Dynamics of fractures in quenched disordered media

Guido Caldarelli, Raffaele Cafiero, and Andrea Gabrielli
Phys. Rev. E 57, 3878 – Published 1 April 1998
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Abstract

We introduce a model for fractures in quenched disordered media. This model has a deterministic extremal dynamics, driven by the energy function of a network of springs (Born Hamiltonian). The breakdown is the result of the cooperation between the external field and the quenched disorder. This model can be considered as describing the low-temperature limit for crack propagation in solids. To describe the memory effects in this dynamics and then to study the resistance properties of the system we realized some numerical simulations of the model. The model exhibits interesting geometric and dynamical properties, with a strong reduction of the fractal dimension of the clusters and of their backbone, with respect to the case in which thermal fluctuations dominate. This result can be explained by a recently introduced theoretical tool as a screening enhancement due to memory effects induced by the quenched disorder.

  • Received 20 October 1997

DOI:https://doi.org/10.1103/PhysRevE.57.3878

©1998 American Physical Society

Authors & Affiliations

Guido Caldarelli1,2, Raffaele Cafiero3,4, and Andrea Gabrielli4,5

  • 1Theory of Condensed Matter, Cavendish Laboratory Madingley Road, CB3 0HE Cambridge, United Kingdom
  • 2Department of Theoretical Physics, The University, M13 9PL Manchester, United Kingdom
  • 3Max-Planck Institute for Physics of Complex Systems, Nöhnitzer Strasse 38, 01187 Dresden, Germany
  • 4INFM–Unità di Roma I, Università di Roma “La Sapienza,” Piazzale Aldo Moro 2, I-00185 Roma, Italy
  • 5Dipartimento di Fisica, Università di Roma “Tor Vergata,” via della Ricerca Scientifica 1, 00133 Roma, Italy

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Issue

Vol. 57, Iss. 4 — April 1998

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