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Coincidence lattice model for the structure and energy of grain boundaries
Affiliation:1. Department of Materials Science and Engineering, Carnegie Mellon University, Pittsburgh, PA 15213, USA;2. Aix-Marseille Univ, CNRS, CINaM, Marseille 13009, France;3. NCEM-Molecular Foundry, LBNL, Berkeley, CA 94270, USA;1. Peter the Great St. Petersburg Polytechnic University, Polytechnicheskaya 29, St. Petersburg 195251, Russia;2. Institute of Problems of Mechanical Engineering, Russian Academy of Sciences, Bolshoj pr. 61, Vasiljevskii Ostrov, St. Petersburg 199178, Russia;3. Saint Petersburg State University, 7/9 Universitetskaya nab., St. Petersburg 199034, Russia;4. ITMO University, Kronverksky pr. 49, St. Petersburg 197101, Russia
Abstract:The Coincidence Site Lattice (CSL) model of grain boundaries is developed on a simple physical basis. We propose that, to a good approximation, the construction of a boundary can be described in terms of three basic steps:(1) a rigid body joining of two perfect crystals along the boundary plane (Step I); (2) a primary relaxation (Step II) consisting of relaxations in the boundary centered on 0-Lattice elements which act to improve lattice matching in these regions; and (3) a possible secondary relaxation (Step III) which produces the final structure composed of patches of a low ∑ boundary and secondary grain boundary dislocations. The energy after Step I is obtained by summing pairwise interactions across the boundary and is found to be relatively low for a number of low ∑ boundaries and to approach a larger constant value for all large ∑ boundaries. The energy decrease due to Step II varies monotonically with crystal misorientation according to a Read-Shockley function, and the energy decrease associated with Step III produces cusps in the energy versus misorientation curve at misorientations corresponding to low ∑ boundaries. The model appears to be consistent with our present knowledge of boundary structure and energy, and its general applicability is discussed.
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