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. 2015 Mar 3;23(3):558–570. doi: 10.1016/j.str.2015.01.011

Table 1.

Data Collection and Refinement Statistics

P1aABDΔ22/CaMNL P1aABDΔ22/β4Fn12 P1aABDΔ22
Data Collection
Source ID14-1 (ESRF) ID23-2 (ESRF) ID14-4 (ESRF)
Wavelength (Å) 0.933 0.873 0.939
Resolution (Å) 48.93–1.8 (1.9–1.8)a 48.16–4.0 (4.47–4.0) 60.37–2.30 (2.38–2.30)
Space group P212121 P65 C2221
Unit cell (Å, °) a = 59.08, b = 65.38, c = 87.3
α = β = γ = 90
a = 96.32, b = 96.32, c = 207.8
α = 90, β = 90, γ = 120
a = 41.60, b = 159.39, c = 183.83 α = 90, β = 90, γ = 90
Molecules/a.u. 2 4 2
Unique reflections 31805 (4301) 9188 (2594) 28020 (2698)
Completeness (%) 99.2 (94.7) 99.1 (99.5) 99.7 (99.8)
Rmergeb 0.095 (0.488) 0.272 (0.793) 0.125 (0.424)
Rmeasc 0.101 (0.527) 0.300 (0.879) 0.143 (0.483)
Rpimd 0.033 (0.193) 0.123 (0.364) 0.067 (0.224)
Multiplicity 9.4 (7.2) 5.7 (5.6) 4.4 (4.2)
Mean I/sig(I) 17.5 (3.7) 7.4 (3.9) 6.9 (2.2)
CC (1/2)e 0.998 (0.877) 0.977(0.751) 0.945 (0.856)

Refinement

Rworkf/Rfreeg 0.151/0.187 0.224/0.287 0.183/0.245
Rmsd bonds (Å) 0.007 0.004 0.009
Rmsd angles (°) 0.963 0.892 1.246
Ramachandran outliers 0 0 0

see also Figure S5.

a

Values in parentheses are for the highest-resolution shell.

b

Rmerge=|IiIi|/Ii, where Ii is the intensity of the ith observation, and Ii is the mean intensity of the reflection.

c

Rmeas=hkl[N/(N1)]1/2i|Ii(hkl)I(hkl)|/hkliIi(hkl).

d

Rpim=hkl[1/(N1)]1/2i|Ii(hkl)I(hkl)|/hkliIi(hkl), where Ii(hkl) is the observed intensity, and I(hkl) is the average intensity of multiple observations of symmetry-related reflections.

e

CC(1/2) = the Pearson correlation coefficient of random half data sets.

f

Rwork=hkl||Fo||Fc||/hkl|Fo|, calculated from working data set.

g

Rfree is calculated from 5% of data randomly chosen and not included in refinement.