2001
DOI: 10.1073/pnas.071034098
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Free energy reconstruction from nonequilibrium single-molecule pulling experiments

Abstract: Laser tweezers and atomic force microscopes are increasingly used to probe the interactions and mechanical properties of individual molecules. Unfortunately, using such time-dependent perturbations to force rare molecular events also drives the system away from equilibrium. Nevertheless, we show how equilibrium free energy profiles can be extracted rigorously from repeated nonequilibrium force measurements on the basis of an extension of Jarzynski's remarkable identity between free energies and the irreversibl… Show more

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Cited by 856 publications
(886 citation statements)
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“…Free-energy profiles were reconstructed following a previously described procedure 3 . Briefly, we assumed a time-dependent Hamiltonian of the single-molecule pulling system of the form H (x,t ) = H 0 (x) + V (x,t ), where H 0 (x) is the Hamiltonian of the unperturbed system and V (x,t ) is the time-dependent perturbation from the trap.…”
Section: Methodsmentioning
confidence: 99%
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“…Free-energy profiles were reconstructed following a previously described procedure 3 . Briefly, we assumed a time-dependent Hamiltonian of the single-molecule pulling system of the form H (x,t ) = H 0 (x) + V (x,t ), where H 0 (x) is the Hamiltonian of the unperturbed system and V (x,t ) is the time-dependent perturbation from the trap.…”
Section: Methodsmentioning
confidence: 99%
“…These methods have been tested through nanomechanical measurements of unfolding transitions in single RNA hairpins 7,23 and applied widely 24 . Based on an extension of the Jarzynski equality, Hummer and Szabo proposed an approach to reconstructing the free-energy landscape from non-equilibrium force-ramp measurements 3 . The Jarzynski equality relates the freeenergy change of a system at a control parameter z(t ), G 0 (z), to the non-equilibrium work done,…”
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confidence: 99%
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“…Once again, in principle (but not in practice) Jarzynski's equation applies to any process no matter how far away from equilibrium and regardless of its size. Because Jarzynski's equation is so novel and counter intuitive, several useful papers have appeared that critique and extend the result (Crooks, 1999;Hummer & Szabo, 2001). Figure 4 shows five unfolding curves and five refolding curves for a RNA hairpin (Collin et al 2005); the RNA was repeatedly unfolded and refolded at a constant loading rate of 7·5 pN/ s. Clearly the process is irreversible; there is hysteresis and a distribution of transition forces.…”
Section: Jarzynski's Methods (Jarzynski 1997)mentioning
confidence: 99%
“…A major "test bed" for fluctuation theorems is provided by dynamical systems with a few degrees of freedom coupled to a thermal bath, a Brownian particle being an example. Much of the corresponding theoretical and experimental work refers to (i) modulated linear systems, where fluctuations have been studied both in transient and stationary regimes [6,7,8,9,10,11,12], and (ii) nonlinear systems, initially at thermal equilibrium, driven to a different, generally nonequilibrium state [13,14,15,16,17].…”
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confidence: 99%