help button home button Biophys. J.
HOME HELP FEEDBACK SUBSCRIPTIONS ARCHIVE SEARCH TABLE OF CONTENTS

Biophysical Journal 70: 609-625 (1996)
© 1996 the Biophysical Society

This Article
Right arrow Full Text (PDF)
Right arrow Alert me when this article is cited
Right arrow Alert me if a correction is posted
Services
Right arrow Similar articles in this journal
Right arrow Similar articles in PubMed
Right arrow Alert me to new issues of the journal
Right arrow Download to citation manager
Right arrow reprints & permissions
Citing Articles
Right arrow Citing Articles via HighWire
Right arrow Citing Articles via Google Scholar
Google Scholar
Right arrow Articles by Käs, J
Right arrow Articles by Janmey, P A
Right arrow Search for Related Content
PubMed
Right arrow PubMed Citation
Right arrow Articles by Käs, J
Right arrow Articles by Janmey, P A

F-actin, a model polymer for semiflexible chains in dilute, semidilute, and liquid crystalline solutions.

J Käs, H Strey, J X Tang, D Finger, R Ezzell, E Sackmann and P A Janmey

Division of Experimental Medicine, Brigham and Women's Hospital, Harvard Medical School, Boston, Massachusetts 02115, USA. kas@calvin.bwh.harvard.edu

ABSTRACT

Single actin filaments were analyzed in solutions ranging from dilute (0.2 microgram/ml), where filaments interact only with solvent, to concentrations (4.0 mg/ml) at which F-actin forms a nematic phase. A persistence length of approximately 1.8 microns and an average length of approximately 22 microns (Kaufmann et al., 1992) identify actin as a model for studying the dynamics of semiflexible polymers. In dilute solutions the filaments exhibit thermal bending undulations in addition to diffusive motion. At higher semidilute concentrations (1.4 mg/ml) three-dimensional reconstructions of confocal images of fluorescently labeled filaments in a matrix of unlabeled F-actin reveal steric interactions between filaments, which account for the viscoelastic behavior of these solutions. The restricted undulations of these labeled chains reveal the virtual tube formed around a filament by the surrounding actin. The average tube diameter <a> scales with monomer concentration c as <a> varies; is directly proportional to c-(0.5 +/- 0.15). The diffusion of filaments in semidilute solutions (c = (0.1-2.0) mg/ml) is dominated by diffusion along the filament contour (reptation), and constraint release by remodeling of the surrounding filaments is rare. The self-diffusion coefficient D parallel along the tube decreases linearly with the chain length for semidilute solutions. For concentrations > 2.5 mg/ml a transition occurs from an isotropic entangled phase to a coexistence between isotropic and nematic domains. Analysis of the molecular motions of filaments suggests that the filaments in the aligned domains are in thermal equilibrium and that the diffusion coefficient parallel to the director D parallel is nearly independent of filament length. We also report the novel direct observation of u-shaped defects, called hairpins, in the nematic domains.




This article has been cited by other articles:


Home page
Biophys. JHome page
M. Tassieri, R. M. L. Evans, L. Barbu-Tudoran, J. Trinick, and T. A. Waigh
The Self-Assembly, Elasticity, and Dynamics of Cardiac Thin Filaments
Biophys. J., March 15, 2008; 94(6): 2170 - 2178.
[Abstract] [Full Text] [PDF]


Home page
Biophys. JHome page
Q. Zhu, C. Vera, R. J. Asaro, P. Sche, and L. A. Sung
A Hybrid Model for Erythrocyte Membrane: A Single Unit of Protein Network Coupled with Lipid Bilayer
Biophys. J., July 15, 2007; 93(2): 386 - 400.
[Abstract] [Full Text] [PDF]


Home page
Biophys. JHome page
C. P. Brangwynne, G. H. Koenderink, E. Barry, Z. Dogic, F. C. MacKintosh, and D. A. Weitz
Bending Dynamics of Fluctuating Biopolymers Probed by Automated High-Resolution Filament Tracking
Biophys. J., July 1, 2007; 93(1): 346 - 359.
[Abstract] [Full Text] [PDF]


Home page
Biophys. JHome page
E. Helfer, P. Panine, M.-F. Carlier, and P. Davidson
The Interplay between Viscoelastic and Thermodynamic Properties Determines the Birefringence of F-Actin Gels
Biophys. J., July 1, 2005; 89(1): 543 - 553.
[Abstract] [Full Text] [PDF]


Home page
J. Neurosci.Home page
O. I. Wagner, J. Lifshitz, P. A. Janmey, M. Linden, T. K. McIntosh, and J.-F. Leterrier
Mechanisms of Mitochondria-Neurofilament Interactions
J. Neurosci., October 8, 2003; 23(27): 9046 - 9058.
[Abstract] [Full Text] [PDF]


Home page
Biophys. JHome page
X. Liu and G. H. Pollack
Mechanics of F-Actin Characterized with Microfabricated Cantilevers
Biophys. J., November 1, 2002; 83(5): 2705 - 2715.
[Abstract] [Full Text] [PDF]


Home page
Proc. Natl. Acad. Sci. USAHome page
M. A. Dichtl and E. Sackmann
Microrheometry of semiflexible actin networks through enforced single-filament reptation: Frictional coupling and heterogeneities in entangled networks
PNAS, May 1, 2002; (2002) 52432499.
[Abstract] [Full Text] [PDF]


Home page
J. Appl. Physiol.Home page
G. N. Maksym, B. Fabry, J. P. Butler, D. Navajas, D. J. Tschumperlin, J. D. Laporte, and J. J. Fredberg
Mechanical properties of cultured human airway smooth muscle cells from 0.05 to 0.4 Hz
J Appl Physiol, October 1, 2000; 89(4): 1619 - 1632.
[Abstract] [Full Text] [PDF]




HOME HELP FEEDBACK SUBSCRIPTIONS ARCHIVE SEARCH TABLE OF CONTENTS
Copyright © 1996 by the Biophysical Society.