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Randomness and slip avalanches in gradient plasticity
Institution:1. The University of Edinburgh, Institute for Materials and Processes, The King’s Buildings, Sanderson Building, Edinburgh EH11DT, UK;2. Aristotle University of Thessaloniki, Laboratory of Mechanics and Materials, Polytechnic School, Box 468, 54124 Thessaloniki, Greece;3. Michigan Technological University, Center for the Mechanics of Material Instabilities and Material Processes, Houghton, MI 49931, USA;1. School of Materials Science and Engineering, Ulsan National Institute of Science and Technology, Ulsan 689–798, Republic of Korea;2. School of Materials Science and Engineering, University of Ulsan, Ulsan 680–749, Republic of Korea;1. Institute of Heavy Ion Physics, State Key Laboratory of Nuclear Science and Technology, Peking University, Beijing 100871, China;2. School of Physical Science and Nuclear Engineering, Beihang University, Beijing 100191, China
Abstract:While localization of deformation at macroscopic scales has been documented and carefully characterized long ago, it is only recently that systematic experimental investigations have demonstrated that plastic flow of crystalline solids on mesoscopic scales proceeds in a strongly heterogenous and intermittent manner. In fact, deformation is characterized by intermittent bursts (‘slip avalanches’) the sizes of which obey power-law statistics. In the spatial domain, these avalanches produce characteristic deformation patterns in the form of slip lines and slip bands. Unlike to the case of macroscopic localization where gradient plasticity can capture the width and spacing of shear bands in the softening regime of the stress–strain graph, this type of mesoscopically jerky like localized plastic flow is observed in spite of a globally convex stress–strain relationship and may not be captured by standard deterministic continuum modelling. We thus propose a generalized constitutive model which includes both second-order strain gradients and randomness in the local stress–strain relationship. These features are related to the internal stresses which govern dislocation motion on microscopic scales. It is shown that the model can successfully describe experimental observations on slip avalanches as well as the associated surface morphology characteristics.
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