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CCP4BB  August 2007

CCP4BB August 2007

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Subject:

Strange diffraction images

From:

Jacob Keller <[log in to unmask]>

Reply-To:

Jacob Keller <[log in to unmask]>

Date:

Mon, 27 Aug 2007 10:44:23 -0500

Content-Type:

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What a beautiful and interesting diffraction pattern!



To me, it seems that there is a blurred set of spots with different cell dimensions, although

nearly the same, underlying the ordered diffraction pattern. A possible interpretation occurred to

me, that the ordered part of the crystal is supported by a less-ordered lattice of slightly

different dimensions, which, because the crystal is a like a layer-cake of 2-d crystals, need not

be commensurable in the short range with the ordered lattice. The nicely-ordered "cake" part of the 

crystal you solved, but the "frosting" between is of a different, less ordered nature, giving rise

to the diffuse pattern which has slightly different lattice spacing. I would have to see more

images to know whether this apparent lattice-spacing phenomenon is consistent, but it at least

seems that way to me from the images you put on the web. I would shudder to think of indexing it,

however.



All the best,



Jacob Keller



ps I wonder whether a crystal was ever solved which had two interpenetrating, non-commensurable

lattices in it. That would be pretty fantastic.



==============Original message text===============

On Mon, 27 Aug 2007 5:57:45 am CDT "Mark J. van Raaij" wrote:



In general, I think we should be careful about too strong statements,  

while in general structures with high solvent diffract to low-res,  

there are a few examples where they diffract to high res. Obviously,  

high solvent content means fewer crystal contacts, but if these few  

are very stable?

Similarly, there are probably a few structures with a high percentage  

of Ramachandran outliers which are real and similarly for all other  

structural quality indicators. However, combinations of various of  

these probably do not exist and in any case, every unusual feature  

like this should be described and an attempt made to explain/analyse  

it, which in the case of the Nature paper that started this thread  

was apparently not done, apart from the rebuttal later (and perhaps  

in unpublished replies to the referees?).



With regards to our structures 1H6W (1.9A) and 1OCY (1.5A), rather  

than faith, I think the structure is held together by a real  

mechanism, which however I can't explain. Like in the structure Axel  

Brunger mentioned, there is appreciable diffuse scatter, which imo  

deserves to be analysed by someone expert in the matter (to whom, or  

anyone else, I would gladly supply the images which I should still  

have on a tape or CD in the cupboard...). For low-res version of one  

image see

http://web.usc.es/~vanraaij/diff45kd.pngand

http://web.usc.es/~vanraaij/diff45kdzoom.pngtwo possibilities I have been thinking about:

1. only a few of the "tails" are ordered, rather like a stack of  

identical tables in which four legs hold the table surfaces stably  

together, but the few ordered tails/legs do not contribute much to  

the diffraction. This raises the question why some tails should be  

"stiff" and others not; perhaps traces of a metal or other small  

molecule stabilise some tails (although crystal optimisation trials  

did not show up such a molecule)?

2. three-fold disorder, either individually or in microdomains too  

small to have been resolved by the beam used. For this I have been  

told to expect better density than observed, but maybe this is not true.

we did try integrating in lower space groups P3, P2 instead of P321  

with no improvement of the density, we tried a RT dataset to see if  

freezing caused the disorder and we tried improving the phases by MAD  

on the mercury derivative, but with no improvement in the density for  

the tail.



Mark J. van Raaij

Unidad de Bioquímica Estructural

Dpto de Bioquímica, Facultad de Farmacia

and

Unidad de Rayos X, Edificio CACTUS

Universidad de Santiago

15782 Santiago de Compostela

Spain

http://web.usc.es/~vanraaij/



On 24 Aug 2007, at 03:01, Petr Leiman wrote:



> ----- Original Message ----- From: "Jenny Martin"  

> <[log in to unmask]>

> To: <[log in to unmask]>

> Sent: Thursday, August 23, 2007 5:46 PM

> Subject: Re: [ccp4bb] The importance of USING our validation tools

>

>> My question is, how could crystals with 80% or more solvent  

>> diffract  so well? The best of the three is 1.9A resolution with I/ 

>> sigI 48 (top  shell 2.5). My experience is that such crystals  

>> diffract very weakly.

>

> You must be thinking about Mark van Raaij's T4 short tail fibre  

> structures. Yes, the disorder in those crystals is extreme. There  

> are ~100-150 A thick disordered layers between the ~200 A thick  

> layers of ordered structure. The diffraction pattern does not show  

> any anomalies (as far as I can remember from 6 years ago). The  

> spots are round, there are virtually no spots not covered by  

> predictions, and the crystals diffract to 1.5A resolution. The  

> disordered layers are perpendicular to the threefold axis of the  

> crystal. The molecule is a trimer and sits on the threefold axis.  

> It appears that the ordered layers somehow know how to position  

> themselves across the disordered layers.  I agree here with Michael  

> Rossmann that in these crystals the ordered layers are held  

> together by faith.

> Mark integrated the dataset in lower space groups, but the  

> disordered stuff was not visible anyway. He will probably add more  

> to the discussion.

>

> Petr

>

>

>>

>> Any thoughts?

>>

>> Cheers,

>> Jenny



===========End of original message text===========







***********************************

Jacob Keller

Northwestern University

6541 N. Francisco #3

Chicago IL 60645

(847)467-4049

[log in to unmask]

***********************************





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