmingham, B15 2TT, UK   W: www.biochemistry.bham.ac.uk/klaus/

===











On 30 Sep 2010, at 10:44, Marcus Winter wrote:







 This recent discussion does tend towards the ideal scenario: of

 identifying ones

 best-diffracting crystals... before embarking on the synchrotron trip.



 The established Oxford Diffraction PX Scanner home laboratory

 instrument can

 therefore be most useful.  This enables the direct X-ray screening

 of individual

 (putative) single crystal objects, in situ, in the (any SBS format)

 crystallisation plate.





 Yours sincerely,



 Marcus Winter (Oxford Diffraction Ltd. - now Agilent Technologies)







 -Original Message-

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

 Of Phil Jeffrey

 Sent: 28 September 2010 19:20

 To: CCP4BB@JISCMAIL.AC.UK

 Subject: Re: [ccp4bb] Lousy diffraction at home but fantastic at

 the synchrotron?



 Often this reflect crystal size - a small crystal in a big beam (or

 one

 with a long path in air) on a home source would see the small

 diffraction signal drop below the noise level quite quickly - often at

 the low resolution intensity dip that sits very approximately around 6

 Angstrom.  On a synchrotron source with a tight low-divergence beam

 that

 matches more closely the crystal dimensions that same crystal will

 appear to do rather better.



 Also one is more likely to expose the crystal longer (in terms of

 total

 photon numbers) at a synchrotron, which itself begets better signal/

 noise.



 Alternatively: everyone tries harder before synchrotron trips



 Phil Jeffrey

 Princeton



 On 9/28/10 1:27 PM, Francis E Reyes wrote:

  Hi all

 

  I'm interested in the scenario where crystals were screened at

 home and

  gave lousy (say  8-10A) but when illuminated with synchrotron

 radiation

  gave reasonable diffraction (  3A) ? Why the discrepancy?

 

  Thanks

 

  F




Re: [ccp4bb] Lousy diffraction at home but fantastic at the synchrotron?

2010-10-12 Thread James Holton
There are a few things that synchrotron beamlines generally do better 
than home sources, but the most important are flux, collimation and 
absorption.


Flux is in photons/s and simply scales down the amount of time it takes 
to get a given amount of photons onto the crystal.  Contrary to popular 
belief, there is nothing magical about having more photons/s: it does 
not somehow make your protein molecules behave and line up in a more 
ordered way.  However, it does allow you to do the equivalent of a 
24-hour exposure in a few seconds (depending on which beamline and which 
home source you are comparing), so it can be hard to get your brain 
around the comparison.


Collimation, in a nutshell, is putting all the incident photons through 
the crystal, preferably in a straight line.  Illuminating anything that 
isn't the crystal generates background, and background buries weak 
diffraction spots (also known as high-resolution spots).  Now, when I 
say crystal I mean the thing you want to shoot, so this includes the 
best part of a bent, cracked or otherwise inhomogeneous crystal.  
The amount of background goes as the square of the beam size, so a 0.5 
mm beam can produce up to 25 times more background than a 0.1 mm beam 
(for a fixed spot intensity).


Also, if the beam has high divergence (the range of incidence angles 
onto the crystal), then the spots on the detector will be more spread 
out than if the beam had low divergence, and the more spread-out the 
spots are the easier it is for them to fade into the background.  Now, 
even at home sources, one can cut down the beam to have very low 
divergence and a very small size at the sample position, but this comes 
at the expense of flux.


Another tenant of collimation (in my book) is the DEPTH of non-crystal 
stuff in the primary x-ray beam that can be seen by the detector.  
This includes the air space between the collimator and the beam stop.  
One millimeter of air generates about as much background as 1 micron of 
crystal, water, or plastic.  Some home sources have ridiculously large 
air paths (like putting the backstop on the detector surface), and that 
can give you a lot of background.  As a rule of thumb, you want you air 
path in mm to be less than or equal to your crystal size in microns.  In 
this situation, the crystal itself is generating at least as much 
background as the air, and so further reducing the air path has 
diminishing returns.  For example, going from 100 mm air and 100 um 
crystal to completely eliminating air will only get you about a 40% 
reduction in background noise (it goes as the square root).


Now, this rule of thumb also goes for the support material around your 
crystal: one micron of cryoprotectant generates about as much background 
as one micron of crystal.  So, if you have a 10 micron crystal mounted 
in a 1 mm thick drop, and manage to hit the crystal with a 10 micron 
beam, you still have 100 times more background coming from the drop than 
you do from the crystal.  This is why in-situ diffraction is so 
difficult: it is hard to come by a crystal tray that is the same 
thickness as the crystals.


Absorption differences between home and beamline are generally because 
beamlines operate at around 1 A, where a 200 um thick crystal or a 200 
mm air path absorbs only about 4% of the x-rays, and home sources 
generally operate at CuKa, where the same amount of crystal or air 
absorbs ~20%.  The absorption correction due to different paths taken 
through the sample must always be less than the total absorption, so you 
can imagine the relative difficulty of trying to measure a ~3% anomalous 
difference.


Lower absorption also accentuates the benefits of putting the detector 
further away.  By the way, there IS a good reason why we spend so much 
money on large-area detectors.  Background falls off with the square of 
distance, but the spots don't (assuming good collimation!).



However, the most common cause of drastically different results at 
synchrotron vs at home is that people make the mistake of thinking that 
all their crystals are the same, and that they prepared them in the 
same way.  This is seldom the case!  Probably the largest source of 
variability is the cooling rate, which depends on the head space of 
cold N2 above the liquid nitrogen you are plunge-cooling in (Warkentin 
et al. 2006).


-James Holton
MAD Scientist

On 9/28/2010 10:27 AM, Francis E Reyes wrote:

Hi all

I'm interested in the scenario where crystals were screened at home 
and gave lousy (say  8-10A) but when illuminated with synchrotron 
radiation gave reasonable diffraction (  3A) ? Why the discrepancy?


Thanks

F

-
Francis E. 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


Re: [ccp4bb] Lousy diffraction at home but fantastic at the synchrotron?

2010-10-12 Thread Gunnar Olovsson
Thank you James for a very interesting  informative discussion on the
subject.

-  Gunnar

Gunnar Olovsson
gun...@byron.biochem.ubc.ca
University of British Columbia
Vancouver,   Canada


On Tue, Oct 12, 2010 at 9:04 AM, James Holton jmhol...@lbl.gov wrote:

 There are a few things that synchrotron beamlines generally do better than
 home sources, but the most important are flux, collimation and absorption.

 Flux is in photons/s and simply scales down the amount of time it takes to
 get a given amount of photons onto the crystal.  Contrary to popular belief,
 there is nothing magical about having more photons/s: it does not somehow
 make your protein molecules behave and line up in a more ordered way.
  However, it does allow you to do the equivalent of a 24-hour exposure in a
 few seconds (depending on which beamline and which home source you are
 comparing), so it can be hard to get your brain around the comparison.

 Collimation, in a nutshell, is putting all the incident photons through the
 crystal, preferably in a straight line.  Illuminating anything that isn't
 the crystal generates background, and background buries weak diffraction
 spots (also known as high-resolution spots).  Now, when I say crystal I
 mean the thing you want to shoot, so this includes the best part of a
 bent, cracked or otherwise inhomogeneous crystal.  The amount of
 background goes as the square of the beam size, so a 0.5 mm beam can produce
 up to 25 times more background than a 0.1 mm beam (for a fixed spot
 intensity).

 Also, if the beam has high divergence (the range of incidence angles onto
 the crystal), then the spots on the detector will be more spread out than if
 the beam had low divergence, and the more spread-out the spots are the
 easier it is for them to fade into the background.  Now, even at home
 sources, one can cut down the beam to have very low divergence and a very
 small size at the sample position, but this comes at the expense of flux.

 Another tenant of collimation (in my book) is the DEPTH of non-crystal
 stuff in the primary x-ray beam that can be seen by the detector.  This
 includes the air space between the collimator and the beam stop.  One
 millimeter of air generates about as much background as 1 micron of crystal,
 water, or plastic.  Some home sources have ridiculously large air paths
 (like putting the backstop on the detector surface), and that can give you a
 lot of background.  As a rule of thumb, you want you air path in mm to be
 less than or equal to your crystal size in microns.  In this situation, the
 crystal itself is generating at least as much background as the air, and so
 further reducing the air path has diminishing returns.  For example, going
 from 100 mm air and 100 um crystal to completely eliminating air will only
 get you about a 40% reduction in background noise (it goes as the square
 root).

 Now, this rule of thumb also goes for the support material around your
 crystal: one micron of cryoprotectant generates about as much background as
 one micron of crystal.  So, if you have a 10 micron crystal mounted in a 1
 mm thick drop, and manage to hit the crystal with a 10 micron beam, you
 still have 100 times more background coming from the drop than you do from
 the crystal.  This is why in-situ diffraction is so difficult: it is hard to
 come by a crystal tray that is the same thickness as the crystals.

 Absorption differences between home and beamline are generally because
 beamlines operate at around 1 A, where a 200 um thick crystal or a 200 mm
 air path absorbs only about 4% of the x-rays, and home sources generally
 operate at CuKa, where the same amount of crystal or air absorbs ~20%.  The
 absorption correction due to different paths taken through the sample must
 always be less than the total absorption, so you can imagine the relative
 difficulty of trying to measure a ~3% anomalous difference.

 Lower absorption also accentuates the benefits of putting the detector
 further away.  By the way, there IS a good reason why we spend so much money
 on large-area detectors.  Background falls off with the square of distance,
 but the spots don't (assuming good collimation!).


 However, the most common cause of drastically different results at
 synchrotron vs at home is that people make the mistake of thinking that all
 their crystals are the same, and that they prepared them in the same way.
  This is seldom the case!  Probably the largest source of variability is the
 cooling rate, which depends on the head space of cold N2 above the liquid
 nitrogen you are plunge-cooling in (Warkentin et al. 2006).

 -James Holton
 MAD Scientist


 On 9/28/2010 10:27 AM, Francis E Reyes wrote:

 Hi all

 I'm interested in the scenario where crystals were screened at home and
 gave lousy (say  8-10A) but when illuminated with synchrotron radiation
 gave reasonable diffraction (  3A) ? Why the discrepancy?

 Thanks

 F

 

[ccp4bb] Lousy diffraction at home but fantastic at the synchrotron?

2010-09-30 Thread Marcus Winter



This recent discussion does tend towards the ideal scenario: of identifying ones

best-diffracting crystals... before embarking on the synchrotron trip.



The established Oxford Diffraction PX Scanner home laboratory instrument can

therefore be most useful.  This enables the direct X-ray screening of individual

(putative) single crystal objects, in situ, in the (any SBS format) 
crystallisation plate.





Yours sincerely,



Marcus Winter (Oxford Diffraction Ltd. - now Agilent Technologies)







-Original Message-
From: CCP4 bulletin board [mailto:ccp...@jiscmail.ac.uk] On Behalf Of Phil 
Jeffrey
Sent: 28 September 2010 19:20
To: CCP4BB@JISCMAIL.AC.UK
Subject: Re: [ccp4bb] Lousy diffraction at home but fantastic at the 
synchrotron?



Often this reflect crystal size - a small crystal in a big beam (or one

with a long path in air) on a home source would see the small

diffraction signal drop below the noise level quite quickly - often at

the low resolution intensity dip that sits very approximately around 6

Angstrom.  On a synchrotron source with a tight low-divergence beam that

matches more closely the crystal dimensions that same crystal will

appear to do rather better.



Also one is more likely to expose the crystal longer (in terms of total

photon numbers) at a synchrotron, which itself begets better signal/noise.



Alternatively: everyone tries harder before synchrotron trips



Phil Jeffrey

Princeton



On 9/28/10 1:27 PM, Francis E Reyes wrote:

 Hi all



 I'm interested in the scenario where crystals were screened at home and

 gave lousy (say  8-10A) but when illuminated with synchrotron radiation

 gave reasonable diffraction (  3A) ? Why the discrepancy?



 Thanks



 F


Re: [ccp4bb] Lousy diffraction at home but fantastic at the synchrotron?

2010-09-30 Thread Klaus Fütterer

Marcus,

May I ask the following: assuming 8 A is obtained from a single  
crystal on the home source, what diffraction limit would one expect  
on the PX scanner?


Best regards,

Klaus


===

Klaus Fütterer, Ph.D.
Reader in Structural Biology
  Undergraduate Admissions

School of Biosciences P: +44-(0)-121-414 5895
University of Birmingham  F: +44-(0)-121-414 5925
Edgbaston E: k.futte...@bham.ac.uk
Birmingham, B15 2TT, UK   W: www.biochemistry.bham.ac.uk/klaus/
===





On 30 Sep 2010, at 10:44, Marcus Winter wrote:




This recent discussion does tend towards the ideal scenario: of  
identifying ones

best-diffracting crystals... before embarking on the synchrotron trip.

The established Oxford Diffraction PX Scanner home laboratory  
instrument can
therefore be most useful.  This enables the direct X-ray screening  
of individual
(putative) single crystal objects, in situ, in the (any SBS format)  
crystallisation plate.



Yours sincerely,

Marcus Winter (Oxford Diffraction Ltd. – now Agilent Technologies)



-Original Message-
From: CCP4 bulletin board [mailto:ccp...@jiscmail.ac.uk] On Behalf  
Of Phil Jeffrey

Sent: 28 September 2010 19:20
To: CCP4BB@JISCMAIL.AC.UK
Subject: Re: [ccp4bb] Lousy diffraction at home but fantastic at  
the synchrotron?


Often this reflect crystal size - a small crystal in a big beam (or  
one

with a long path in air) on a home source would see the small
diffraction signal drop below the noise level quite quickly - often at
the low resolution intensity dip that sits very approximately around 6
Angstrom.  On a synchrotron source with a tight low-divergence beam  
that

matches more closely the crystal dimensions that same crystal will
appear to do rather better.

Also one is more likely to expose the crystal longer (in terms of  
total
photon numbers) at a synchrotron, which itself begets better signal/ 
noise.


Alternatively: everyone tries harder before synchrotron trips

Phil Jeffrey
Princeton

On 9/28/10 1:27 PM, Francis E Reyes wrote:
 Hi all

 I'm interested in the scenario where crystals were screened at  
home and
 gave lousy (say  8-10A) but when illuminated with synchrotron  
radiation

 gave reasonable diffraction (  3A) ? Why the discrepancy?

 Thanks

 F


[ccp4bb] Lousy diffraction at home but fantastic at the synchrotron?

2010-09-28 Thread Francis E Reyes

Hi all

I'm interested in the scenario where crystals were screened at home  
and gave lousy (say  8-10A) but when illuminated with synchrotron  
radiation gave reasonable diffraction (  3A) ? Why the discrepancy?


Thanks

F

-
Francis E. 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


Re: [ccp4bb] Lousy diffraction at home but fantastic at the synchrotron?

2010-09-28 Thread Van Den Berg, Bert
I find this interesting as well, mainly because I have never seen this myself 
and I have looked at plenty of badly diffracting crystals. In my hands, 
synchrotron data at most end up being ~1.5 angstrom better in terms of 
resolution than the same crystals on our home source. I'm wondering if this 
phenomenon is real, or whether it is just a matter of people screening 
more/better crystals at the synchrotron compared to at home? Or a lousy home 
source?

Bert


On 9/28/10 1:27 PM, Francis E Reyes francis.re...@colorado.edu wrote:

Hi all

I'm interested in the scenario where crystals were screened at home
and gave lousy (say  8-10A) but when illuminated with synchrotron
radiation gave reasonable diffraction (  3A) ? Why the discrepancy?

Thanks

F

-
Francis E. 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




Re: [ccp4bb] Lousy diffraction at home but fantastic at the synchrotron?

2010-09-28 Thread Ethan Merritt
On Tuesday 28 September 2010 10:27:17 am Francis E Reyes wrote:
 Hi all
 
 I'm interested in the scenario where crystals were screened at home  
 and gave lousy (say  8-10A) but when illuminated with synchrotron  
 radiation gave reasonable diffraction (  3A) ? Why the discrepancy?

Such a happy outcome is very rare.

I normally expect the high intensity at a beamline to push the line
separating weak but visible and too weak to see towards higher
resolution usable data.  But that isn't a change in the diffracting
properties of the crystal, just a change in achievable signal-to-noise.

Two possibilities come to mind.

A) Unintentional annealing during transport/or and as a consequence of
   crystal handling after shipment.  We've certainly seen this, but
   usually the result is bad ice rings rather than better diffraction. 

B) Home screening used a relatively large beam that saw the entirely 
   of a highly imperfect crystal.  The synchrotron beam used a much
   smaller aperture that happened to illuminate only a sweet spot.
   This is one argument advanced for the use of micro-focus beams.

B') An extreme case of B.  Multiple crystals in the loop.
   Home screening caught a bad one; beamline screening caught a good one.

-- 
Ethan A Merritt
Biomolecular Structure Center,  K-428 Health Sciences Bldg
University of Washington, Seattle 98195-7742


Re: [ccp4bb] Lousy diffraction at home but fantastic at the synchrotron?

2010-09-28 Thread Phil Jeffrey
Often this reflect crystal size - a small crystal in a big beam (or one 
with a long path in air) on a home source would see the small 
diffraction signal drop below the noise level quite quickly - often at 
the low resolution intensity dip that sits very approximately around 6 
Angstrom.  On a synchrotron source with a tight low-divergence beam that 
matches more closely the crystal dimensions that same crystal will 
appear to do rather better.


Also one is more likely to expose the crystal longer (in terms of total 
photon numbers) at a synchrotron, which itself begets better signal/noise.


Alternatively: everyone tries harder before synchrotron trips

Phil Jeffrey
Princeton

On 9/28/10 1:27 PM, Francis E Reyes wrote:

Hi all

I'm interested in the scenario where crystals were screened at home and
gave lousy (say  8-10A) but when illuminated with synchrotron radiation
gave reasonable diffraction (  3A) ? Why the discrepancy?

Thanks

F