Abstract

In this study, we use discrete dislocation dynamics simulation to investigate the effect of heterogeneous dislocation density on the transition between quasi-elastic deformation and plastic flow in face-centered cubic single crystals. By analyzing the stress–strain curves of samples with an initial, axial dislocation density gradient, we arrive at the following conclusions: (i) in the regime of quasi-elastic deformation before the onset of plastic flow, the effective elastic modulus of the simulated samples falls significantly below the value for a dislocation-free crystal. This modulus reduction increases with decreasing dislocation density gradient: crystals with homogeneous dislocation distribution are thus weakest in the quasi-elastic regime; (ii) the transition towards plastic flow occurs first in regions of reduced dislocation density. Therefore, the overall yield stress decreases with increasing dislocation density gradient; (iii) crystals with dislocation density gradient exhibit a more pronounced hardening stage during which stress is re-distributed onto stronger regions with higher dislocation density until the sample flows at a constant flow stress that is approximately independent of dislocation density gradient. We interpret these findings in terms of a continuum dislocation dynamics inspired model of dislocation density evolution that accounts for geometrically reversible (‘inversive’) dislocation motions. The transition between quasi-elastic and plastic deformation is interpreted as a transition from inversive to non-inversive dislocation motion, and the initial differences in elastic modulus are related to a density dependent polarizability of the dislocation system. The subsequent plastic flow behavior is analyzed in terms of a modified version of Mughrabi’s composite model.

Highlights

  • Graded microstructures can be observed in many biological materials, such as bones, bamboo, shells, etc., where the microstructure change gradually

  • The overall yield stress decreases with increasing dislocation density gradient; (iii) crystals with dislocation density gradient exhibit a more pronounced hardening stage during which stress is re-distributed onto stronger regions with higher dislocation density until the sample flows at a constant flow stress that is approximately independent on dislocation density gradient

  • We have studied the transition from quasi-elastic behavior to plastic flow in small samples containing either a homogeneous distribution of dislocations or a heterogeneous distribution with a dislocation density gradient

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Summary

Introduction

Graded microstructures can be observed in many biological materials, such as bones, bamboo, shells, etc., where the microstructure change gradually These graded structures are the result of natural selection and natural evolution, and almost all of them have some special excellent properties [1]. The paper is organized as follows: We first give a concise presentation of the simulation method and present the results obtained by DDD simulation, which we discuss in terms of characteristic differences of dislocation behavior in the quasi-elastic/microplastic and the plastic deformation regime of microcrystals with and without dislocation density gradient. We move to a more theoretical description, where we formulate a dislocation density based framework to interpret the characteristic differences between dislocation behavior in graded and non-graded samples, and between quasi-elastic and plastic deformation regimes. We conclude with a brief discussion that puts our results into the general context of recent interpretations of the elastic-plastic transition

Simulation Set-up
Sample geometry
Initial and boundary conditions Our initial dislocation configuration consists of randomly located Frank-Read
Plastic deformation regime
Elastic-plastic transition
Findings
Discussion and Conclusions

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