Buckling, stiffening, and negative dissipation in the dynamics of a biopolymer in an active medium
- Norio Kikuchia,
- Allen Ehrlicherb,
- Daniel Kochc,
- Josef A. Käsc,
- Sriram Ramaswamya,d,1 and
- Madan Raoe,f
- aCentre for Condensed Matter Theory, Department of Physics, Indian Institute of Science, Bangalore 560 012, India;
- bTranslational Medicine, Brigham and Women's Hospital, Harvard Medical School, One Blackfan Circle, Karp 6, Boston, MA 02115;
- cInstitute of Soft Matter Physics, Universität Leipzig, Linnéstrasse 5, 04103 Leipzig, Germany;
- dCondensed Matter Theory Unit, Jawaharlal Nehru Center for Advanced Scientific Research, Bangalore 560 064, India;
- eRaman Research Institute, C.V. Raman Avenue, Bangalore 560 080, India; and
- fNational Centre for Biological Sciences, Tata Institute of Fundamental Research, Bellary Road, Bangalore 560 065, India
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Edited by Tom C. Lubensky, University of Pennsylvania, Philadelphia, PA, and approved September 23, 2009 (received for review January 14, 2009)
Abstract
We present a generic theory for the dynamics of a stiff filament under tension, in an active medium with orientational correlations, such as a microtubule in contractile actin. In sharp contrast to the case of a passive medium, we find the filament can stiffen, and possibly oscillate or buckle, depending on both the contractile or tensile nature of the activity and the filament-medium anchoring interaction. We also demonstrate a strong violation of the fluctuation–dissipation (FD) relation in the effective dynamics of the filament, including a negative FD ratio. Our approach is also of relevance to the dynamics of axons, and our model equations bear a remarkable formal similarity to those in recent work [Martin P, Hudspeth AJ, Juelicher F (2001) Proc Natl Acad Sci USA 98:14380–14385] on auditory hair cells. Detailed tests of our predictions can be made by using a single filament in actomyosin extracts or bacterial suspensions.
Footnotes
- 1To whom correspondence should be addressed. E-mail: sriram{at}physics.iisc.ernet.in
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Author contributions: N.K., A.E., D.K., J.A.K., S.R., and M.R. designed research, performed research, and wrote the paper.
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The authors declare no conflict of interest.
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This article is a PNAS Direct Submission.
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This article contains supporting information online at www.pnas.org/cgi/content/full/0900451106/DCSupplemental.
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↵* If included, these terms would lead to shifts of effective Frank constants and additional possible instabilities in the effective equation of motion Eq. 4.
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↵† Passive stresses arising from the free-energy functional enter only at higher order in gradients.










