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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2014-11-01
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Online Access: | http://journal.frontiersin.org/Journal/10.3389/fphy.2014.00068/full |
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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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