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首页> 外文期刊>Physical review. B, Condensed Matter And Materals Physics >Shock waves in complex binary solids: Cubic Laves crystals, quasicrystals, and amorphous solids
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Shock waves in complex binary solids: Cubic Laves crystals, quasicrystals, and amorphous solids

机译:复杂的二元固体中的冲击波:立方拉夫晶体,准晶体和无定形固体

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Shock waves have been simulated by molecular dynamics in the cubic Laves phase C15, in related Frank-Kasper-type (AlCu)Li quasicrystals, and in an amorphous solid of the same composition and potential parameters. The goal of this study was to generate shock waves in periodic and aperiodic structures and to compare their behavior. The expectation was that new types of defects would show up in aperiodic materials. Three regimes are observed in the Laves phase: at low shock wave intensity the system reacts elastically, at high intensities it turns disordered. In the intermediate region the velocity of the elastic wave saturates and an additional plastic wave appears. Extended defects are created which form a network of walls of finite width. The crystallites in between are rotated by the shock wave. If the samples are quenched a polycrystalline phase is obtained. The size of the grains decreases with increasing shock wave intensity until complete fragmentation occurs in the third regime. The behavior of the quasicrystal models is similar, except that there is a continuous transition from a quasielastic behavior to the plastic regime. Ring processes are observed which break up into open paths when the shock wave energy grows. The transition to a complete destruction of the structure is continuous. In the amorphous solid a linear u_s-u_p relation is found over the whole range of piston velocities. Two regimes are present, with unsteady plastic waves at weak shock strengths and steady waves in the range coinciding with the upper regime in the ordered structures.
机译:冲击波已经通过分子动力学在立方Laves相C15中,在相关的Frank-Kasper型(AlCu)Li准晶体中以及在具有相同组成和潜在参数的非晶态固体中进行了模拟。这项研究的目的是在周期性和非周期性结构中产生冲击波,并比较它们的行为。人们期望在非周期性材料中会出现新型缺陷。在拉夫斯相中观察到三种状态:在低冲击波强度下,系统发生弹性反应,在高强度下,系统变得无序。在中间区域,弹性波的速度达到饱和,并出现另一个塑性波。产生了扩展的缺陷,这些缺陷形成了有限宽度的壁网。两者之间的微晶被冲击波旋转。如果将样品淬火,则获得多晶相。晶粒尺寸随着冲击波强度的增加而减小,直到在第三种状态下发生完全破碎为止。准晶体模型的行为类似,除了从准弹性行为到塑性状态的连续过渡之外。观察到环形过程,当冲击波能量增加时,该过程分解为开放路径。向结构的完全破坏的过渡是连续的。在非晶态固体中,在整个活塞速度范围内都存在线性u_s-u_p关系。存在两种状态,在弱冲击强度下具有不稳定的塑性波,而在有序结构中,稳定波的范围与上部状态一致。

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