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猝灭无序和不稳定性控制三维动态断裂。

Quenched disorder and instability control dynamic fracture in three dimensions.

作者信息

Lubomirsky Yuri, Bouchbinder Eran

机构信息

Chemical and Biological Physics Department, Weizmann Institute of Science, Rehovot, 7610001, Israel.

出版信息

Nat Commun. 2024 Aug 29;15(1):7494. doi: 10.1038/s41467-024-51573-6.

DOI:10.1038/s41467-024-51573-6
PMID:39209817
原文链接:https://pmc.ncbi.nlm.nih.gov/articles/PMC11362301/
Abstract

Materials failure in 3D still poses basic challenges. We study 3D brittle crack dynamics using a phase-field approach, where Gaussian quenched disorder in the fracture energy is incorporated. Disorder is characterized by a correlation length R and strength σ. We find that the mean crack velocity v is bounded by a limiting velocity, which is smaller than the homogeneous material's prediction and decreases with σ. It emerges from a dynamic renormalization of the fracture energy with increasing crack driving force G, resembling a critical point, due to an interplay between a 2D branching instability and disorder. At small G, the probability of localized branching on a scale R is super-exponentially small. With increasing G, this probability quickly increases, leading to misty fracture surfaces, yet the associated extra dissipation remains small. As G is further increased, branching-related lengthscales become dynamic and persistently increase, leading to hackle-like structures and a macroscopic contribution to the fracture surface. The latter dynamically renormalizes the actual fracture energy until, eventually, any increase in G is balanced by extra fracture surface, with no accompanying increase in v. Finally, branching width reaches the system's thickness such that 2D symmetry is statistically restored. Our findings are consistent with a broad range of experimental observations.

摘要

三维材料失效仍然面临着基本挑战。我们使用相场方法研究三维脆性裂纹动力学,其中引入了断裂能中的高斯淬火无序。无序由相关长度R和强度σ表征。我们发现平均裂纹速度v受限于一个极限速度,该极限速度小于均匀材料的预测值,且随σ减小。它源于随着裂纹驱动力G增加,断裂能的动态重整化,类似于一个临界点,这是由于二维分支不稳定性和无序之间的相互作用。在小G时,尺度为R的局部分支概率超指数级小。随着G增加,该概率迅速增大,导致断裂表面模糊,但相关的额外耗散仍然很小。随着G进一步增加,与分支相关的长度尺度变得动态且持续增加,导致出现类似毛边的结构,并对断裂表面有宏观贡献。后者动态重整实际断裂能,直到最终,G的任何增加都由额外的断裂表面平衡,而v没有随之增加。最后,分支宽度达到系统厚度,使得二维对称性在统计上得以恢复。我们的发现与广泛的实验观察结果一致。

https://cdn.ncbi.nlm.nih.gov/pmc/blobs/24bc/11362301/3faf96cfba27/41467_2024_51573_Fig7_HTML.jpg
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https://cdn.ncbi.nlm.nih.gov/pmc/blobs/24bc/11362301/299b90d8e7ff/41467_2024_51573_Fig4_HTML.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/24bc/11362301/9902957578b8/41467_2024_51573_Fig5_HTML.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/24bc/11362301/28f833ba7db0/41467_2024_51573_Fig6_HTML.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/24bc/11362301/3faf96cfba27/41467_2024_51573_Fig7_HTML.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/24bc/11362301/99c199193483/41467_2024_51573_Fig1_HTML.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/24bc/11362301/333ed23f4255/41467_2024_51573_Fig2_HTML.jpg
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https://cdn.ncbi.nlm.nih.gov/pmc/blobs/24bc/11362301/9902957578b8/41467_2024_51573_Fig5_HTML.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/24bc/11362301/28f833ba7db0/41467_2024_51573_Fig6_HTML.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/24bc/11362301/3faf96cfba27/41467_2024_51573_Fig7_HTML.jpg

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本文引用的文献

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Dynamics of crack front waves in three-dimensional material failure.三维材料破坏中裂纹前沿波的动力学
Phys Rev E. 2023 Oct;108(4):L043002. doi: 10.1103/PhysRevE.108.L043002.
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Dynamic Crack-Front Deformations in Cohesive Materials.内聚材料中的动态裂纹前沿变形
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