Discrete Element Modeling of Brittle Crack Roughness in Three Dimensions

Crack morphology obtained in the fracture of materials with a disordered micro-structure is studied using numericalsimulations. Physical properties are embedded on a regular three dimensional lattice as discrete stochastic elements which conform to the laws of linear elasticity. In this model, also...

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Main Authors: Bjørn eSkjetne, Alex eHansen, Torbjørn eHelle
Format: Article
Language:English
Published: Frontiers Media S.A. 2014-11-01
Series:Frontiers in Physics
Subjects:
Online Access:http://journal.frontiersin.org/Journal/10.3389/fphy.2014.00068/full
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spelling doaj-fe42450382e9481b82e45b2c28988da22020-11-25T01:01:51ZengFrontiers Media S.A.Frontiers in Physics2296-424X2014-11-01210.3389/fphy.2014.00068107380Discrete Element Modeling of Brittle Crack Roughness in Three DimensionsBjørn eSkjetne0Alex eHansen1Torbjørn eHelle2NTNUNTNUNTNUCrack morphology obtained in the fracture of materials with a disordered micro-structure is studied using numericalsimulations. Physical properties are embedded on a regular three dimensional lattice as discrete stochastic elements which conform to the laws of linear elasticity. In this model, also known as the beam lattice, these elements are analogous to beams in that relative displacements between neighbouring nodes induce axial, bending and shearing forces, as in a real elastic solid. The stochastic nature enters via the introduction of random breaking thresholds on the individual elements. Using this model, the exponent characterizing the scaling with system size of the crack roughness perpendicular to the fracture plane is reported. Two different types of disorder have been used to generate the thresholds, i.e., distributions with a tail towardsstrong elements or with a tail towards weak elements. At weak disorders the self-affine regime seems to lie beyond thesystem sizes presently included. At stronger disorders a self-affine regime appears, for which we obtain exponents consistent with 0.6 for both types of disorder. The latter result is in fair agreement with the experimental value reported for large length scales, 0.50.http://journal.frontiersin.org/Journal/10.3389/fphy.2014.00068/fulldisorderFracturescaling lawsdiscrete element modelstochastic mediabeam model
collection DOAJ
language English
format Article
sources DOAJ
author Bjørn eSkjetne
Alex eHansen
Torbjørn eHelle
spellingShingle Bjørn eSkjetne
Alex eHansen
Torbjørn eHelle
Discrete Element Modeling of Brittle Crack Roughness in Three Dimensions
Frontiers in Physics
disorder
Fracture
scaling laws
discrete element model
stochastic media
beam model
author_facet Bjørn eSkjetne
Alex eHansen
Torbjørn eHelle
author_sort Bjørn eSkjetne
title Discrete Element Modeling of Brittle Crack Roughness in Three Dimensions
title_short Discrete Element Modeling of Brittle Crack Roughness in Three Dimensions
title_full Discrete Element Modeling of Brittle Crack Roughness in Three Dimensions
title_fullStr Discrete Element Modeling of Brittle Crack Roughness in Three Dimensions
title_full_unstemmed Discrete Element Modeling of Brittle Crack Roughness in Three Dimensions
title_sort discrete element modeling of brittle crack roughness in three dimensions
publisher Frontiers Media S.A.
series Frontiers in Physics
issn 2296-424X
publishDate 2014-11-01
description Crack morphology obtained in the fracture of materials with a disordered micro-structure is studied using numericalsimulations. Physical properties are embedded on a regular three dimensional lattice as discrete stochastic elements which conform to the laws of linear elasticity. In this model, also known as the beam lattice, these elements are analogous to beams in that relative displacements between neighbouring nodes induce axial, bending and shearing forces, as in a real elastic solid. The stochastic nature enters via the introduction of random breaking thresholds on the individual elements. Using this model, the exponent characterizing the scaling with system size of the crack roughness perpendicular to the fracture plane is reported. Two different types of disorder have been used to generate the thresholds, i.e., distributions with a tail towardsstrong elements or with a tail towards weak elements. At weak disorders the self-affine regime seems to lie beyond thesystem sizes presently included. At stronger disorders a self-affine regime appears, for which we obtain exponents consistent with 0.6 for both types of disorder. The latter result is in fair agreement with the experimental value reported for large length scales, 0.50.
topic disorder
Fracture
scaling laws
discrete element model
stochastic media
beam model
url http://journal.frontiersin.org/Journal/10.3389/fphy.2014.00068/full
work_keys_str_mv AT bjørneskjetne discreteelementmodelingofbrittlecrackroughnessinthreedimensions
AT alexehansen discreteelementmodelingofbrittlecrackroughnessinthreedimensions
AT torbjørnehelle discreteelementmodelingofbrittlecrackroughnessinthreedimensions
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