Abstract

We examine theoretically the impact of dissolved solute atoms on the motion of dislocations in metals and, hence, on their plastic response. Two regimes of behavior are distinguished; a low velocity regime, in which the dislocation drags a near equilibrium solute cloud, and a high velocity regime, in which the dislocation is alternately trapped and free running. In both regimes, the overdamped motion of a dislocation in the alloy is exactly as it would be in the pure system but with regime-dependent dislocation mobilities. In the low velocity regime, the forces between dislocations are replaced by forces between dislocation-solute cloud “quasiparticles.” This paper provides analytical estimates for the mobilities in the two regimes, as well as expressions for calculating quasiparticle interactions. Finally, a prescription is provided for carrying out dislocation dynamics simulations without explicitly incorporating solute degrees of freedom.

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