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. Author manuscript; available in PMC: 2013 Apr 13.
Published in final edited form as: J Mol Biol. 2012 Feb 1;417(5):395–405. doi: 10.1016/j.jmb.2012.01.026

Table 1. Diffraction Data Collection and Structure Refinement Statistics.

Data Collectiona
Crystal IpaB28.226 IpaB28.226 IpaB28.226 SipB30.237 SipB30.237
Native Pt Remote Pt Peak SeMet Remote SeMet Peak
Beamline APS 22-BM APS 22-BM APS 22-BM APS 22-BM APS 22-BM
Space Group P21 P21 P21 P21212 P21212
Unit Cell Dimensions
a (Å) 52.391 52.300 52.300 51.144 51.052
b (Å) 28.372 28.060 28.060 84.646 84.715
c (Å) 104.804 104.760 104.760 159.155 159.336
β(°) 95.966 95.920 95.920
Wavelength (Å) 1.0000 1.0000 1.0719 0.9724 0.9793
Resolution (Å) 50-2.1 50-2.5 50-2.5 50-2.8 50-3.0
Completeness (%) 91.7 (59.3) 95.7 (72.0) 97.2 (80.5) 98.0 (87.2) 99.2 (95.5)
Reflections (total) 61,832 68,016 71,247 209,952 86,789
Reflections (unique) 18,186 10,464 10,634 17,478 14,590
Redundancy (fold) 3.4x 6.5x 6.7x 12.0x 5.9x
<I>/<σI> 13.4 (2.0) 18.6 (2.82) 19.4 (3.6) 18.8 (2.55) 14.3 (2.05)
Rmerge (%)b 8.5 (42.5) 8.4 (35.0) 8.2 (27.8) 10.0 (67.1) 11.5 (61.1)
Refinement
RCSB Accession Code 3U0C 3TUL
Protein Molecules/AU 2 4
Rwork/Rfree (%)c 24.53/29.45 29.73/31.67
Number of Atoms
Protein 2426 3877
Solvent 88 43
Ramachandran Plot (%)
Favored 97.7 95.7
Allowed 0.6 4.0
Outliers 1.7 0.2
RMSD
Bond
Lengths (Å) 0.008 0.009
Bond
Angles (°) 1.066 1.240
B factor (Å2)
Protein 44.76 52.56
Solvent 50.60 58.10
a

Numbers in parentheses are for the highest-resolution no.

b

Rmerge = ΣhΣi|Ii(h)-<I(h)>|/ΣhΣiIi(h), where Ii(h) is the ith measurement of reflection h and <I(h)> is a weighted mean of all measurements of h.

c

R = Σh|Fobs(h)-Fcalc(h)|/Σh|Fobs|. Rcryst and Rfree were calculated from the working and test reflection sets, respectively. The test set constituted 5% of the total reflections not used in refinement.

Procedures detailing crystallization and data collection of IpaB28.226 and SipB30.237 are detailed in Supplementary Material. Briefly, crystals of both proteins were obtained by the hanging drop vapor diffusion method. Following data collection, individual reflections were indexed, integrated, and scaled using HKL2000 49. Both structures were determined by two-wavelength MAD phasing using the program AutoSol within the PHENIX suite 50. The experimental models were iteratively improved by manual building in Coot 51; 52, and refined using phenix.refine within the PHENIX suite 50.