Journal
ACTA MATERIALIA
Volume 80, Issue -, Pages 67-76Publisher
PERGAMON-ELSEVIER SCIENCE LTD
DOI: 10.1016/j.actamat.2014.07.051
Keywords
Molecular dynamics (MD); Plastic deformation; Nanoporous; Nanovoid collapse; Dislocation dynamics
Funding
- Comision Nacional de Energia Atomica (CNEA)
- SeCTyP, UN Cuyo Grant
- [PICT-PRH-0092]
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We study the mechanical behavior of nanoporous gold under uniaxial compression and strain rates in the range of 10(7)-10(9) s(-1) using molecular dynamics simulations. We consider the low-porosity regime (porosity of similar to 5%), which is characterized by several stages of plastic deformation. At the onset of plasticity, pores act as if isolated by emitting shear dislocation loops. At higher deformations, the mechanical response is determined by the interactions between dislocations in the dense dislocation forest, leading to strain hardening. Increasing the strain rate results in an increasing flow stress ranging from 0.4 to 0.7 GPa within the range of applied strain rates. The von Mises stress sigma(VM) in the hardening regime features two possible power-law dependencies as a function of dislocation density rho(d): in the initial stages of plastic deformation we obtained sigma(VM) proportional to rho(2)(d), but changes to Taylor hardening crvm sigma(VM) proportional to rho(1/2)(d) at higher dislocation densities. The velocity of dislocations is estimated to be similar to 60% of the speed of sound in the early stages of plastic deformation, but later decreases dramatically due to dislocation-dislocation and dislocation-pore interactions. The unloading of the complex dislocation and stacking fault network leads to the production of vacancies. As a result, we propose that the vacancy clusters observed experimentally in recovered samples and attributed to dislocation-free plasticity are instead due to the aggregation of those vacancies left behind during recovery. (C) 2014 Acta Materialia Inc. Published by Elsevier Ltd. All rights reserved.
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