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Research
The group is currently interested
in some basic questions in non-equilibrium and statistical physics as
revealed in various problems in materials science and solid
mechanics. We are especially interested in problems that involve many
interacting time and length scales, where conceptual and mathematical
bridges between microscopic physics and continuum field theories are
essential. In many of these problems the major challenge is to
understand how collective microscopic processes give rise to emergent
macroscopic behaviors that can be described by relatively simple
partial differential equations; these should be fully consistent with
fundamental principles of physics and thermodynamics and incorporate a
few constitutive relations to link between the different scales.
Dynamic fracture
- Instabilities: branching, oscillations, cavitation
- Weakly nonlinear theory, crack tip singularity
The ability of solids to withstand
mechanical forces is one of their fundamental properties. When a solid
is loaded externally, there reaches a point where its global energy
can be reduced by breaking into pieces, i.e by creating new free
surfaces instead of continuing to store mechanical energy. The major
vehicle for these failure processes are cracks, which are
non-equilibrium propagating dissipative structures. Cracks are
"natural laboratories" for probing material behavior under extreme
conditions as their tips concentrate stresses and strains that
approach a mathematical singularity. Moreover, crack propagation
involves many interacting time and length scales ranging from the
linear elastic forcing on large scales to the strong non-linearities
and dissipation on the small scales near the crack's tip.
Cracks often exhibit rather
complex dynamics, including some poorly understood instabilities, and
the laws that govern their motion have remained an object of constant
study for nearly a century. My research aims at understanding the
origin of crack tip instabilities and the structure of the near tip
region. The research combines theoretical tools (classical field
theory, asymptotic expansions, perturbation theory, complex analysis,
field singularities) and close interaction with experimental work.
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The post-mortem crack pattern.
A sequence of photographs of a rapidly propagating
crack undergoing a transition from straight (top two pictures) to oscillatory motion,
courtesy of A. Livne and J. Fineberg.
See also Phys. Rev. Lett. 98, 124301 (2007). |
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(a) A sketch of a crack propagation experiment (left).
A ~5mm2 close-up on the crack tip region (center).
The dashed red line is the parabolic crack tip opening profile predicted by Linear Elastic
Fracture Mechanics (LEFM). Zooming in on the crack tip region reveals the existence of a nonlinear zone (deviation
from the parabolic profile), whose size is denoted by δ (right).
(b) Blowup of the near-tip region with an imprinted tracer field that allows a direct measurement of
the deformation (left). The measured yy-component of the strain field near the tip of the crack
(right). The "singular" behavior is apparent. Quantitative analysis of this field confirmed the
weakly nonlinear theory of dynamic fracture.
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Selected publications:
- The Near-Tip Fields of Fast Cracks
A. Livne, E. Bouchbinder, I. Svetlizky, J. Fineberg
Science 327, 1359 (2010).
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Dynamic Crack Tip Equation of Motion: High-speed Oscillatory Instability
E. Bouchbinder
Phys. Rev. Lett. 103, 164301 (2009).
arXiv:0908.1178
- The 1/r Singularity in Weakly Nonlinear Fracture Mechanics
E. Bouchbinder, A. Livne, J. Fineberg
J. Mech. Phys. Solids 57, 1568 (2009). arXiv:0902.2121
- Weakly Nonlinear Theory of Dynamic Fracture
E. Bouchbinder, A. Livne, J. Fineberg
Phys. Rev. Lett. 101, 264302 (2008). arXiv:0807.4868
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Breakdown of Linear Elastic Fracture Mechanics near the Tip of a Rapid Crack
A. Livne, E. Bouchbinder, J. Fineberg
Phys. Rev. Lett. 101, 264301 (2008). arXiv:0807.4866
Statistical physics of cracks (roughness)
- Quasi-static crack growth models, the iterated conformal mapping method
- The roughness of fracture surfaces
One of the major goals of the physics of complex systems is to
characterize the patterns observed in nature and to explain how these
emerge from simple mathematical models. The spatio-temporal dynamics
of cracks generate a wealth of patterns that call for theoretical
investigation. One of the remarkable properties of many fracture
surfaces is that they exhibit self-affine symmetry. This property
implies that the fluctuations of the surface about its mean height are
statistically invariant under an anisotropic scale transformation
characterized by a roughness exponent. We have developed several
stochastic, quasi-static crack growth models that account for the
interplay between the mechanics of cracks with complex geometries and
material disorder. These models generated rough fracture surfaces
with self-affine scaling properties.
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The fracture surface of the aluminum alloy
obtained by J.-J. Ammann and E. Bouchaud, Eur. Phys. J. Appl. Phys. 4,
133 (1998). The raw data was analyzed using the irreducible
representations of the SO(2) symmetry group, see Phys. Rev. Lett. 95,
255503 (2005)
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Selected publications:
- Statistical Physics of Fracture Surfaces Morphology
E. Bouchbinder, I. Procaccia, S. Sela
J. Stat. Phys. 125, 1029 (2006). arXiv:cond-mat/0510368
- Fracture Surfaces as Multiscaling Graphs
E. Bouchbinder, I. Procaccia, S. Santucci, L. Vanel
Phys. Rev. Lett. 96, 055509 (2006). arXiv:cond-mat/0508183
- Disentangling Scaling Properties in Anisotropic Fracture
E. Bouchbinder, I. Procaccia, S. Sela
Phys. Rev. Lett. 95, 255503 (2005). arXiv:cond-mat/0508549
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Roughening of Fracture Surfaces: the Role of Plastic Deformations
E. Bouchbinder, J. Mathiesen, I. Procaccia
Phys. Rev. Lett. 92, 245505 (2004). arXiv:cond-mat/0312669
Nonequilibrium thermodynamics of driven glassy systems
- Internal variables theory
- Effective temperature theory
- Glassy dynamics/phenomena
Glassy systems are usually regarded as the paradigmatic examples of
non-equilibrium systems because they exhibit an anomalously slow
relaxation behavior and a broken time-translation invariance
(ergodicity breaking). These systems are driven even further from
equilibrium when deformed by externally applied forces. Under such
conditions, standard equilibrium thermodynamics is
inapplicable. Therefore, a basic theoretical question is whether there
exists a generalized thermodynamic formalism for such systems.
In a recent work we have developed an internal-variable,
effective-temperature non-equilibrium thermodynamics for glass-forming
materials driven away from thermodynamic equilibrium by external
forces. The basic idea is that the slow configurational degrees of
freedom of such materials are weakly coupled to the fast
kinetic-vibrational degrees of freedom and therefore these two
subsystems can be described by different temperatures during
deformation. The configurational subsystem contains coarse-grained
internal variables that are state variables that account for the
effect of the evolving glassy structure on various mechanical
properties. We highlighted the need for understanding how both energy
and entropy are shared by the different components of the system and
use the first and second laws of thermodynamics to constrain the
equations of motion for the internal variables and the effective
temperature.
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Visualization of the composition of a computer simulated amorphous silicon in terms of solid-like (blue)
and liquid-like (green) atomic environments, courtesy of M. Demkowicz (see also Phil. Mag. 86, 4153
(2006)). A theoretical analysis of the deformation of this simulated amorphous silicon is presented in Phys.
Rev. E 75, 036107 (2007).
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Selected publications:
Irreversible plastic deformation
- Elasto-plasticity of amorphous systems,
Shear-Transformation-Zones (STZ) theory
- Dislocation-mediated plasticity, strain hardening
The ability of solids to deform irreversibly, i.e. plastically, is of
enormous importance to human kind. Yet, we have a rather limited
fundamental understanding of the physics of plastic deformation in
amorphous and heavily dislocated solids. The ultimate theoretical
challenge in these fields is to develop dynamic equations of motion -
the analog of the Navier Stokes equations - for amorphous and heavily
dislocated solids. Building on advances in understanding amorphous
materials, through detailed experiments and computer simulations, we
have recently extended the original Shear-Transformation-Zones (STZ)
theory to conform with the internal-variable, effective-temperature
non-equilibrium thermodynamics discussed above. Furthermore, we have
recently explored the implications of this thermodynamic framework to
strain hardening theory of heavily dislocated polycrystalline solids.
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A level set simulation of a continuously deformed bar undergoing a
necking instability, using the Shear- Transformation-Zones (STZ)
theory. The color code represents the magnitude of the effective
temperature that quantifies the degree of local structural
disorder. The emergence of shear bands prior to failure is
evident.
Figure courtesy of Chris Rycroft, UC Berkeley and the
Lawrence Berkeley Laboratory.
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A level set simulation of an expanding circular hole using the Shear-Transformation-Zones (STZ)
theory. The perfect circular hole is disturbed by a finite amplitude perturbation in order to study the
shape stability of the expanding hole. The color code as above. A non-stationary linear stability
analysis of this problem is presented in Phys. Rev. E 78, 026124 (2008).
Figure courtesy of Chris
Rycroft, UC Berkeley and the Lawrence Berkeley Laboratory.
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Selected publications:
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