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. 2000 Jul 25;97(16):8868–8873. doi: 10.1073/pnas.160259697

Figure 2.

Figure 2

Free energy of binding for specific ensembles of arc repressor. The FR) curves are shown for the folded (red) and unfolded (green) minima as well as the fully ordered [(Q = 1 (black)] and disordered [Q = 0 (blue)] states at Tf. ΔR = RR0 is the separation distance relative to that of the bound complex (R0). The effective capture radius is expanded by 8 Å for the unfolded state over the folded (which is 16 Å) and by 14 Å over that for the completely folded Q = 1 state. The orange curve is the free energy of the steepest descent path on the FR, Qp) surface shown in Fig. 3. Note the broken scales of R used to delineate the folding events, which occur in a narrow range of approach distance. The radius of the square well potential is b = R0 + 6.5 Å. The Debye–Waller factor for the folded residues is Δf = 1 Å, and for the unfolded chain Δu = 17 Å, which is the end-to-end distance of a random coil with 20 bond segments (the number of residues in the binding site).