Abstract

Recently acoustic signature of dislocation avalanches in HCP materials was found to be long tailed in size and energy, suggesting critical dynamics. Even more recently, the intermittent plastic response was found to be generic for micro- and nano-sized systems independently of their crystallographic symmetry. These rather remarkable discoveries are reviewed in this paper in the perspective of the recent studies performed in our group. We discuss the physical origin and the scaling properties of plastic fluctuations and address the nature of their dependence on crystalline symmetry, system size, and disorder content. A particular emphasis is placed on the associated emergent behaviors, including the formation of dislocation structures, and on our ability to temper plastic fluctuations by alloying. We also discuss the "smaller is wilder" size effect that culminates in a paradoxical crack-free brittle behavior of very small, initially dislocation free crystals. We show that the implied transition between different rheological behaviors is regulated by the ratio of length scales $R=L/l$, where $L$ is the system size and $l$ is the internal length. We link this new size effect with other related phenomena like size dependence of strength ("smaller is stronger") and the size induced switch between different hardening mechanisms. One of the technological challenges in nanoscience is to tame the intermittency of plastic flow. We show that this task can be accomplished by generating tailored quenched disorder which allows one to control micro- and nano-scale forming and opens new perspectives in micro-metallurgy and structural engineering of ultra-small load-carrying elements. These results could not be achieved by conventional methods that do not explicitly consider the stochastic nature of collective dislocation dynamics.

Highlights

  • Beyond the qualitative pioneering study of Becker and Orowan [1], the fluctuating nature of crystal plasticity has been largely overlooked for a long time, not in the least, because for most materials of engineering interest these fluctuations remained almost undetectable and considered as negligible comparing to the macroscopic response at bulk scales

  • The acoustic signature of dislocation avalanches in HCP materials was found to be long tailed in size and energy, suggesting critical dynamics [2, 3]

  • The results presented above argue for a BD transition “without a crack”, i.e. in terms of collective behavior of dislocations characterized by a particular scale-free structure of plastic fluctuations

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Summary

Introduction

Beyond the qualitative pioneering study of Becker and Orowan [1], the fluctuating nature of crystal plasticity has been largely overlooked for a long time, not in the least, because for most materials of engineering interest these fluctuations remained almost undetectable and considered as negligible comparing to the macroscopic response at bulk scales. The situation changed only when new technology opened a way to precision measurement of acoustic emissions accompanying plastic deformation. The acoustic signature of dislocation avalanches in HCP materials was found to be long tailed in size and energy, suggesting critical dynamics [2, 3]. The intermittent plastic response was found to be generic for micro- and nano-sized systems independently of their crystallographic symmetry The intermittent plastic response was found to be generic for micro- and nano-sized systems independently of their crystallographic symmetry (e.g. [4, 5])

Continuum mechanics versus discrete approaches
The goals of this review
Historical background
From subcritical to supercritical plasticity
The concept of wildness
External versus internal length scales
Alloys
Wildness versus strength
Modelling
Mesoscopic model
Mean-field model
Conclusions
Full Text
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