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具有强非均匀性的纤维束中的脆韧转变。

Brittle-to-ductile transition in a fiber bundle with strong heterogeneity.

作者信息

Kovács Kornél, Hidalgo Raul Cruz, Pagonabarraga Ignacio, Kun Ferenc

机构信息

Department of Theoretical Physics, University of Debrecen, P. O. Box: 5, H-4010 Debrecen, Hungary.

出版信息

Phys Rev E Stat Nonlin Soft Matter Phys. 2013 Apr;87(4):042816. doi: 10.1103/PhysRevE.87.042816. Epub 2013 Apr 29.

DOI:10.1103/PhysRevE.87.042816
PMID:23679482
Abstract

We analyze the failure process of a two-component system with widely different fracture strength in the framework of a fiber bundle model with localized load sharing. A fraction 0≤α≤1 of the bundle is strong and it is represented by unbreakable fibers, while fibers of the weak component have randomly distributed failure strength. Computer simulations revealed that there exists a critical composition α(c) which separates two qualitatively different behaviors: Below the critical point, the failure of the bundle is brittle, characterized by an abrupt damage growth within the breakable part of the system. Above α(c), however, the macroscopic response becomes ductile, providing stability during the entire breaking process. The transition occurs at an astonishingly low fraction of strong fibers which can have importance for applications. We show that in the ductile phase, the size distribution of breaking bursts has a power law functional form with an exponent μ=2 followed by an exponential cutoff. In the brittle phase, the power law also prevails but with a higher exponent μ=9/2. The transition between the two phases shows analogies to continuous phase transitions. Analyzing the microstructure of the damage, it was found that at the beginning of the fracture process cracks nucleate randomly, while later on growth and coalescence of cracks dominate, which give rise to power law distributed crack sizes.

摘要

我们在具有局部载荷分担的纤维束模型框架内,分析了具有截然不同断裂强度的双组分系统的失效过程。纤维束中有0≤α≤1的部分是强的,由不可断裂的纤维表示,而弱组分的纤维具有随机分布的失效强度。计算机模拟表明,存在一个临界组成α(c),它将两种定性不同的行为区分开来:在临界点以下,纤维束的失效是脆性的,其特征是系统可断裂部分内的损伤突然增长。然而,在α(c)以上,宏观响应变得具有韧性,在整个断裂过程中提供稳定性。这种转变发生在强纤维的比例低得出奇的情况下,这可能对应用具有重要意义。我们表明,在韧性阶段,断裂突发的尺寸分布具有幂律函数形式,指数μ = 2,随后是指数截断。在脆性阶段,幂律也占主导地位,但指数更高,μ = 9/2。两个阶段之间的转变显示出与连续相变的相似性。通过分析损伤的微观结构发现,在断裂过程开始时,裂纹随机形核,而在后期,裂纹的扩展和合并占主导地位,这导致了裂纹尺寸的幂律分布。

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