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Fluid Dynamics Seminar
Thursday, Jan. 31, 2013,
4:00 PM
Cullimore, Room 611
New Jersey Institute of Technology
Rheology of cytoskeleton: from mesoscopic mechanics to macroscopic instabilities
Len Pismen
Department of Chemical Engineering - Technion,
Israel Institute of Technology
Abstract
Cytoskeleton is the principal structural element of eukaryotic cells
responsible for their integrity, reshaping, proliferation and motion.
Its main building blocks are actin filaments - semiflexible polymer
chains cross-linked into a network and prestressed by molecular
motors. Cytoskeleton is a highly complex polar medium characterized by
nonlinear viscoelastic response that may be modified by external
forces or chemical signals. It is an active medium driven out of
equilibrium by ATP hydrolysis, needed both for continuous
polymerization (treadmilling) and for generating stress induced by
myosin motors.
The talk concentrates upon specific rheological properties of
cytoskeleton caused by the presence of motors, which result both in
generation of active forces and in flexible anisotropic response to
external forcing, that may lead to opposite effects of fluidization or
reinforcement. A mesoscopic description of cytoskeleton is aimed at
deducing its macroscopic response based on microstructural
characteristics, including chemo-mechanical interactions related to
motor activity and assembly or disintegration of acto-myosin stress
cables.
On the macroscopic level, the challenging problem of cytoskeleton
mechanics lies in strong interactions among the three interconnected
fields - network polarization, elastic deformation, and motor activity
causing prestress and agitation of the network. We explore nonlinear
dynamics of an active polarizable layer based on generic continuum
model with neo-Hookean elasticity and chemo-mechanical interactions.
The model exhibits two kinds of instabilities: a stationary long
wavelength instability can be observed if the medium is activated by
expansion, while an oscillatory short wavelength instability can occur
in the case of compressive activation. The former instability may lead
to the spontaneous polarization effect, and the latter, to patchiness
and oscillations in tissue reshaping.