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Multiscale modeling of crack initiation and propagation at the nanoscale
Affiliation:2. Department of Mechanical and Aerospace Engineering Carleton University, Ottawa, ON, Canada;1. Research Institute for Energy Equipment Materials, Hebei University of Technology, Tianjin 300132, China;2. Tianjin Key Laboratory of Materials Laminating Fabrication and Interface Control Technology, Tianjin 300132, China;3. Department of Physics, University of Science and Technology Bannu, Bannu 28100, Pakistan;4. School of Mechanical Engineering, Hebei University of Technology, Tianjin 300132, China;1. Graduiertenkolleg 1462, Bauhaus-Universität Weimar, 99423 Weimar, Germany;2. Department of Mechanical Engineering, Isfahan University of Technology, Isfahan 84156-83111, Iran;3. Institute of Structural Mechanics, Bauhaus-Universität Weimar, Marienstr. 15, D-99423 Weimar, Germany;1. Structural Impact Laboratory (SIMLab), Department of Structural Engineering, Norwegian University of Science and Technology (NTNU), NO-7491 Trondheim, Norway;2. Centre for Advanced Structural Analysis (CASA), NTNU, NO-7491 Trondheim, Norway;3. Department of Solid Mechanics, Royal Institute of Technology (KTH), SE-100 44 Stockholm, Sweden;1. Department of Physics and Astronomy, University of Denver, Denver, CO 80208, USA;2. Department of Chemistry, Indiana University of PA, Indiana, PA 15705, USA;3. Department of Physics, Indiana University of PA, 975 Oakland Avenue, Weyandt Hall, Indiana, PA 15705, USA
Abstract:
Fracture occurs on multiple interacting length scales; atoms separate on the atomic scale while plasticity develops on the microscale. A dynamic multiscale approach (CADD: coupled atomistics and discrete dislocations) is employed to investigate an edge-cracked specimen of single-crystal nickel, Ni, (brittle failure) and aluminum, Al, (ductile failure) subjected to mode-I loading. The dynamic model couples continuum finite elements to a fully atomistic region, with key advantages such as the ability to accommodate discrete dislocations in the continuum region and an algorithm for automatically detecting dislocations as they move from the atomistic region to the continuum region and then correctly “converting” the atomistic dislocations into discrete dislocations, or vice-versa. An ad hoc computational technique is also applied to dissipate localized waves formed during crack advance in the atomistic zone, whereby an embedded damping zone at the atomistic/continuum interface effectively eliminates the spurious reflection of high-frequency phonons, while allowing low-frequency phonons to pass into the continuum region.The simulations accurately capture the essential physics of the crack propagation in a Ni specimen at different temperatures, including the formation of nano-voids and the sudden acceleration of the crack tip to a velocity close to the material Rayleigh wave speed. The nanoscale brittle fracture happens through the crack growth in the form of nano-void nucleation, growth and coalescence ahead of the crack tip, and as such resembles fracture at the microscale. When the crack tip behaves in a ductile manner, the crack does not advance rapidly after the pre-opening process but is blunted by dislocation generation from its tip. The effect of temperature on crack speed is found to be perceptible in both ductile and brittle specimens.
Keywords:Multiscale  Nanoscale  Crack  Dislocation
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