2018
DOI: 10.1103/physreve.98.032117
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Mesoscopic description of the equal-load-sharing fiber bundle model

Abstract: One aim of the equal load sharing fiber bundle model is to describe the critical behavior of failure events. One way of accomplishing this, is through a discrete recursive dynamics. We introduce a continuous mesoscopic equation catching the critical behavior found through recursive dynamics. It allows us to link the model with the unifying framework of absorbing phase transitions traditionally used in the study of non-equilibrium phase transitions. Moreover, it highlights the analogy between equal load sharing… Show more

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Cited by 3 publications
(3 citation statements)
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References 21 publications
(47 reference statements)
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“…Analytically known that in the mean-field limit this kind of hybrid phase transition happens, e.g. power law behavior of damage is obtained when approaching the critical load of global failure d c − d ∝ (σ c − σ ) 1/2 (see 47,48 ). This permits to have non-diverging cluster sizes at the LLS to ELS transition point, smaller than the typical distance of WS: ξ = 1/(2p) 1/2 (see 44 ).…”
Section: Discussionmentioning
confidence: 99%
“…Analytically known that in the mean-field limit this kind of hybrid phase transition happens, e.g. power law behavior of damage is obtained when approaching the critical load of global failure d c − d ∝ (σ c − σ ) 1/2 (see 47,48 ). This permits to have non-diverging cluster sizes at the LLS to ELS transition point, smaller than the typical distance of WS: ξ = 1/(2p) 1/2 (see 44 ).…”
Section: Discussionmentioning
confidence: 99%
“…One such step was done in Ref. [45] by writing down a mesoscopic description of the ELS-FBM. By specifically, writing the time evolution of the order parameter n(σ) − n c η and the driving field (stress increase) as J σ c − σ, the dynamics is described by…”
Section: Some Related Work On the Dynamics Of Fbmmentioning
confidence: 99%
“…One such step was done in Ref. [43] by writing down a mesoscopic description of the ELS-FBM. specifically, writing the time evolution of the order parameter n(σ) − n c = η and the driving field (stress increase) as J = σ c − σ, the dynamics is described by…”
Section: Some Related Work On the Dynamics Of Fbmmentioning
confidence: 99%