Perhaps worth pointing out that that Wilson B is the based on the assumption of randomly distributed atoms. This is not at all how proteins are, and in particular secondary structures give a preponderance of spacings in the 4 angstrom-ish region and a peak of mean intensity in these shells. For this reason the apparent fall-off in the Wilson in this resolution range is steeper as you are falling down off of the peak due to this seondary structure giving favoured spacings that produce a deviation from randomness in this resolution range. So it will be dependent on the secondary structure of the an individual protein . So the Wilson gets about right when you deal with spacings that tend to be unbiased by secondary structure - which unfortunately is the bit that is missing in the low resolution crystal data. Wilson fall off in low resolution looks steep because the random assumption is invalid.
Maybe you can guess the secondary content of your protein from where the bump is in the Wilson plot - beta gives a bulge in the 4 ang region - alpha in the 5 to 9 ang region.
all the best
Martyn
Martyn Symmons
Cambridge
----- Original Message ----
From: Pavel Afonine
we've solved a large structure (~20,000 residues/asymm unit), with 4-fold ncs and diffraction data to 3.3A.
The Rfree/Rfac is ~28%-24% with OK geometry with no major outliers in the Ramachandran plot. I would think I'm done (.. after 6 years!). However, my refined model b-factor (~130A2) is >> Wilson b-factor (~80A2). Obviously I'm not too happy with it.
Here is what I tried to resolve this discrepancy: --> play with wxu_scale --> play with B-factor weight in ncs restraint (4-fold ncs) --> play with number of macrocycles --> Redefine tls groups
So far nothing really works, except switching from individual_adp to group_adp. However, this increases my Rfree by almost 3%.
Any ideas?
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