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. 2004 Oct 22;88(1):76–84. doi: 10.1529/biophysj.104.049239

TABLE 1.

Molecule 〈Δx〉(nm) f* (pN) ln kf(f)(s−1) ln ku(f)(s−1)
P5ab,Mg+2 19 ± 2 14.5 ± 1 41 ± 1.9 − (2.8 ± 0.1)f −39 ± 2.3 + (2.9 ± 0.2)f
P5ab, by Cocco et al. (2003) 15.1 27.5 − 2.74f −42.9 + 1.93f
P5ab, EDTA 18 ± 2 13.3 ± 1 37 ± 4.0 − (2.7 ± 0.3)f −32 ± 4.8 + (2.6 ± 0.4)f
P5ab, by us 20.0 12.9 ± 0.5 36.1 ± 1.4 − (2.7 ± 0.1)f −31.5 ± 0.7 + (2.6 ± 0.1)f
P5ab, fork dynamics 20.0 12.6 ± 0.3 16.8 ± 0.2 − (1.1 ± 0.0)f −26.7 ± 0.2 + (2.3 ± 0.0)f
P5abcΔA, Mg+2 22 ± 4 12.7 ± 0.3 58 ± 7.5 − (4.2 ± 0.5)f −39 ± 9.3 + (2.7 ± 0.7)f
P5abcΔA, by Cocco et al. (2003) 12.9 9.4 − 2.05f −43.8 + 2.06f
P5abcΔA, EDTA 23 ± 2 11.4 ± 0.5 31 ± 6.0 − (2.6 ± 0.5)f −31 ± 11 + (2.5 ± 0.3)f
P5abcΔA, by us 25.0 11.3 ± 0.6 36.2 ± 1.8 − (3.4 ± 0.2)f −27.8 ± 0.8 + (2.3 ± 0.1)f

Simulation results for the P5ab and P5abcΔA compared to the experimental data from Liphardt et al. (2001) (in bold). Cocco et al. (2003) have studied the rate constants of folding and unfolding in the presence of Mg+2. However, they did not give any results in the absence of the ion about which we concern here. We list their results as a comparison. Note in our model the τo value of the P5ab is the same with the value of the P5abcΔA, but it does not equal to the τo in the fork dynamics.