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Edward A. Berry wrote:

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Carlos Frazao wrote:


I understand that in earlier days, when data were much-much harder to collect, crystallographers were very happy with complete (although unredundant) data set. Then, Rmerge(or Rsym) were perfectly adequated in pratical terms, as data collection expriments were designed essentially to assure that at the end of the week data were complete - it was not pratical to collect redundant data. Today, with ccd's and synchrotron radiation, we quite often try to obtain data as redundant as possible, in particular to detect anomalous signal, and Rmerge statistics are simply not applicable anymore.


I just want to clarify that Rmerge or R-sym are _not_ appropriate at low
redundancy- they are appropriate at high redundancy (where they approach
the value of Rmeas) and at low redundancy they underestimate the deviation
by a factor of up to sqrt(2)=1.41.

I apologise for not having been accurate in statement. But that was not the issue I was trying to raise, but rather that in those times, due to practical reasons, usually there were no highly redundant data in macromolecular crystallography, and therefore the available statiscs indicators didn't concern too much with the redundancy issue.

What about the physical meaning of Rmeas=Rrim ? If understood correctly the Weiss papers, it indicates the "averaged precision of individual measurements". How does this correlate with the paramter we should (I believe) use instead: the "precision of the final averaged data"? Wouldn't these two statistics increasingly differ with redundancy? Why do we keep quoting statistics of the "individual measurements" when we use instead a final averaged data set for structure determination and refinement?
Carlos

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Dr. Carlos Frazao
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