Geometric micromechanical modeling of structure changes, fracture and grain boundary layers in polycrystals

J. Clayton, J. Knap
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引用次数: 11

Abstract

A constitutive framework based on concepts from phase field theory and pseudo-Finsler geometry is exercised in numerical simulations of deformation and fracture of ceramic polycrystals. The material system of interest is boron carbide, a hard but brittle ceramic. Some microstructures are enabled with thin layers of a secondary amorphous phase of boron nitride between grains of boron carbide. The constitutive theory accounts for physical mechanisms of twinning, crystal-to-glass phase transformations, cleavage fracture within grains and separation and cavitation at grain boundaries (GBs). According to the generalized Finsler approach, geometric quantities such as the metric tensor and connection coefficients can depend on one or more director vectors, also called internal state vectors, that enter the energy potential in a manner similar to order parameters of phase field models. A partially linearized version of the theory is invoked in finite element simulations of polycrystals, with and without GB layers, subjected to pure shear loading. Effects of grain size and layer properties — thickness, shear modulus and surface energy — are studied parametrically. Results demonstrate that twinning and amorphization occur prominently in nanocrystals but less so in aggregates with larger grains that tend to fail earlier by fracture. Structural changes occur readily in the latter at smaller applied strains only in conjunction with elastic shear softening in localized degraded or damaged regions. Hall–Petch scaling of peak shear strength with grain size is observed. Strength is increased via addition of amorphous layers that shift the failure mode from transgranular to intergranular and further by cavity expansion in layers that induces local elastic compression and suppresses crack extension. Stiff layers provide the largest peak strength enhancement, while elastically compliant layers may improve toughness and strength in the softening regime.
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多晶体结构变化、断裂和晶界层的几何微观力学建模
基于相场理论和伪芬斯勒几何概念的本构框架用于陶瓷多晶体变形和断裂的数值模拟。感兴趣的材料体系是碳化硼,一种坚硬但易碎的陶瓷。一些微结构是通过碳化硼晶粒之间的氮化硼的第二非晶相薄层实现的。本构理论解释了孪晶、晶体到玻璃的相变、晶粒内的解理断裂以及晶界处的分离和空化(GBs)的物理机制。根据广义Finsler方法,度量张量和连接系数等几何量可以取决于一个或多个指向矢,也称为内部状态向量,它们以类似于相场模型的阶参数的方式进入能量势。在有和没有GB层的多晶体在纯剪切载荷下的有限元模拟中,引用了该理论的部分线性化版本。参数化研究了晶粒尺寸和层性质——厚度、剪切模量和表面能——的影响。结果表明,孪晶和非晶化在纳米晶体中显著发生,但在晶粒较大的聚集体中较少发生,这些聚集体往往会更早地因断裂而失效。后者在较小的施加应变下很容易发生结构变化,只有在局部退化或损坏区域发生弹性剪切软化。观察到峰值剪切强度随晶粒尺寸的Hall–Petch标度。通过添加非晶层(将失效模式从穿晶转变为晶间),以及通过层中的空腔膨胀(诱导局部弹性压缩并抑制裂纹扩展),强度得以提高。刚性层提供最大的峰值强度增强,而弹性柔顺层可以提高软化状态下的韧性和强度。
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来源期刊
Journal of Micromechanics and Molecular Physics
Journal of Micromechanics and Molecular Physics Materials Science-Polymers and Plastics
CiteScore
3.30
自引率
0.00%
发文量
27
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