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. 2005 Sep 8;437(7056):231-4.
doi: 10.1038/nature04061.

Verification of the Crooks fluctuation theorem and recovery of RNA folding free energies

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Verification of the Crooks fluctuation theorem and recovery of RNA folding free energies

D Collin et al. Nature. .

Abstract

Atomic force microscopes and optical tweezers are widely used to probe the mechanical properties of individual molecules and molecular interactions, by exerting mechanical forces that induce transitions such as unfolding or dissociation. These transitions often occur under nonequilibrium conditions and are associated with hysteresis effects-features usually taken to preclude the extraction of equilibrium information from the experimental data. But fluctuation theorems allow us to relate the work along nonequilibrium trajectories to thermodynamic free-energy differences. They have been shown to be applicable to single-molecule force measurements and have already provided information on the folding free energy of a RNA hairpin. Here we show that the Crooks fluctuation theorem can be used to determine folding free energies for folding and unfolding processes occurring in weak as well as strong nonequilibrium regimes, thereby providing a test of its validity under such conditions. We use optical tweezers to measure repeatedly the mechanical work associated with the unfolding and refolding of a small RNA hairpin and an RNA three-helix junction. The resultant work distributions are then analysed according to the theorem and allow us to determine the difference in folding free energy between an RNA molecule and a mutant differing only by one base pair, and the thermodynamic stabilizing effect of magnesium ions on the RNA structure.

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Figures

Figure 1
Figure 1. Force–extension curves
The stochasticity of the unfolding and refolding process is characterized by a distribution of unfolding or refolding work trajectories. Five unfolding (orange) and refolding (blue) force–extension curves for the RNA hairpin are shown (loading rate of 7.5 pN s−1). The blue area under the curve represents the work returned to the machine as the molecule switches from the unfolded to the folded state. The RNA sequence is shown as an inset.
Figure 2
Figure 2. Test of the CFT using an RNA hairpin
Work distributions for RNA unfolding (continuous lines) and refolding (dashed lines). We plot negative work, PR(−W), for refolding. Statistics: 130 pulls and three molecules (r = 1.5pNs−1), 380 pulls and four molecules (r = 7.5pNs−1), 700 pulls and three molecules (r = 20.0pNs−1), for a total of ten separate experiments. Good reproducibility was obtained among molecules (see Supplementary Fig. S2). Work values were binned into about ten equally spaced intervals. Unfolding and refolding distributions at different speeds show a common crossing around ΔG = 110.3kBT.
Figure 3
Figure 3. Free-energy recovery and test of the CFT for non-gaussian work distributions
Experiments were carried out on the wild-type and mutant S15 three-helix junction without Mg2+. Unfolding (continuous lines) and refolding (dashed lines) work distributions. Statistics: 900 pulls and two molecules (wild type, purple); 1,200 pulls and five molecules (mutant type, orange). Crossings between distributions are indicated by black circles. Work histograms were found to be reproducible among different molecules (error bars indicating the range of variability). Inset, test of the CFT for the mutant. Data have been linearly interpolated between contiguous bins of the unfolding and refolding work distributions.
Figure 4
Figure 4. Use of CFT to extract the stabilizing contribution of Mg2+ to the free energy of the S15 three-helix junction (wild type)
Unfolding (continuous lines) and refolding (dashed lines) work distributions. Green curves, 450 pulls and two molecules in Mg2+; purple curves, 900 pulls and two molecules without Mg2+. Crossings between distributions are indicated by black circles. Work histograms are reproducible between the molecules (error bars indicating the range of variability). Inset, the same histograms in logarithmic scale (axes labels as for the main panel) showing (vertical black bars) the regions of work values where unfolding and refolding distributions are expected to cross each other by Bennett’s acceptance ratio method (Supplementary Information).

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