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Energy landscape analysis of native folding of the prion protein yields the diffusion constant, transition path time, and rates
Energy landscape analysis of native folding of the prion protein yields the diffusion constant, transition path time, and rates
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Energy landscape analysis of native folding of the prion protein yields the diffusion constant, transition path time, and rates
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Energy landscape analysis of native folding of the prion protein yields the diffusion constant, transition path time, and rates
Energy landscape analysis of native folding of the prion protein yields the diffusion constant, transition path time, and rates

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Energy landscape analysis of native folding of the prion protein yields the diffusion constant, transition path time, and rates
Energy landscape analysis of native folding of the prion protein yields the diffusion constant, transition path time, and rates
Journal Article

Energy landscape analysis of native folding of the prion protein yields the diffusion constant, transition path time, and rates

2012
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Overview
Protein folding is described conceptually in terms of diffusion over a configurational free-energy landscape, typically reduced to a one-dimensional profile along a reaction coordinate. In principle, kinetic properties can be predicted directly from the landscape profile using Kramers theory for diffusive barrier crossing, including the folding rates and the transition time for crossing the barrier. Landscape theory has been widely applied to interpret the time scales for protein conformational dynamics, but protein folding rates and transition times have not been calculated directly from experimentally measured free-energy profiles. We characterized the energy landscape for native folding of the prion protein using force spectroscopy, measuring the change in extension of a single protein molecule at high resolution as it unfolded/refolded under tension. Key parameters describing the landscape profile were first recovered from the distributions of unfolding and refolding forces, allowing the diffusion constant for barrier crossing and the transition path time across the barrier to be calculated. The full landscape profile was then reconstructed from force-extension curves, revealing a double-well potential with an extended, partially unfolded transition state. The barrier height and position were consistent with the previous results. Finally, Kramers theory was used to predict the folding rates from the landscape profile, recovering the values observed experimentally both under tension and at zero force in ensemble experiments. These results demonstrate how advances in single-molecule theory and experiment are harnessing the power of landscape formalisms to describe quantitatively the mechanics of folding.