A scale transition plasticity theory - from crystal to continuum
Citation for published version (APA):Poh, L. H., Peerlings, R. H. J., & Geers, M. G. D. (2010). A scale transition plasticity theory - from crystal to continuum. Poster session presented at Mate Poster Award 2010 : 15th Annual Poster Contest.
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Mechanics of Materials
1.
Introduction
Gradient crystal plasticity models take into account the ad-ditional work done by the geometrically necessary disloca-tions (GNDs). However, these models are not efficient when solving for large problems. We developed an 1D continuum gradient plasticity model by homogenizing the (microscopic) work done in a single-slip crystal.
2.
Homogenization theory
Polycrystalline metals compose of grains separated by grain boundaries, with the interior of grains having similar struc-ture as that of a single crystal. In the continuum model, each macroscopic point represents the averaged response of a single crystal centered atx with micro-coordinates y, as depicted in Fig1.
Figure 1: Continuum model with unit cells of lengthL
The plastic slip within the crystal (γ) is decomposed into a slow-varying component (˜εp) and its gradient (∂ ˜ε∂xp) as well as a fluctuation functionf(y) and its amplitude g(x), shown schematically in Fig2.
γ(x + y) = ˜εp(x) +∂ ˜εp(x)
∂x y + g(x)f(y)
Figure 2: Decomposition of microscopic plastic slipγ
This expression forγ is substituted into the single crystal plasticity model by [1]. The continuum power expenditure is derived by homogenizing the microscopic free energy and dissipation. The homogenized micro-force balance is given by:
(Ga + 2μ)˜εp− (Gl2+μL2
2 )∇2˜εp= Gaεp
whereG is the shear modulus, a = kLl22 (k is a fluctuation
parameter),μ is the resistance modulus at grain boundaries andl is a length scale parameter. This expression has the same form as the "implicit" gradient formulation which is widely used in softening models [2].
3.
Influence of grain boundaries
The grain boundary resistance plays a major role in the ma-terial response. This is easily observed in an uniform defor-mation where the gradient term vanishes. The stress-strain graphs of a rigid plastic material for two extreme cases, the micro-free (μ → 0) and the micro-hard (μ → ∞) boundary conditions are shown in Fig3.
Figure 3: Stress-strain graphs (σ0= yield stress,H = hardening modulus)
References
[1] Cermelli, P., Gurtin, M. E., 2002. Geometrically nec-essary dislocations in viscoplastic single crystals and bicrystals undergoing small deformations. Int J Solid Struct 39, 6281-6309.
[2] Peerlings, R. H. J., De Borst, R., Brekelmans, W. A. M., De Vree, J. H. P., 1996. Gradient enhanced damage for quasi-brittle materials. Int J Numer Methods Eng 39, 3391-3403.