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Originally published as Biophys J. BioFAST on February 9, 2007.
doi:10.1529/biophysj.106.094052
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Biophysical Journal 92:2996-3009 (2007)
© 2007 The Biophysical Society

Force Unfolding Kinetics of RNA Using Optical Tweezers. I. Effects of Experimental Variables on Measured Results

Jin-Der Wen *, Maria Manosas §, Pan T. X. Li *, Steven B. Smith {dagger}, Carlos Bustamante * {dagger} {ddagger}, Felix Ritort § ¶ and Ignacio Tinoco, Jr. *

* Department of Chemistry, {dagger} Department of Physics, and {ddagger} Department of Molecular and Cell Biology and Howard Hughes Medical Institute, University of California, Berkeley, California; § Departament de Fisica Fonamental, Facultat de Fisica, Universitat de Barcelona, 08028 Barcelona, Spain; and CIBER de Bioingenieria, Biomateriales i Nanomedicina, Instituto de Sanidad Carlos III, Madrid, Spain

Correspondence: Address reprint requests to I. Tinoco, Tel.: 510-526-3817; E-mail: intinoco{at}lbl.gov.

Experimental variables of optical tweezers instrumentation that affect RNA folding/unfolding kinetics were investigated. A model RNA hairpin, P5ab, was attached to two micron-sized beads through hybrid RNA/DNA handles; one bead was trapped by dual-beam lasers and the other was held by a micropipette. Several experimental variables were changed while measuring the unfolding/refolding kinetics, including handle lengths, trap stiffness, and modes of force applied to the molecule. In constant-force mode where the tension applied to the RNA was maintained through feedback control, the measured rate coefficients varied within 40% when the handle lengths were changed by 10-fold (1.1–10.2 Kbp); they increased by two- to threefold when the trap stiffness was lowered to one-third (from 0.1 to 0.035 pN/nm). In the passive mode, without feedback control and where the force applied to the RNA varied in response to the end-to-end distance change of the tether, the RNA hopped between a high-force folded-state and a low-force unfolded-state. In this mode, the rates increased up to twofold with longer handles or softer traps. Overall, the measured rates remained with the same order-of-magnitude over the wide range of conditions studied. In the companion article on pages 3010–3021, we analyze how the measured kinetics parameters differ from the intrinsic molecular rates of the RNA, and thus how to obtain the molecular rates.


Related articles in Biophys. J.:

Force Unfolding Kinetics of RNA using Optical Tweezers. II. Modeling Experiments
M. Manosas, J.-D. Wen, P. T. X. Li, S. B. Smith, C. Bustamante, I. Tinoco, Jr., and F. Ritort
Biophys. J. 2007 92: 3010-3021. [Abstract] [Full Text]  



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E. B. Walton, S. Lee, and K. J. Van Vliet
Extending Bell's Model: How Force Transducer Stiffness Alters Measured Unbinding Forces and Kinetics of Molecular Complexes
Biophys. J., April 1, 2008; 94(7): 2621 - 2630.
[Abstract] [Full Text] [PDF]




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