Dear William,

In a similar circumstance, we cut out the density from one crystal, and used 
that to solve the structures of non-isomorphous crystals by molecular 
replacement.  At this point, we had an envelope (needed to cut out the 
density), initial maps, and operators to place one copy of the density in the 
other crystals, which is all you need for multi-crystal averaging.  The more 
non-isomorphous your crystals are, the more powerful this is.  What’s important 
(Kevin Cowtan explained this in a talk at the IUCr meeting in Glasgow) is that 
the size of the difference in cell dimensions should preferably be comparable 
to the resolution of the data (dmin) or larger.  Our case was a bit difficult 
because the non-isomorphism was marginal — enough to stop us from using MIR(AS) 
but barely enough to help the phasing.

There are other cases of people using similar approaches in the literature.

Best wishes,

Randy Read

-----
Randy J. Read
Department of Haematology, University of Cambridge
Cambridge Institute for Medical Research    Tel: +44 1223 336500
Wellcome Trust/MRC Building                         Fax: +44 1223 336827
Hills Road                                                            E-mail: 
[email protected]
Cambridge CB2 0XY, U.K.                               
www-structmed.cimr.cam.ac.uk

On 18 Feb 2015, at 12:51, William Chao <[email protected]> wrote:

> Dear all,
> 
> I am trying to phase a largish novel structure of 130 kDa with P21 (sometimes 
> P222) space group. So far I have collected a few 3.5ish-Å 3-wavelength MAD 
> datasets from SeMet derivatives as well as an anisomorphous 6Å Hg peak 
> dataset (with detectable anomalous signal). As my crystal is rather 
> anisotropic, CC1/2 of one direction of the Se data drops below 0.5 at 4Å. I 
> can generate a map from a MAD dataset that gives a overall shape of the 
> molecule with clear molecular boundary​ after solvent flattening, resembling 
> the shape of some EM class averages that I obtained earlier. However, the 
> density of this map is very discontinuous and is impossible to build any 
> helix in by machine or by eye. ​
> 
> As I use an insect-cell expression system and the occupancy of Se is expected 
> to be low, the programmes that I used could only find a 2 reasonable sites 
> out of 24 Se per molecule. I have about 10 Se crystals and 50 native crystals 
> (which I shall use for derivatisation) left for one last trip before the 
> synchrotron shuts down for two months. Could someone advise me on a 
> reasonable data collection strategy that could maximise my chance on this 
> upcoming trip? I am sure that many people have encountered difficult data 
> like this one and have solved their structures successfully. Would anyone be 
> able to advise me on how it'd be best to improve my phases/density given the 
> limitations of the data?
> 
> Also to mention that the best native crystal can diffract to 3A with CC1/2 of 
> the worst direction dropping to 0.5 at 3.5A.
> 
> Many thanks in advance!
> 
> William
> ---​
> 
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