Aster formation and rupture transition in semi-flexible fiber networks with mobile cross-linkers

被引:16
作者
Astroem, Jan A. [1 ]
Kumar, P. B. Sunil [2 ]
Karttunen, Mikko [3 ]
机构
[1] Helsinki Univ Technol, LCE, FI-02015 Helsinki, Finland
[2] Indian Inst Technol, Dept Phys, Madras 600036, Tamil Nadu, India
[3] Univ Western Ontario, Dept Appl Math, London, ON N6A 5B7, Canada
基金
芬兰科学院; 加拿大自然科学与工程研究理事会;
关键词
SELF-ORGANIZATION; MOLECULAR MOTORS; HEAVY-MEROMYOSIN; SMOOTH-MUSCLE; MYOSIN; FORCE; ACTIN; MICROTUBULES; MECHANICS; MOTILITY;
D O I
10.1039/b815892d
中图分类号
O64 [物理化学(理论化学)、化学物理学];
学科分类号
070304 ; 081704 ;
摘要
Fibrous active network structures whose properties are regulated by motor proteins, or simply motors, are fundamental to life. Here, a full elastic and three dimensional model for such networks and motors is presented. The effects of surface anchoring are accounted for and we demonstrate that for unidirectional motors two basic contractile phases emerge in these systems. The transition is governed by a single parameter (tau(b)/tau(c)) which is the ratio of the breaking strain (tau(b)) and the motility limiting strain (tau(c)) of the motors. For tau(b)/tau(c) less than or similar to 2 and clamped boundaries, the network ruptures and formation of local asters occurs with a high density of motors at the centre and the fibers radially spanning out. This phase displays contraction strain during the formation of asters but the network stress is relaxed once the asters have emerged, demonstrating that the formation of aster-like structures provides a mechanism for stress relaxation. For 2.7 less than or similar to tau(b)/tau(c) the network remains intact, but reaches a force equilibrium with a high contraction strain in the case of clamped boundaries. Between these two limits the network is partly ruptured. Experimental measurements (e. g. J.T. Nishizaka, H. Miyata, H. Yoshikawa, S. Ishiwata and K. Kinosita Jr., Nature, 1995, 377, 251 and J.F. Finer, R. M. Simmons, J.A. Spudich, Nature, 1994, 368, 113) indicate that actin filament and myosin motors interact with tau(b)/tau(c) approximate to 2.7 which is right at the limit of motor induced fracture for a random network, indicating that e. g. a cytoskeleton with active myosin is susceptible to rupture. This is perhaps not a coincidence and may well be an important factor contributing to cellular dynamics. In the case of free boundaries the network collapses onto one single aster. We also show that the distribution of energy on the motors is a power-law, below the motility limit energy, with the exponent -0.5.
引用
收藏
页码:2869 / 2874
页数:6
相关论文
共 40 条
[1]  
[Anonymous], 1990, Matrix Computations
[2]  
[Anonymous], 1986, Theory of Elasticity
[3]   Theory of self-assembly of microtubules and motors [J].
Aranson, Igor S. ;
Tsimring, Lev S. .
PHYSICAL REVIEW E, 2006, 74 (03)
[4]   Random networks of fibres display maximal heterogeneity in the distribution of elastic energy [J].
Astrom, J. A. ;
Timonen, J. ;
Myllys, M. ;
Fellman, J. ;
LeBell, J. .
EUROPEAN PHYSICAL JOURNAL E, 2007, 22 (01) :61-66
[5]   Strain hardening, avalanches, and strain softening in dense cross-linked actin networks [J].
Astrom, Jan A. ;
Kumar, P. B. Sunil ;
Vattulainen, Ilpo ;
Karttunen, Mikko .
PHYSICAL REVIEW E, 2008, 77 (05)
[6]   Active gels: dynamics of patterning and self-organization [J].
Backouche, F. ;
Haviv, L. ;
Groswasser, D. ;
Bernheim-Groswasser, A. .
PHYSICAL BIOLOGY, 2006, 3 (04) :264-273
[7]   Bidirectional cooperative motion of molecular motors [J].
Badoual, M ;
Jülicher, F ;
Prost, J .
PROCEEDINGS OF THE NATIONAL ACADEMY OF SCIENCES OF THE UNITED STATES OF AMERICA, 2002, 99 (10) :6696-6701
[8]  
Bathe KJ, 1982, FINITE ELEMENT PROCE, P20071
[9]  
BOAL D, 2002, MECH CELL
[10]   Dynamic stability of spindles controlled by molecular motor kinetics [J].
Campas, O. ;
Casademunt, J. ;
Pagonabarraga, I. .
EPL, 2008, 81 (04)