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1988
DOI: 10.1016/0001-6160(88)90099-5
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Atomistics of crack propagation

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Cited by 33 publications
(13 citation statements)
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“…On the other hand, in dynamic fracture simulations large system sizes are necessary because of the boundary effects such as wave reflection and the problem of dislocations near fixed boundaries. Thus, simulations have so far mostly been done by using a simple pair potential in a twodimensional system 6,7 or in a system with otherwise less degrees of freedom. 8 Until recently, three-dimensional ͑3D͒ simulations with a realistic many-body potential for describing the behavior of ductile materials, e.g., copper, could be realized only in small systems.…”
Section: Introductionmentioning
confidence: 99%
“…On the other hand, in dynamic fracture simulations large system sizes are necessary because of the boundary effects such as wave reflection and the problem of dislocations near fixed boundaries. Thus, simulations have so far mostly been done by using a simple pair potential in a twodimensional system 6,7 or in a system with otherwise less degrees of freedom. 8 Until recently, three-dimensional ͑3D͒ simulations with a realistic many-body potential for describing the behavior of ductile materials, e.g., copper, could be realized only in small systems.…”
Section: Introductionmentioning
confidence: 99%
“…Molecular dynamics simulations were also performed to investigate the crack propagation velocity (Sieradzki and Dienes 1988;Abraham and Gao 2000) and crack branching (Zhou et al 1996). According to Abraham and Gao (2000), the propagation velocity is bounded by the Rayleigh wave speed in mode I whereas it could reach the To analyze the sensitivity of the model predictions to this parameter, the closed form solutions of the model are used [Equations (15) to (21)].…”
mentioning
confidence: 99%
“…Marder has pointed out that theory and experiment are at variance with respect to one another and has properly emphasized the fact that cracks have a terminal velocity of about half of theoretical predictions. While detailed comparison between theory and experiment regarding a crack-tip equation of motion has not been possible, we would like to point out that molecular-dynamic (MD) simulations have been used to study these issues in considerable detail [2][3][4]. The results of these simulations suggest that crack dynamics is strongly influenced by the lattice structure of a solid and that the physics which controls the terminal velocity of a crack can only be understood by consideration of the discrete atomic nature of solids.…”
mentioning
confidence: 99%
“…Since the theoretical crack-tip terminal velocity is the long wavelength Rayleigh velocity ( = 0.56i^), this corresponds to about 64% of the value predicted by continuum approaches. Sieradzki et al [3] used MD to study crack propagation in the 2D triangular Johnson solid. The relevant results of that investigation are the following: (1) The measured terminal velocity is independent of sample size and loading condition and is =0.25i^ and (2) cracks rapidly achieve terminal velocity even under loading conditions when the energy available for crack growth barely exceeds the energy required to create the crack faces.…”
mentioning
confidence: 99%
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