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首页> 外文期刊>The Journal of Chemical Physics >Local and bulk melting of shocked columnar nanocrystalline Cu: Dynamics, anisotropy, premelting, superheating, supercooling, and re-crystallization
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Local and bulk melting of shocked columnar nanocrystalline Cu: Dynamics, anisotropy, premelting, superheating, supercooling, and re-crystallization

机译:冲击圆柱状纳米晶Cu的局部和整体熔化:动力学,各向异性,预熔化,过热,过冷和重结晶

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We perform large-scale molecular dynamics simulations to study shock-induced melting transition of idealized hexagonal columnar nanocrystalline Cu. The as-constructed nanocrystalline Cu consists of unrotated (reference) and rotated columnar crystals, relative to the columnar axis. Shock loading is applied along three principal directions of the columnar Cu: two transverse (zigzag and armchair) and one longitudinal directions. Dynamic local melting processes are highly anisotropic with respect to the shock directions. For the transverse directions, hotspot effect and disparate dynamic responses of grains with different orientations may lead to partial or complete premelting of the initially rotated grains, which in turn leads to transient supercooling and heterogeneous recrystallization, and thus, the formation of nanocrystalline solids with modified grain structures or solid-liquid mixtures, depending on the extent of supercooling. With increasing shock strengths, the reference grains melt heterogeneously at interfaces and homogeneously inside. Conversely, "bulk" premelting of the rotated grains is absent for the longitudinal direction, except for grain boundary melting. The progression of recrystallization or heterogenous melting diminishes and eventually eliminates the transient premelting or superheating of the system via latent heat and thermal diffusion. Premelting or superheating appears unlikely for bulk melting or well-defined Hugoniot states, if the thermal and mechanical equilibria are achieved, and the thermodynamic melting curve coincides with the partial melting Hugoniot states of a polycrystalline solid.
机译:我们执行大规模的分子动力学模拟,以研究理想六角形圆柱状纳米晶Cu的激振诱导的熔化转变。如此构造的纳米晶Cu相对于柱状轴由未旋转(参考)和旋转的柱状晶体组成。沿圆柱状Cu的三个主要方向施加冲击载荷:两个横向方向(曲折和扶手椅)和一个纵向方向。动态局部熔化过程相对于冲击方向是高度各向异性的。对于横向方向,具有不同方向的晶粒的热点效应和不同的动态响应可能会导致初始旋转的晶粒部分或完全预熔融,进而导致瞬态过冷和异质重结晶,从而形成改性纳米颗粒晶粒结构或固液混合物,取决于过冷程度。随着冲击强度的增加,参考晶粒在界面处异质熔化,并在内部均匀熔化。相反,除了晶粒边界熔化之外,在纵向方向上不存在对旋转晶粒的“批量”预熔化。重结晶或非均相熔化的进程会减少,并最终通过潜热和热扩散消除了系统的瞬态预熔化或过热。如果实现了热和机械平衡,并且预热或过热对于本体熔融或明确定义的Hugoniot状态似乎不太可能,并且热力学熔融曲线与多晶固体的部分熔融Hugoniot状态重合。

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