A model for the contractility of the cytoskeleton including the effects of stress-fibre formation and dissociation

A model for the contractility of cells is presented that accounts for the dynamic reorganization of the cytoskeleton. It is motivated by three key biochemical processes: (i) an activation signal that triggers actin polymerization and myosin phosphorylation, (ii) the tension-dependent assembly of the actin and myosin into stress fibres, and (iii) the cross-bridge cycling between the actin and the myosin filaments that generates the tension. Simple relations are proposed to model these coupled phenomena and a constitutive law developed for the activation and response of a single stress fibre. This law is generalized to two- and three-dimensional cytoskeletal networks by employing a homogenization analysis and a finite strain continuum model is developed. The key features of the model are illustrated by considering: (i) a single stress fibre on a series of supports and (ii) a two-dimensional square cell on four supports. The model is shown to be capable of predicting a variety of key experimentally established characteristics including: (i) the decrease of the forces generated by the cell with increasing support compliance, (ii) the influence of cell shape and boundary conditions on the development of structural anisotropy, and (iii) the high concentration of the stress fibres both at the focal adhesions and at the sites of localized applied tension. Moreover, consistent with the experimental findings, the model predicts that multiple activation signals are more effective at developing stress fibres than a single prolonged signal.

[1]  D. Burr,et al.  Recovery periods restore mechanosensitivity to dynamically loaded bone. , 2001, The Journal of experimental biology.

[2]  Raimond L Winslow,et al.  Comparison of putative cooperative mechanisms in cardiac muscle: length dependence and dynamic responses. , 1999, American journal of physiology. Heart and circulatory physiology.

[3]  Alexander A Spector,et al.  Emergent patterns of growth controlled by multicellular form and mechanics. , 2005, Proceedings of the National Academy of Sciences of the United States of America.

[4]  L. Addadi,et al.  Force and focal adhesion assembly: a close relationship studied using elastic micropatterned substrates , 2001, Nature Cell Biology.

[5]  Anthony G. Evans,et al.  A bio-chemo-mechanical model for cell contractility , 2006, Proceedings of the National Academy of Sciences.

[6]  R. Hill Elastic properties of reinforced solids: some theoretical principles , 1963 .

[7]  C F Dewey,et al.  Theoretical estimates of mechanical properties of the endothelial cell cytoskeleton. , 1996, Biophysical journal.

[8]  Shu Chien,et al.  Handbook of Bioengineering , 1986 .

[9]  D E Ingber,et al.  Mechanotransduction across the cell surface and through the cytoskeleton. , 1993, Science.

[10]  Kenneth E. Newhouse,et al.  Handbook of Bioengineering , 1987, The Yale Journal of Biology and Medicine.

[11]  S. Suresh,et al.  Cell and molecular mechanics of biological materials , 2003, Nature materials.

[12]  J. Kolega,et al.  Effects of mechanical tension on protrusive activity and microfilament and intermediate filament organization in an epidermal epithelium moving in culture , 1986, The Journal of cell biology.

[13]  K. Burridge,et al.  Focal adhesions, contractility, and signaling. , 1996, Annual review of cell and developmental biology.

[14]  Yoram Rudy,et al.  From Genome to Physiome: Integrative Models of Cardiac Excitation , 2000, Annals of Biomedical Engineering.

[15]  P. Janmey,et al.  Tissue Cells Feel and Respond to the Stiffness of Their Substrate , 2005, Science.

[16]  R. Austin,et al.  Force mapping in epithelial cell migration. , 2005, Proceedings of the National Academy of Sciences of the United States of America.

[17]  Gregory M. Fomovsky,et al.  The development of structural and mechanical anisotropy in fibroblast populated collagen gels. , 2005, Journal of biomechanical engineering.

[18]  M. Dembo,et al.  Cell movement is guided by the rigidity of the substrate. , 2000, Biophysical journal.

[19]  D. Ingber Tensegrity: the architectural basis of cellular mechanotransduction. , 1997, Annual review of physiology.

[20]  F. Grinnell,et al.  Stress relaxation of contracted collagen gels: disruption of actin filament bundles, release of cell surface fibronectin, and down-regulation of DNA and protein synthesis. , 1991, Experimental cell research.

[21]  D. Ingber,et al.  Mechanotransduction across the cell surface and through the cytoskeleton , 1993 .

[22]  Daniel Choquet,et al.  Extracellular Matrix Rigidity Causes Strengthening of Integrin–Cytoskeleton Linkages , 1997, Cell.

[23]  Albert K. Harris,et al.  Fibroblast traction as a mechanism for collagen morphogenesis , 1981, Nature.

[24]  Joachim P Spatz,et al.  A theoretical description of elastic pillar substrates in biophysical experiments. , 2005, Chemphyschem : a European journal of chemical physics and physical chemistry.

[25]  Christopher S. Chen,et al.  Cells lying on a bed of microneedles: An approach to isolate mechanical force , 2003, Proceedings of the National Academy of Sciences of the United States of America.

[26]  Frederick Grinnell,et al.  Fibroblasts, myofibroblasts, and wound contraction , 1994, The Journal of cell biology.

[27]  D. L. Taylor,et al.  Traction forces of cytokinesis measured with optically modified elastic substrata , 1997, Nature.

[28]  Ning Wang,et al.  Directional control of lamellipodia extension by constraining cell shape and orienting cell tractional forces , 2002, FASEB journal : official publication of the Federation of American Societies for Experimental Biology.

[29]  P. Janmey,et al.  Nonlinear elasticity in biological gels , 2004, Nature.

[30]  R. Franke,et al.  Induction of human vascular endothelial stress fibres by fluid shear stress , 1984, Nature.