2021
DOI: 10.3389/fphy.2021.752086
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From Nucleation to Percolation: The Effect of System Size when Disorder and Stress Localization Compete

Abstract: A phase diagram for a one-dimensional fiber bundle model is constructed with a continuous variation in two parameters guiding the dynamics of the model: strength of disorder and range of stress relaxation. When the range of stress relaxation is very low, the stress concentration plays a prominent role and the failure process is nucleating where a single crack propagates from a particular nucleus with a very high spatial correlation unless the disorder strength is high. On the other hand, a high range of stress… Show more

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Cited by 2 publications
(2 citation statements)
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“…The critical range that separates these two limits has been studied elsewhere [17,18]. The underlying mechanism is not only valid for the fiber bundle model [17][18][19][20] but also seen in the random fuse model [32,33] and in molecular dynamics simulations [34]. The present study is a manifestation of these two competing effects.…”
Section: Discussionmentioning
confidence: 54%
See 1 more Smart Citation
“…The critical range that separates these two limits has been studied elsewhere [17,18]. The underlying mechanism is not only valid for the fiber bundle model [17][18][19][20] but also seen in the random fuse model [32,33] and in molecular dynamics simulations [34]. The present study is a manifestation of these two competing effects.…”
Section: Discussionmentioning
confidence: 54%
“…In the fiber bundle model, the mode of failure depends mainly on two factors: the strength of disorder in the individual failure threshold of the fibers and the range of stress release [15][16][17][18] when one such fiber is broken. Such interplay between disorder and damage nucleation not only affects the failure mode but also influences the spatial correlation during the failure process [17][18][19][20]. The range of stress release has two extreme limits, viz.…”
Section: Introductionmentioning
confidence: 99%