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Diffuse-interface polycrystal plasticity: Expressing grain boundaries as geometrically necessary dislocations

机译:扩散界面多晶塑性:表示晶界为   几何必要的位错

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摘要

The standard way of modeling plasticity in polycrystals is by using thecrystal plasticity model for single crystals in each grain, and imposingsuitable traction and slip boundary conditions across grain boundaries. In thisfashion, the system is modeled as a collection of boundary-value problems withmatching boundary conditions. In this paper, we develop a diffuse-interfacecrystal plasticity model for polycrystalline materials that results in a singleboundary-value problem with a single crystal as the reference configuration.Using a multiplicative decomposition of the deformation gradient into latticeand plastic parts, i.e. F(X,t) = F^L(X,t) F^P(X,t), an initial stress-freepolycrystal is constructed by imposing F^L to be a piecewise constant rotationfield R^0(X), and F^P = R^0(X)^T, thereby having F(X,0) = I, and zero elasticstrain. This model serves as a precursor to higher order crystal plasticitymodels with grain boundary energy and evolution.
机译:在多晶体中建模可塑性的标准方法是对每个晶粒中的单晶使用晶体可塑性模型,并在晶粒边界上施加适当的牵引力和滑移边界条件。在这种情况下,系统被建模为具有匹配边界条件的边界值问题的集合。在本文中,我们开发了一种多晶材料的扩散界面晶体可塑性模型,该模型会导致以单晶为参考构型的单边界值问题。使用变形梯度的乘法分解成晶格和塑性零件,即F(X, t)= F ^ L(X,t)F ^ P(X,t),通过将F ^ L设为分段恒定旋转场R ^ 0(X)来构造初始无应力多晶,并且F ^ P = R ^ 0(X)^ T,从而使F(X,0)= I,并且弹性应变为零。该模型是具有晶界能和演化的高阶晶体可塑性模型的先驱。

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