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. 2016 Nov 18;292(2):446–461. doi: 10.1074/jbc.M116.755884

TABLE 1.

Statistics on qualities of diffraction data sets and atomic models

Data set ΔlnkmGlu/GlnP-gp (apo) ΔlnkmGlu/GlnP-gp (ATP) FLmP-gp (apo) FLmP-gp (methylated) ΔlnkmGlu/GlnP-gp (Hg)
Data collection
    Space group P212121 P212121 P212121 P212121 P212121
    Cell dimension (Å) 98.0, 116.6, 375.6 97.5, 116.4, 375.1 100.6, 119.5, 383.9 88.0, 136.8, 185.9 98.2, 114.7, 375.4
    Wave length (Å) 1.0 1.0 1.0 0.89 1.0
    Resolution (Å) 29.81–3.35 34.72–3.85 50.0–4.02 50.0–3.50 49.11–3.29
    (outer shell) (3.47–3.35)a (3.987–3.85) (4.10–4.02) (3.63–3.50) (3.41–3.29)
    Rmergeb 0.101 (0.46) 0.131 (0.957) 0.106 (0.557) 0.092 (0.449) 0.150 (0.905)
    Rmeasc 0.106 (0.533) 0.136 (1.005) 0.113 (0.692) 0.102 (0.554) 0.153 (0.934)
    〈I〉/σI 17.5 (1.1) 12.0 (2.4) 9.1 (1.4) 11.5 (1.2) 13.4 (2.7)
    Completeness (%) 0.97 (87.3) 1.00 (1.00) 0.93 (0.71) 0.94 (0.84) 0.93 (0.86)
    Average redundancy 8.9 14.6 5.0 4.3 21.6
    No. of unique reflections 58,212 41,157 37,377 27,310 60,351
    No. free of reflections 2343 1951 1881 1355 1982

Model refinement
    Resolution (Å) 22.41–3.35 21.30–3.85 20.11–4.02 21.43–3.50 33.54–3.29
    No. of molecules/AU 2 2 2 1 2
    Rwork/Rfree 0.2400/0.2826 0.2556/0.2910 0.2576/0.3026 0.2855/0.3149 0.2430/0.2848
    No. of protein atoms 18,374 18,382 18,372 9117 18,374
    No. of residues (% complete) 2369 (93%) 2364 (93%) 2369 (93%) 1174 (92%) 2369 (93%)
    No. of cofactors 0 2 ATP molecules 0 0 0
    No. of solvents 0 0 0 2 0
    r.m.s. deviations
        Bond length (Å) 0.008 0.007 0.007 0.005 0.005
        Bond angle (°) 1.21 1.06 1.02 1.08 0.66
    Ramachandran plot (%)
        Favorable 95 95 95 96 97
        Additional allowed 4.7 4.2 4.6 3.2 2.6
        Disallowed 0.3 0.8 0.4 0.8 0.4
    PDB entry 5KPD 5KOY 5KPI 5KPJ 5KO2

a Values in parentheses are for the highest resolution shells.

b Rmerge is defined as Σ|Ih,i − 〈Ih〉|/ΣIh,i, where Ih,i is the intensity for ith observation of a reflection with Miller index h, and 〈Ih〉 is the mean intensity for all measured Ih and Friedel pairs.

c Rmeas, redundancy-independent merging R-factor, is defined as Σ(n/(n − 1))1/2|Ih,i − 〈Ih〉|/ΣIh,i, where n is the number of observations for reflection h.