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. 2017 Jul 19;7:5798. doi: 10.1038/s41598-017-06133-y

Table 1.

Data collection and structural parameters obtained by SAXS.

TupA TupA* TupA W TupA W* TupA Mo
Data collection parameters
    Instrument P12 BM29 P12 BM29 P12
    Wavelength, Å 1.24 0.99 1.24 0.99 1.24
    s-range, Å−1 0.0027–0.45 0.003–0.49 0.0027–0.45 0.003–0.49 0.0027–0.45
    Exposure time, s 1 10 1 10 1
    Concentration range, mg/ml 1.0–8.5 0.8–6.0 1.0–6.0 0.8–12.0 1.0–6.0
    Temperature, K 280 278 280 278 280
Structural parameters
    Rg, Å [from P(r)] 25.5 ± 0.3 25.4 ± 0.3 24.1 ± 0.2 23.8 ± 0.2 24.4 ± 0.2
    Rg, Å (from Guinier) 24.2 ± 0.4 24.0 ± 0.4 23.0 ± 0.3 22.8 ± 0.3 22.9 ± 0.3
    Dmax, Å 96 ± 3 95 ± 3 90 ± 3 89 ± 3 92 ± 3
    Porod volume, Å3 × 103 51.4 ± 3.5 48.5 ± 3.3 45.7 ± 3.1 44.4 ± 3.0 45.8 ± 3.1
Mol. mass determination (kDa)
    From I(0) 29 ± 2 32 ± 2 26 ± 2 29 ± 2 26 ± 2
    From Porod volume 31 ± 2 29 ± 2 28 ± 2 27 ± 2 28 ± 2
Model vs. data discrepancy (χ2)
    Holo-form model 4.0 2.4 0.9 2.2 0.9
    MX 7.8 5.8 1.8 11.6 1.8
    Apo-form model 1.0 0.7 2.0 11.9 1.7

Molecular mass (M) was estimated from forward scattering I(0) and Porod volume respectively, the theoretical molecular mass predicted from sequence is 29.7 kDa. Radius of gyration, R g (Å) was calculated using the Guinier approximation and also the distance distribution function (P(r) using GNOM), which also estimates maximum particle dimension (D max). χ2 values correspond to discrepancies between models and experimental data, the lowest χ2 value per dataset is highlighted. MX: crystal structure.

*Data collected at BM29 beamline, ESRF, Grenoble, France. The rest of the datasets were collected at EMBL P12 beamline, DESY, Hamburg, Germany.