Nonlinear mechanics of soft fibrous networks

Mechanical networks of fibres arise on a range of scales in nature and technology, from the
cytoskeleton of a cell to blood clots, from textiles and felts to skin and collageneous tissues.
Their collective response is dependent on the individual response of the constituent filaments
as well as density, topology and order in the network. Here, we use the example of a lowdensity synthetic felt of athermal filaments to study the generic features of the mechanical
response of such networks including strain stiffening and large effective Poisson ratios.
A simple microscopic model allows us to explain these features of our observations, and
provides us with a baseline framework to understand active biomechanical networks.

A dynamic fate map of the forebrain shows how vertebrate eyes form and explains two causes of cyclopia

Mechanisms for shaping and folding sheets of cells during development are poorly understood. An example is the complex
reorganisation of the forebrain neural plate during neurulation, which must fold a sheet into a tube while evaginating two eyes
from a single contiguous domain within the neural plate. We, for the first time, track these cell rearrangements to show that
forebrain morphogenesis differs significantly from prior hypotheses. We postulate a new model for forebrain neurulation and
demonstrate how mutations affecting two signalling pathways can generate cyclopic phenotypes by disrupting normal cell
movements or introducing new erroneous behaviours.

Sensorimotor control during isothermal tracking in Caenorhabditis elegans

In order to purposefully navigate their environments,
animals rely on precise coordination between their sensory
and motor systems. The integrated performance of circuits
for sensorimotor control may be analyzed by quantifying
an animal’s motile behavior in defined sensory
environments. Here, we analyze the ability of the
nematode C. elegans to crawl isothermally in spatial
thermal gradients by quantifying the trajectories of
individual worms responding to defined spatiotemporal
thermal gradients. We show that sensorimotor control
during isothermal tracking may be summarized as a
strategy in which the worm changes the curvature of
its propulsive undulations in response to temperature
changes measured at its head. We show that a concise
mathematical model for this strategy for sensorimotor
control is consistent with the exquisite stability of the
worm’s isothermal alignment in spatial thermal gradients
as well as its more complex trajectories in spatiotemporal
thermal gradients.

Fall and rise of a viscoelastic filament

When a viscoelastic fluid blob is stretched out into a thin horizontal filament, it
sags and falls gradually under its own weight, forming a catenary-like structure that
evolves dynamically. If the ends are brought together rapidly after stretching, the
falling filament tends to straighten by rising. These two effects are strongly influenced
by the elasticity of the fluid and yield qualitatively different behaviours from the case
of a purely viscous filament analysed previously (Teichman & Mahadevan, J. Fluid
Mech. vol. 478, 2003, p. 71). Starting from the bulk equations for the motion of a
viscoelastic fluid, we derive a simplified equation for the dynamics of a viscoelastic
filament and analyse this equation in some simple settings to explain our observations.

Microtubules can bear enhanced compressive loads in living cells because of lateral reinforcements

Cytoskeletal microtubules have been proposed
to infl uence cell shape and mechanics based
on their ability to resist large-scale compressive
forces exerted by the surrounding contractile cytoskeleton.
Consistent with this, cytoplasmic microtubules are often
highly curved and appear buckled because of compressive loads. However, the results of in vitro studies suggest that microtubules should buckle at much larger length
scales, withstanding only exceedingly small compressive
forces. This discrepancy calls into question the structural
role of microtubules, and highlights our lack of quantitative
knowledge of the magnitude of the forces they experience
and can withstand in living cells. We show that intracellular microtubules do bear large-scale compressive loads
from a variety of physiological forces, but their buckling
wavelength is reduced signifi cantly because of mechanical coupling to the surrounding elastic cytoskeleton. We
quantitatively explain this behavior, and show that this
coupling dramatically increases the compressive forces
that microtubules can sustain, suggesting they can make a
more signifi cant structural contribution to the mechanical
behavior of the cell than previously thought possible

Dynamics of surfactant-driven fracture of particle rafts

We investigate the dynamic fracture of a close-packed monolayer of particles, or particle raft, floating at
a liquid-gas interface induced by the localized addition of surfactant. Unusually for a two-dimensional
solid, our experiments show that the speed of crack propagation here is not affected by the elastic
properties of the raft. Instead it is controlled by the rate at which surfactant is advected to the crack tip by
means of the induced Marangoni flows. Further, the velocity of propagation is not constant in time and the
length of the crack scales as t
3=4. More broadly, this surfactant-induced rupture of interfacial rafts suggests
ways to manipulate them for applications.

Crack-front instability in a confined elastic film

We study the undulatory instability of a straight crack front generated by peeling a
flexible elastic plate from a thin elastomeric adhesive film. We show that there is a
threshold for the onset of the instability that is dependent on the ratio of two lengthscales that arise naturally in the problem: the thickness of the film and an elastic length
defined by the stiffness of the plate and that of the film. A linear stability analysis
predicts that the wavelength of the instability scales linearly with the film thickness. Our
results are qualitatively and quantitatively consistent with recent experiments, and show
how crack fronts may lose stability due to a competition between bulk and surface effects
in the presence of multiple length scales.

Capillary rise between elastic sheets

When a paintbrush is dipped into a pot of paint and pulled out, surface tension
forces cause the individual hairs in the brush to coalesce even as the brush becomes
impregnated with paint. We study a simple model of this elastocapillary interaction
in the context of the surface-tension-driven vertical rise of a liquid between two
long flexible hydrophilic sheets that are held a small distance apart at one end. We
provide an analytic theory for the static shapes of the sheets as well as the liquid rise
height which is different from that of the classical law of Jurin, and show that our
experiments are quantitatively consistent with the theory.

Transitions to nematic states in homogeneous suspensions of high aspect ratio magnetic rods

Isotropic-nematic and nematic-nematic transitions from a homogeneous suspension of high aspect
ratio magnetic rods are studied for both Maier-Saupe and Onsager excluded volume potentials.
Asymptotic analysis in the vicinity of critical points yields insight into the stability and type of
polarized nematic states emanating from nonpolarized equilibrium states. This, in conjunction with
recently published global numerical results, yields a unified picture of the bifurcation diagram and
provides a convenient base state to study effects of external orienting fields.

Non-spherical bubbles

Non-spherical bubbles A. Balasubramaniam, M. Abkarian, L. Mahadevan and H.A. Stone,  Nature , 438, 930, 2005.