1996
DOI: 10.1103/physrevb.54.15094
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Fracture of disordered three-dimensional spring networks: A computer simulation methodology

Abstract: In this paper a computational technique is proposed to describe brittle fracture of highly porous random media. Geometrical heterogeneity in the ''open cell foam'' structure of the porous medium on a mesoscopic length scale ͑ϳ100 nm͒ is mapped directly onto a three-dimensional ͑3D͒ elastic network by using molecular dynamics techniques to generate starting configurations. The aspects in our description are that the elastic properties of an irregular 3D-network are described using not only a potential with a tw… Show more

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Cited by 28 publications
(25 citation statements)
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“…1) suggest that disordered elastic networks [15] may be used to model TAs. Our initial studies were conducted on a square network of linear springs.…”
mentioning
confidence: 99%
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“…1) suggest that disordered elastic networks [15] may be used to model TAs. Our initial studies were conducted on a square network of linear springs.…”
mentioning
confidence: 99%
“…Externally imposed deviations increased the potential energy of the network via a combination of elastic [ contributions. Here Dl and Du are changes in the length of a spring and the bond angle between adjacent springs, respectively [15]. The differences between trabeculae are modeled by assigning random values for k and…”
mentioning
confidence: 99%
“…In Ref. [8], it was proposed that a system to model mechanical properties of a TA can be obtained by adapting a disordered network of fragile elastic elements [9]. The model system includes potential energy contributions from elasticity and from changes in bond angles between adjacent springs.…”
mentioning
confidence: 99%
“…Within the past decade many papers have been published on the subject of the simulation of brittle 1 fracture. A commonly used approach in these papers is the lattice model (Arabi [1], Chung [3], Donze [4]). This method models objects as a lattice of points or pointmasses connected by stiff springs.…”
Section: Introductionmentioning
confidence: 99%
“…(Even with the use of implicit integration methods, the simulation of a lattice of stiff springs entails a computational cost as least equal to that of Lagrange multipliers.) For example, in Chung [3], the simulation of an object with 2701 lattice-links is done in 137 time-steps, each taking 86 seconds on a 75MHz MIPS R8000, for a total of three and a half hours. A comparable simulation with our method on the same hardware would take roughly five and a half 1 The term "brittle," as used in materials science literature (and in this paper) means that the substance does not undergo significant plastic (reversible) deformation before breaking [2].…”
Section: Introductionmentioning
confidence: 99%