Revealing the bifurcation in the unfolding pathways of GFP by using single-molecule experiments and simulations

  1. Moritz Mickler*,
  2. Ruxandra I. Dima,
  3. Hendrik Dietz*,
  4. Changbong Hyeon,§,
  5. D. Thirumalai,, and
  6. Matthias Rief*,,**
  1. *Physik Department E22, Technische Universität München, James-Franck-Strasse, D-85748 Garching, Germany;
  2. Department of Chemistry, University of Cincinnati, Cincinnati, OH 45221;
  3. Center for Theoretical Biological Physics, University of California at San Diego, La Jolla, CA 92093;
  4. §Department of Chemistry, Chung-Ang University, Seoul 156-756, Republic of Korea;
  5. Biophysics Program, Institute for Physical Science and Technology, University of Maryland, College Park, MD 20741; and
  6. **Munich Center for Integrated Protein Science CiPSM, 81377 Munich, Germany
  1. Edited by José N. Onuchic, University of California at San Diego, La Jolla, CA, and approved October 25, 2007 (received for review June 11, 2007)

Abstract

Nanomanipulation of biomolecules by using single-molecule methods and computer simulations has made it possible to visualize the energy landscape of biomolecules and the structures that are sampled during the folding process. We use simulations and single-molecule force spectroscopy to map the complex energy landscape of GFP that is used as a marker in cell biology and biotechnology. By engineering internal disulfide bonds at selected positions in the GFP structure, mechanical unfolding routes are precisely controlled, thus allowing us to infer features of the energy landscape of the wild-type GFP. To elucidate the structures of the unfolding pathways and reveal the multiple unfolding routes, the experimental results are complemented with simulations of a self-organized polymer (SOP) model of GFP. The SOP representation of proteins, which is a coarse-grained description of biomolecules, allows us to perform forced-induced simulations at loading rates and time scales that closely match those used in atomic force microscopy experiments. By using the combined approach, we show that forced unfolding of GFP involves a bifurcation in the pathways to the stretched state. After detachment of an N-terminal α-helix, unfolding proceeds along two distinct pathways. In the dominant pathway, unfolding starts from the detachment of the primary N-terminal β-strand, while in the minor pathway rupture of the last, C-terminal β-strand initiates the unfolding process. The combined approach has allowed us to map the features of the complex energy landscape of GFP including a characterization of the structures, albeit at a coarse-grained level, of the three metastable intermediates.

Footnotes

  • To whom correspondence may be addressed. E-mail: thirum{at}umd.edu or mrief{at}ph.tum.de
  • Author contributions: M.M. and R.I.D. contributed equally; R.I.D., D.T., and M.R. designed research; M.M., R.I.D., H.D., and C.H. performed research; M.M., R.I.D., H.D., C.H., D.T., and M.R. analyzed data; and R.I.D., D.T., and M.R. wrote the paper.

  • The authors declare no conflict of interest.

  • This article is a PNAS Direct Submission.

  • This article contains supporting information online at www.pnas.org/cgi/content/full/0705458104/DC1.

« Previous | Next Article »Table of Contents