2001
DOI: 10.1557/proc-703-v3.9
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Dynamic Fracture Mechanisms in Nanostructured and Amorphous Silica Glasses Million-Atom Molecular Dynamics Simulations

Abstract: Parallel molecular dynamics simulations are performed to investigate dynamic fracture in bulk and nanostructured silica glasses at room temperature and 1000 K. In bulk silica the crack front develops multiple branches and nanoscale pores open up ahead of the crack tip. Pores coalesce and then they merge with the advancing crack-front to cause cleavage fracture. The calculated fracture toughness is in good agreement with experiments. In nanostrucutred silica the crack-front meanders along intercluster boundarie… Show more

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Cited by 26 publications
(39 citation statements)
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“…2 is advanced to À45 Å. The results are similar to those of SiO 2 MD simulations by Brutzel et al [26] and Muralidharan et al [27]. And the branching crack nucleated in the front of main crack is also observed, it may be contributed by interaction between water and SiO 2 .…”
Section: Analysis Of Molecular Dynamics Simulationsupporting
confidence: 86%
“…2 is advanced to À45 Å. The results are similar to those of SiO 2 MD simulations by Brutzel et al [26] and Muralidharan et al [27]. And the branching crack nucleated in the front of main crack is also observed, it may be contributed by interaction between water and SiO 2 .…”
Section: Analysis Of Molecular Dynamics Simulationsupporting
confidence: 86%
“…The origin of the nucleation of cavities should be found more likely in the amorphous structure, which contains inherent atomic density fluctuations at the nanometer scale. Such a scenario was indeed predicted by Molecular Dynamics Simulation [27,28,29,30] that evidenced atomic density fluctuations in the structure of simulated amorphous silica : The Si and O atoms are shown to form silica tetrahedra connected together to build rings of different sizes ranging from 3 to 9 tetrahedra. At larger length scales, ranging from 1.5 nm to 6 nm, the density of these rings is found to fluctuate with high density areas surrounded by low density areas.…”
Section: Discussionmentioning
confidence: 64%
“…At larger length scales, ranging from 1.5 nm to 6 nm, the density of these rings is found to fluctuate with high density areas surrounded by low density areas. Moreover, the Molecular Dynamics simulations of van Brutzel [28,29,30] show that, at this length scale, crack propagates by growth and coalescence of small cavities which appear in areas with low density of rings, ahead of the crack tip. They behave as stress concentrators and grow under the stress imposed by the presence of the main crack to give birth to the cavities actually observed in the AFM frames.…”
Section: Discussionmentioning
confidence: 99%
“…atoms in the material lack translational and/or rotational symmetry) as opposed to crystalline counterparts. Figure 7 displays a sectional view from a 3D molecular dynamics simulation of a pure amorphous silica system [43,[78][79][80][81][82][83]. In the context of the short range structural order, one silicon atom resides in the center of the tetrahedron structure with four oxygen atoms located at the corners of the tetrahedron.…”
Section: The Structure Of Oxide Glassesmentioning
confidence: 99%
“…These rings correspond to the mid-range order of SiO 2 glasses. A ring is the shortest path connecting a Si atom back to itself via Si O bonds [81,84,85]. The nomenclature for the ring size depends on the number of Si atoms in the ring.…”
Section: The Structure Of Oxide Glassesmentioning
confidence: 99%