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. Author manuscript; available in PMC: 2014 Mar 14.
Published in final edited form as: Phys Chem Chem Phys. 2013 Jan 29;15(10):3372–3388. doi: 10.1039/c3cp43992e

Figure 2.

Figure 2

Folding from activated to downhill, using WW domain experiments and simulations as an example. (A and C) The bottom shows schematic free energy profiles7,49 along the Cα-RMSD reaction coordinate at temperatures below and above the melting temperature Tm. Protein populations in folded/unfolded minima (orange) and near the barrier (green) are shown as dots. The top (A) shows two probe signal profiles. They increase monotonically with reaction coordinate, and can therefore serve as experimental reaction coordinates. Different probes progress differently as the protein folds,49 yielding probe-dependent kinetics particularly when the barrier is low and the protein population samples the transition region (vertical dashed line). (B). On the molecular time scale τm (vertical dashed line) the rate coefficient is not a ‘rate constant,’ but depends on time:51 pre-activated population (green in C) reacts promptly, much faster than population that needs to be activated (orange in C). Only later does the rate coefficient ‘settle down.’ (D) In the example, at T>Tm the pre-activated population is negligible, and exponential-decay kinetics with a ‘slow’ time constant τa is observed. At T<Tm, the pre-activated population is large, and a prompt phase precedes the ‘slow’ exponential-decay kinetics. The insets in (D) show corresponding single molecule traces: For a high barrier (T>Tm in the example), the activated protein (green), is sampled rarely. For a low barrier (T<Tm), the activated protein is sampled frequently. In essence, there are always pre-activated proteins that fold promptly downhill at the ‘speed limit.’ If the barrier is large, this population is unobservably small due to the Boltzmann factor. If the barrier is small, the population becomes easy to observe.85 The terms ‘molecular time,’ ‘speed limit’, ‘transition state transit time,’ ‘downhill folding time’ refer to the same time scale, but are not identical. Also, the decay in (D) at t<τm is not necessarily an exponential with time constant τm,87 although frequently fitted as such.49, 85, 100