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Acta Crystallographica Section D: Structural Biology logoLink to Acta Crystallographica Section D: Structural Biology
. 2023 Jun 20;79(Pt 7):666–667. doi: 10.1107/S2059798323004825

Bulk-solvent and overall scaling revisited: faster calculations, improved results. Corrigendum.

P V Afonine a,*, R W Grosse-Kunstleve a, P D Adams a,b, A Urzhumtsev c,d
Editor: R J Reade
PMCID: PMC10306067  PMID: 37338421

The article by Afonine et al. [ Acta Cryst. (2013). D69, 625–634] is corrected.

Keywords: Phenix, anisotropy, bulk solvent, scaling

Abstract

Equations in Sections 2.3 and 2.4 of the article by Afonine et al. [Acta Cryst. (2013). D69, 625–634] are corrected.


In the article by Afonine et al. (2013) some improper notations and errors in several equations in Sections 2.3 and 2.4 have been corrected. We note that the Computational Crystallography Toolbox (Grosse-Kunstleve et al., 2002) has been using the correct version of these equations since 2013. Updated versions of Section 2.3 and equations (42), (43) and (45) are given below.

2.3. Bulk-solvent parameters and overall isotropic scaling

Assuming the resolution-dependent scale factors k mask(s) and k isotropic(s) to be constants k mask and k isotropic in each thin resolution shell, the determination of their values is reduced to minimizing the residual

2.3.

where the sum is calculated over all reflections s in the given resolution shell, and k overall and k anisotropic(s) are calculated previously and fixed. This minimization problem is generally highly over-determined because the number of reflections per shell is usually much larger than two.

Introducing w s = |F mask(s)|2, Inline graphic + Inline graphic , u s = |F calc(s)|2, Inline graphic and Inline graphic and substituting them into (22) leads to the minimization of

2.3.

with respect to K and k mask. This leads to a system of two equations:

2.3.

Developing these equations with respect to k mask,

2.3.

and introducing new notations for the coefficients, we obtain

2.3.

Multiplying the second equation by Y 2 and substituting KY 2 from the first equation into the new second equation, we obtain a cubic equation with fixed coefficients

2.3.

The senior coefficient in equation (27) satisfies the Cauchy–Schwarz inequality:

2.3.

Therefore, equation (27) can be rewritten as

2.3.

and solved using a standard procedure.

The corresponding values of K are obtained by substituting the roots of equation (29) into the first equation in equation (26),

2.3.

If no positive root exists, k mask is assigned a zero value, which implies the absence of a bulk-solvent contribution. If several roots with k mask ≥ 0 exist then the one that gives the smallest value of LS(K, k mask) is selected.

If desired, one can fit the right-hand side of expression (10) to the array of k mask values by minimizing the residual

2.3.

for all k mask > 0. This can be achieved analytically as described in Appendix A. Similarly, one can fit k overall exp(−B overalls 2/4) to the array of K values.

Equations (42), (43) and (45) in Section 2.4 of Afonine et al. (2013) are also updated as follows

2.3.
2.3.
2.3.

References

  1. Afonine, P. V., Grosse-Kunstleve, R. W., Adams, P. D. & Urzhumtsev, A. (2013). Acta Cryst. D69, 625–634. [DOI] [PMC free article] [PubMed]
  2. Grosse-Kunstleve, R. W., Sauter, N. K., Moriarty, N. W. & Adams, P. D. (2002). J. Appl. Cryst. 35, 126–136.

Articles from Acta Crystallographica. Section D, Structural Biology are provided here courtesy of International Union of Crystallography

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