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. 2015 Mar 10;108(5):1275–1280. doi: 10.1016/j.bpj.2015.02.004

Figure 2.

Figure 2

(A) TIRFM measurements of the intensities of YFP-FliGWT subunits in otherwise CW-only tethered motors (in strains with fliGCW on the genome and an IPTG-inducible vector carrying eyfp-fliGWT). This particular measurement (n = 33 motors) was obtained at an IPTG concentration of 5 μM. (B) Mean YFP-FliG/FliGTotal fractions (from distributions of the sort shown in A) of YFP-FliG subunits incorporated in motors, shown as a function of inducer concentration. (C) CWbias as a function of the fraction of FliGCW in otherwise WT motors. Squares (circles) indicate experiments in which strains carried fliGWT (fliGCW) on the genome and a vector expressing fliGCW (fliGWT). No hysteresis in switch function is seen. The black curve is the model prediction for N = 26, E = 0.25, Em = 0.45, and J = 1.9.