2008
DOI: 10.1016/j.mechmat.2007.10.003
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Ordering effect of kinetic energy on dynamic deformation of brittle solids

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Cited by 14 publications
(45 citation statements)
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“…The time histories of the normal stress (in the loading direction) divided by the corresponding strain rate and the Poisson's ratio are presented in Figure 1. It is evident from Figure 1(a) that the two characteristic slopes are the short-time and long-time moduli (E ð"Þ st ,E ð"Þ lt , respectively 1 ) observed by Mastilovic et al (2008), presented herein in a more convenient graph.…”
Section: Lattice Simulationsmentioning
confidence: 79%
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“…The time histories of the normal stress (in the loading direction) divided by the corresponding strain rate and the Poisson's ratio are presented in Figure 1. It is evident from Figure 1(a) that the two characteristic slopes are the short-time and long-time moduli (E ð"Þ st ,E ð"Þ lt , respectively 1 ) observed by Mastilovic et al (2008), presented herein in a more convenient graph.…”
Section: Lattice Simulationsmentioning
confidence: 79%
“…The particular model used herein is described in a number of papers published over the last decade [see for instance, Mastilovic et al (2008) and references therein]; the only, but noteworthy, difference from those previous studies is that the present simulation setup does not include the application of the initial velocity field that cancels out the inertial effects. Thus, to put it as succinctly as possible, the lattice is formed by 'continuum particles' located at lattice nodes (1000 Â 1201) and connected by nonlinear springs characterized by a critical elongation defining rupture.…”
Section: Lattice Simulationsmentioning
confidence: 99%
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“…The effects of this loading procedure are demonstrated in literature (as reported by Mastilovic et al, 2008).…”
Section: Computer Simulations Of Uniaxial Tensionmentioning
confidence: 79%
“…The natural randomness of the mesoscale material texture is an example of the aleatory variability. The intrinsic (pre-existing) disorder is, in the course of deformation, further enhanced by the extrinsic disorder due to the damage evolution that is governed (to an extent depending on deformation rate; Mastilovic et al, 2008) by the local fluctuations of energy barriers quenched within the material and the local fluctuations of stress. The nonlocal and nonlinear character of these far-from-equilibrium processes is such that concepts of strain and damage (and temperature, in general) based on spatial and temporal averaging are, at best, conditionally acceptable (Mastilovic and Krajcinovic, 1999).…”
Section: Introductionmentioning
confidence: 99%