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. 2011 Mar 15;286(19):17047–17059. doi: 10.1074/jbc.M110.212571

TABLE 2.

Parameters derived from SAXS experiments

Sample Concentrationa Q rangeb Rgc Dmaxc I(0)c χ2d
mg/ml Å Å a.u.
ASV-IN(1–286)e 2.3 0.007–0.4 33.1 ± 0.6 109.4 ± 1.3 0.033 0.8
    (wild type)
ASV-IN(1–286)e,f 2.4 0.01–0.4 36.8 ± 0.2 119.7 ± 0.8 0.034 3.4
    (E157C/F199K)
ASV-IN(1–286)e 0.7 0.01–0.4 31.5 ± 0.2 92.8 ± 1.0 0.024 1.7
    (C23S/C125S/F199K/W259A)
trxA-ASV-IN(1–286)e 2.3 0.01–0.4 39.0 ± 0.4 114.9 ± 1.1 0.030 1.1
    (C23S/C125S/F199K/W259A)
ASV-IN(49–286)e,f 1.1 0.01–0.42 26.0 ± 0.8 75.0 ± 2.2 0.022 2.2
    (F199K)
ASV-IN(1–207)e,f 3.6 0.01–0.41 20.0 ± 0.1 61.0 ± 0.4 0.011 0.8
PFV-IN(1–402)d 4.3 0.007–0.42 38.5 ± 0.2 117.9 ± 0.6 0.031 2.7
    (wild type)

a Data were determined by absorbance at 280 nm with a calculated molar extinction coefficient.

b Q = 4πsinθ/λ, where 2θ is the scattering angle; recorded data in this range were used for P(r) analysis and subsequent ab initio shape reconstructions.

c This was determined using the program IRENA. Comparable results were obtained using the program GNOM and by Guinier analysis with Auto Rg (65).

d Goodness of fit was assessed by reduced χ2 analysis.

e Data were collected at APS beamline DND-CAT 5ID-D.

f Data were also collected at local sources.