Abstract

Quasicontinuum simulations of “positive” and “negative” dislocations simultaneously interacting with Σ11 symmetrical tilt grain boundary (GB) during nanoindentation reveal two distinctive dislocation/GB interactions depending on the indenter size h and demarcated by a potential independent critical indenter size h¯cr. When h is less than h¯cr, lattice dislocations are eliminated by a reflected dislocation from dislocation-GB interaction. Meanwhile, less grain boundary dislocations (GBDs) are emitted. However, when h is greater than h¯cr, the “positive” and “negative” dislocations nucleate separately and interact with GB dependently due to one interaction site absorbing GBDs nucleated from another interaction site. The resulted GB configuration shows a regularly-stepped shape. Studies of a free-standing dissociated dislocation dipole (DP) shows that, hcr, depending on potentials, is a critical distance between two extended dislocations of a DP, at which the DP transforms configuration between stacking fault overlapping and non-overlapping configuration. The full edge DP model based on continuum theory, which does not take the strong interactions between partial dislocations into account, fails to predict hcr.

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