Paddling mechanism for the substrate translocation by AAA+ motor revealed by multiscale molecular simulations

  1. Nobuyasu Kogaa,b,1,2,
  2. Tomoshi Kamedac,1,
  3. Kei-ichi Okazakib and
  4. Shoji Takadaa,b,d,3
  1. aDepartment of Biophysics, Kyoto University, Sakyo, Kyoto 606-8502, Japan;
  2. bGraduate School of Science and Technology, Kobe University, Nada, Kobe 657-8501, Japan;
  3. cComputational Biology Research Center (CRBC), Advanced Industrial Science and Technology (AIST), 2-43 Aomi, Koto, Tokyo 135-0064, Japan; and
  4. dCREST, Japan Science and Technology Agency, 4-1-8, Honcho, Kawaguchi-shi,Saitama 332-0012 Japan
  • 2Present address: Department of Biochemistry, University of Washington, J Wing, Health Sciences Building, Box 357350, Seattle, WA 98195.

  1. 1N.K. and T.K. contributed equally to this work.

  2. Edited by Peter G. Wolynes, University of California at San Diego, La Jolla, CA, and approved August 11, 2009 (received for review April 30, 2009)

Abstract

Hexameric ring-shaped AAA+ molecular motors have a key function of active translocation of a macromolecular chain through the central pore. By performing multiscale molecular dynamics (MD) simulations, we revealed that HslU, a AAA+ motor in a bacterial homologue of eukaryotic proteasome, translocates its substrate polypeptide via paddling mechanism during ATP-driven cyclic conformational changes. First, fully atomistic MD simulations showed that the HslU pore grips the threaded signal peptide by the highly conserved Tyr-91 and Val-92 firmly in the closed form and loosely in the open form of the HslU. The grip depended on the substrate sequence. These features were fed into a coarse-grained MD, and conformational transitions of HslU upon ATP cycles were simulated. The simulations exhibited stochastic unidirectional translocation of a polypeptide. This unidirectional translocation is attributed to paddling motions of Tyr-91s between the open and the closed forms: downward motions of Tyr-91s with gripping the substrate and upward motions with slipping on it. The paddling motions were caused by the difference between the characteristic time scales of the pore-radius change and the up-down displacements of Tyr-91s. Computational experiments on mutations at the pore and the substrate were in accord with several experiments.

Footnotes

  • 3To whom correspondence should be addressed. E-mail: takada{at}biophys.kyoto-u.ac.jp
  • Author contributions: N.K., T.K., and S.T. designed research; N.K. and T.K. performed research; N.K. performed research of CG simulations, and T.K. performed research of fully atomistic simulations; N.K., T.K., and K.-i.O. contributed new analytic tools; N.K. and T.K. analyzed data; and N.K., T.K., and S.T. wrote the paper.

  • The authors declare no conflict of interest.

  • This article is a PNAS Direct Submission.