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首页> 外文期刊>Scientific reports. >Acoustic Emission from Porous Collapse and Moving Dislocations in Granular Mg-Ho Alloys under Compression and Tension
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Acoustic Emission from Porous Collapse and Moving Dislocations in Granular Mg-Ho Alloys under Compression and Tension

机译:压缩和拉伸状态下粒状Mg-Ho合金多孔塌陷和运动位错的声发射

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摘要

We identified heterogeneous Mg-Ho alloys as an ideal material to measure the most extensive acoustic emission spectra available. Mg-Ho alloys are porous and show a high density of dislocations, which slide under external tension and compression. These dislocations nucleate near numerous heterogeneities. Two mechanisms compete under external forcing in the structural collapse, namely collapsing holes and the movements of dislocations. Their respective fingerprints in acoustic emission (AE) measurements are very different and relate to their individual signal strengths. Porous collapse generates very strong AE signals while dislocation movements create more but weaker AE signals. This allows the separation of the two processes even though they almost always coincide temporarily. The porous collapse follows approximately mean-field behavior (ε?=?1.4, τ’?=?1.82, α?=?2.56, x?=?1.93, χ?=?1.95) with mean field scaling fulfilled. The exponents for dislocation movement are greater (ε?=?1.92, τ’?=?2.44, α?=?3.0, x?=?1.7, χ?=?1.42) and follows approximately the force integrated mean-field predictions. The Omori scaling is similar for both mechanisms. The Bath’s law is well fulfilled for the porous collapse but not for the dislocation movements. We suggest that such ‘complex’ mixing behavior is dominant in many other complex materials such as (multi-) ferroics, entropic alloys and porous ferroelastics, and, potentially, homogeneous materials with the simultaneous appearance of different collapse mechanisms.
机译:我们将异质Mg-Ho合金确定为测量最广泛的声发射光谱的理想材料。 Mg-Ho合金是多孔的,位错密度高,在外部张力和压缩作用下会滑动。这些位错在许多异质性附近成核。在外力作用下结构坍塌有两种机制,即孔洞塌陷和位错运动。它们在声发射(AE)测量中的各自指纹非常不同,并且与它们各自的信号强度有关。多孔塌陷产生非常强的AE信号,而位错运动产生更多但较弱的AE信号。即使两个过程几乎总是暂时重合,也可以将这两个过程分开。多孔塌陷遵循近似的平均场行为(ε= 1.4,τ′= 1.82,α= 2.56,x = 1.93,χ= 1.95),并且满足平均场比例。位错运动的指数更大(ε?=?1.92,τ'?=?2.44,α?=?3.0,x?=?1.7,χ?=?1.42),并且近似遵循力积分平均场的预测。这两种机制的Omori缩放比例相似。巴斯的定律很好地满足了多孔塌陷,但不适用于错位运动。我们建议这种“复杂”的混合行为在许多其他复杂的材料中占主导地位,例如(多)铁磁性材料,熵合金和多孔铁弹性体,以及可能同时出现不同塌陷机理的均质材料。

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