Abstract

The use of Nye's dislocation tensor for calculating the density of geometrically necessary dislocations (GND) is widely adopted in the study of plastically deformed materials. The “curl” operation involved in finding the Nye tensor, while conceptually straightforward has been marred with inconsistencies and several different definitions are in use. For the three most common definitions, we show that their consistent application leads to the same result. To eliminate frequently encountered confusion, a summary of expressions for Nye's tensor in terms of elastic and plastic deformation gradient, and for both small and large deformations, is presented. A further question when estimating GND density concerns the optimization technique used to solve the under-determined set of equations linking Nye's tensor and GND density. A systematic comparison of the densities obtained by two widely used techniques, L1 and L2 minimisation, shows that both methods yield remarkably similar total GND densities. Thus the mathematically simpler, L2, may be preferred over L1 except when information about the distribution of densities on specific slip systems is required. To illustrate this, we compare experimentally measured lattice distortions beneath nano-indents in pure tungsten, probed using 3D-resolved synchrotron X-ray micro-diffraction, with those predicted by 3D strain-gradient crystal plasticity finite element calculations. The results are in good agreement and show that the volumetric component of the elastic strain field has a surprisingly small effect on the determined Nye tensor. This is important for experimental techniques, such as micro-beam Laue measurements and HR-EBSD, where only the deviatoric strain component is measured.

Highlights

  • Before the development of crystal plasticity finite element formulations, phenomenological continuum models were used to describe plastic deformation in materials

  • Crystal plasticity finite element (CPFE) formulations address this issue by explicitly modelling plasticity in terms of crystallographic slip at the grain scale (Roters et al, 2010)

  • For example CPFE has been used to simulate the development of microstructures and the consequent effect on the macroscopic material response (Aifantis, 1984), to simulate surface roughening in thin film mechanics problems (Raabe et al, 2003), grain-boundary and interface mechanics (Bate and Hutchinson, 2005; Meissonnier et al, 2001), strain-gradient effects (Dunne et al, 2012, 2007), polycrystalline morphology and texture, the necessary conditions for crack nucleation (Chen et al, 2017), geometrically necessary dislocations (GNDs) (Dahlberg et al, 2014), creep and high temperature deformation (Balasubramanian and Anand, 2002), texture formation (Asaro and Rice, 1977), deformation twinning (Kalidindi, 1998), multiphase mechanics (Vogler and Clayton, 2008) etcetera

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Summary

Introduction

Before the development of crystal plasticity finite element formulations, phenomenological continuum models were used to describe plastic deformation in materials. Without delving into the underlying microstructural processes, these approaches, calibrated by experiments, could capture plasticity at the macroscopic scale (Dunne and Petrinic, 2004; Khan, Akhtar.S, 1995). Crystal plasticity finite element (CPFE) formulations address this issue by explicitly modelling plasticity in terms of crystallographic slip at the grain scale (Roters et al, 2010). Popularity of these formulations has increased dramatically as they directly account for complex interactions between individual grains of polycrystals and the resulting locally heterogeneous loading. CPFE has been used with other modelling techniques such as continuum dislocation dynamics, and nonlinear thermoelasticity to simulate the response of materials under extreme dynamic loading (Luscher et al, 2016)

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