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首页> 外文期刊>International Journal of Plasticity >Interaction of dislocation with GP zones or theta '' phase precipitates in aluminum: Atomistic simulations and dislocation dynamics
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Interaction of dislocation with GP zones or theta '' phase precipitates in aluminum: Atomistic simulations and dislocation dynamics

机译:磷酸中脱位与GP区或θ的相互作用铝:原子模拟和错位动力学

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摘要

We investigate the interaction of edge dislocation in aluminum matrix with GP zones and theta '' phase with molecular dynamics (MD) simulations. All these copper-containing precipitates have a form of single or multilayer parallel copper disks separated by planes of aluminum atoms. The maximal number of copper layers of theta '' phase considered in the present work is equal to six; the diameter of precipitates varies from 3 to 15 nm. It is shown that all types of precipitates are initially overcome by dislocation with formation of the Orowan loop around them. The most fragile precipitate is GP zone of first type with a 3 nm diameter; it is sheared during the first closure of the Orowan loop by magnitude of leading partial dislocation, and obtains an additional displacement of trailing partial after the dislocation detachment. The remaining inclusions, even GP zones of a larger diameter, demonstrate the process of accumulation of surface deformation over time due to the shift of the upper half of the copper atom disks relative to the lower one. The moments of separation of the shifted halves are determined for different types of inclusion. Cutting of the strongest six-layer theta '' phase is not observed during our MD simulations. The evolution of local stress acting on copper atoms is traced over the several interactions required for the complete shearing of obstacle. The maximal local stress reached during deformation of GP of the first type of the smallest size is equal to 1.5 GPa, while the substantial increase in acting local stress is registered for higher number of copper disks. The local stress of 5.7 GPa is observed during the sequential interactions of dislocation with six-layer theta '' phase. The entire MD system demonstrate analogical growth of the average level of acting stress simultaneously with the increase in local stress on inclusion; it varies from about 125 MPa in the case of smallest GP zone to about 670 MPa for the hardest theta '' phase. The MD data is generalized in the form of the model of dislocation dynamics at interaction with precipitate. The model was previously proposed by Krasnikov and Mayer (2019) for the case of theta' phase in aluminum. In the present work, it is modified by accounting the change in the energy of the dislocation core during contact with different types of inclusions. The energy values are fitted from a comparison of the time dependences of average stress in system with MD data. Variation of the core energy for the dislocation line segments attached to precipitate allows us to take into account specific features of precipitates with different number of layers.
机译:我们研究了与GP区与GP区和分子动力学(MD)模拟的铝基矩阵中边缘位错的相互作用。所有这些含铜沉淀物具有由铝原子的平面分离的单层或多层平行铜盘形式。在本工作中考虑的θ“相位的铜层的最大数量等于六个;沉淀物的直径从3至15nm变化。结果表明,所有类型的沉淀物最初通过与周围的orowan环的形成脱位来克服。最脆弱的沉淀物是第一类型的GP区域,直径为3nm;在orowan环路的第一次封闭期间通过前导部分位错的幅度封闭,并且在错位脱落之后获得尾随部分的额外位移的剪切。剩余的夹杂物,即使是较大直径的GP区域,也表明了由于铜原子盘相对于下部的上半部分的偏移而随着时间的推移累积表面变形的过程。确定移位半部的分离的瞬间用于不同类型的包容性。在我们的MD模拟期间未观察到最强的六层θ'阶段。作用在铜原子上的局部应力的演变在完全剪切障碍物所需的几个相互作用上进行跟踪。在第一类型最小尺寸的GP变形期间达到的最大局部应力等于1.5GPa,而作用局部应力的显着增加是为较高数量的铜盘登记。在六层θ“相位的顺序相互作用期间观察到5.7GPa的局部应力。整个MD系统表明了随着局部应力的增加,表明了动作应力的平均水平的模拟生长;在最小的GP区域到大约670 MPa的情况下,它因最小的THETA阶段而异。 MD数据以与沉淀物相互作用的位错动态模型的形式广泛化。先前由Krasnikov和Mayer(2019)提出的模型,以便在铝中的θ相。在本作工作中,通过在与不同类型的夹杂物联系期间考虑位错核心的能量的变化来修改它。能量值拟合与MD数据系统平均压力的时间依赖性的比较。附着于沉淀物的位错线段的核心能量的变化使我们能够考虑具有不同数量的层的沉淀物的具体特征。

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