- •Contents
- •Contributors
- •Preface
- •1 Introduction, with the biological basis for cell mechanics
- •Introduction
- •The role of cell mechanics in biological function
- •Maintenance of cell shape
- •Cell migration
- •Mechanosensing
- •Stress responses and the role of mechanical forces in disease
- •Active cell contraction
- •Structural anatomy of a cell
- •The extracellular matrix and its attachment to cells
- •Transmission of force to the cytoskeleton and the role of the lipid bilayer
- •Intracellular structures
- •Overview
- •References
- •2 Experimental measurements of intracellular mechanics
- •Introduction
- •Forces to which cells are exposed in a biological context
- •Methods to measure intracellular rheology by macrorheology, diffusion, and sedimentation
- •Whole cell aggregates
- •Sedimentation of particles
- •Diffusion
- •Mechanical indentation of the cell surface
- •Glass microneedles
- •Cell poker
- •Atomic force microscopy
- •Mechanical tension applied to the cell membrane
- •Shearing and compression between microplates
- •Optical traps
- •Magnetic methods
- •Twisting of magnetized particles on the cell surface and interior
- •Passive microrheology
- •Optically detected individual probes
- •One-particle method
- •Two-particle methods
- •Dynamic light scattering and diffusing wave spectroscopy
- •Fluorescence correlation spectroscopy
- •Optical stretcher
- •Acoustic microscopy
- •Outstanding issues and future directions
- •References
- •3 The cytoskeleton as a soft glassy material
- •Introduction
- •Magnetic Twisting Cytometry (MTC)
- •Measurements of cell mechanics
- •The structural damping equation
- •Reduction of variables
- •Universality
- •Scaling the data
- •Collapse onto master curves
- •Theory of soft glassy rheology
- •What are soft glassy materials
- •Sollich’s theory of SGMs
- •Soft glassy rheology and structural damping
- •Open questions
- •Biological insights from SGR theory
- •Malleability of airway smooth muscle
- •Conclusion
- •References
- •4 Continuum elastic or viscoelastic models for the cell
- •Introduction
- •Purpose of continuum models
- •Principles of continuum models
- •Boundary conditions
- •Mechanical and material characteristics
- •Example of studied cell types
- •Blood cells: leukocytes and erythrocytes
- •Limitations of continuum model
- •Conclusion
- •References
- •5 Multiphasic models of cell mechanics
- •Introduction
- •Biphasic poroviscoelastic models of cell mechanics
- •Analysis of cell mechanical tests
- •Micropipette aspiration
- •Cells
- •Biphasic properties of the pericellular matrix
- •Indentation studies of cell multiphasic properties
- •Analysis of cell–matrix interactions using multiphasic models
- •Summary
- •References
- •6 Models of cytoskeletal mechanics based on tensegrity
- •Introduction
- •The cellular tensegrity model
- •The cellular tensegrity model
- •Do living cells behave as predicted by the tensegrity model?
- •Circumstantial evidence
- •Prestress-induced stiffening
- •Action at a distance
- •Do microtubules carry compression?
- •Summary
- •Examples of mathematical models of the cytoskeleton based on tensegrity
- •The cortical membrane model
- •Tensed cable nets
- •Cable-and-strut model
- •Summary
- •Tensegrity and cellular dynamics
- •Conclusion
- •Acknowledgement
- •References
- •7 Cells, gels, and mechanics
- •Introduction
- •Problems with the aqueous-solution-based paradigm
- •Cells as gels
- •Cell dynamics
- •Gels and motion
- •Secretion
- •Muscle contraction
- •Conclusion
- •Acknowledgement
- •References
- •8 Polymer-based models of cytoskeletal networks
- •Introduction
- •The worm-like chain model
- •Force-extension of single chains
- •Dynamics of single chains
- •Network elasticity
- •Nonlinear response
- •Discussion
- •References
- •9 Cell dynamics and the actin cytoskeleton
- •Introduction: The role of actin in the cell
- •Interaction of the cell cytoskeleton with the outside environment
- •The role of cytoskeletal structure
- •Actin mechanics
- •Actin dynamics
- •The emergence of actin dynamics
- •The intrinsic dynamics of actin
- •Regulation of dynamics by actin-binding proteins
- •Capping protein: ‘decommissioning’ the old
- •Gelsolin: rapid remodeling in one or two steps
- •β4-thymosin: accounting (sometimes) for the other half
- •Dynamic actin in crawling cells
- •Actin in the leading edge
- •Monomer recycling: the other ‘actin dynamics’
- •The biophysics of actin-based pushing
- •Conclusion
- •Acknowledgements
- •References
- •10 Active cellular protrusion: continuum theories and models
- •Cellular protrusion: the standard cartoon
- •The RIF formalism
- •Mass conservation
- •Momentum conservation
- •Boundary conditions
- •Cytoskeletal theories of cellular protrusion
- •Network–membrane interactions
- •Network dynamics near the membrane
- •Special cases of network–membrane interaction: polymerization force, brownian and motor ratchets
- •Network–network interactions
- •Network dynamics with swelling
- •Other theories of protrusion
- •Numerical implementation of the RIF formalism
- •An example of cellular protrusion
- •Protrusion driven by membrane–cytoskeleton repulsion
- •Protrusion driven by cytoskeletal swelling
- •Discussion
- •Conclusions
- •References
- •11 Summary
- •References
- •Index
94 F. Guilak et al.
Fig. 5-5. Micropipette aspiration of the pericellular matrix (PCM) of chondrocytes. This region surrounds cells in articular cartilage, similar to a glycocalyx, but contains significant amounts of extracellular matrix collagens, proteoglycans, and other macromolecules. The mechanical properties of this region appear to have a significant influence on the stress-strain and fluid-flow environment of the cell. From Alexopoulos et al., 2005.
Young’s modulus of the PCM was significantly decreased (38.7 ± 16.2 kPa vs. 23.5 ± 12.9 kPa, p < 0.001), and the permeability was significantly elevated (4.19 ± 3.78 × 10−17 m4/N·s vs. 10.2 ± 9.38 × 10−17 m4/N·s, p < 0.001). The Poisson ratio was similar for both nondegenerate and osteoarthritic PCM (0.044 ± 0.063 vs. 0.030 ± 0.068, p > 0.6). These findings suggest that the PCM may undergo enzymatic and mechanical degradation with osteoarthritis, similar to that occurring in the ECM. In combination with previous theoretical models of cell–matrix interactions in cartilage, these findings suggest that changes in the properties of the PCM may have an important influence on the biomechanical environment of the cell.
Together, these studies support the utility of in vitro mechanical analyses of isolated functional cell–matrix units. Because cartilage, in particular, is avascular and aneural, characterization of PCM mechanical and chemical properties is a key step toward characterizing the in vivo state of the cell and its metabolic response to alterations in the local cellular environment. The triphasic model provides a framework for developing extended models of the PCM that can delineate effects of the distinct mechanochemical composition of the PCM, relative to the ECM, on the local environment of the cell.
Indentation studies of cell multiphasic properties
In addition to micropipette aspiration, various techniques for cellular indentation have been used to measure the modulus of adherent cells, including cell indentation (Daily et al., 1984; Duszyk et al., 1989; Zahalak et al., 1990), scanning probe microscopy (Radmacher et al., 1992; Shroff et al., 1995), or cytoindentation (Shin and Athanasiou, 1999; Koay et al., 2003). (See also the discussion of experimental approaches in Chapter 2.) The conceptual basis of these techniques is generally similar, in that a rigid probe is used to indent the cell and the ensuing creep or stress-relaxation behavior
Multiphasic models of cell mechanics |
95 |
(a)CELL AND PERICELLULAR MATRIX MODEL
(b)
R
R
Fig. 5-6. (a) Biphasic finite element mesh of the micropipette aspiration experiment. The cell and pericellular matrix were modeled using an axisymmetric mesh with bilinear quadrilateral elements (342 nodes, 314 elements). (b) Transient response of normal and osteoarthritic chondrons (cell with the pericellular matrix), and the associated biphasic prediction of their mechanical behavior. The transient mechanical behavior of the PCM was well-described by a biphasic model, suggesting that the viscoelastic response of the pericellular matrix is attributable to flow-dependent effects, similar to that of the extracellular matrix. From Alexopoulos et al., 2005 with permission.
is recorded. These techniques have generally used elastic or viscoelastic models to calculate the equilibrium or dynamic moduli of cells over a range of frequencies. In one set of cell indentation experiments, MG63 osteoblast-like cells were modeled with either a linear elasticity solution of half-space indentation or the linear biphasic theory under the assumption that the viscoelastic behavior of each cell was due to the interaction between the solid cytoskeletal matrix and the cytoplasmic fluid (Shin and Athanasiou, 1999). The intrinsic biphasic material properties (aggregate modulus, Poisson’s ratio, and permeability) were determined by curve-fitting the experimental surface reaction force and deformation with a linear biphasic finite element code in conjunction with optimization routines. These cells exhibited a compressive aggregate modulus