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. 2012 Jul 18;103(2):323–330. doi: 10.1016/j.bpj.2012.05.050

Figure 3.

Figure 3

Parameters describing the buckling transition. Data from simulations that use the WLC model are shown (solid circles, 5-nm segments and open squares, 2.5-nm segments). Experimental data were taken from Brutzer et al. (20) (shown as lines; standard error of the measurements is depicted as shaded area if larger than the line width). The buckling parameters are shown as function of force at 320 mM Na+ (ad) and as a function of ionic strength at constant stretching force of 3.5 pN (e–h). (a and e) Positions of the buckling point Nb. (b and f) Abrupt DNA length jump and (c and g) torque jump at the buckling point. (d and h) Energy difference between the formation energies Eloop and Ehelix. EloopEhelix represents the energetic penalty to nucleate a plectonemic superhelix and was calculated using Eq. 4.