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. 2018 Jan 10;3(1):292–301. doi: 10.1021/acsomega.7b01692

Figure 3.

Figure 3

(a) For either shearing or unzipping (shown here for main duplex length 30 bp), the transition barrier ΔG and ΔGtot can be defined by the free energy of the transition state (1 bond) and the minimum free energy of the unbound states, respectively, relative to the initial 10-bond state. Cut-outs on the right correspond to insets in graphs (b), depicting the derivation of these free energies graphically. (b) The transition barrier (top) remains largely constant for shearing and shows a minimum of around 30 bp for unzipping; the total free-energy change (bottom) mostly decreases with increasing main duplex length. These can be fitted to eqs 1 and 2 of Section 2.4, where allowing the main duplex to kink at a critical torque of 29 pN nm (solid lines) improves fitting of the transition barrier but degrades fitting of the total free-energy difference of unzipping, relative to a model in which the main duplex does not kink (dashed lines).