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Energetic solutions to rate-independent large-strain elasto-plastic evolutions driven by discrete dislocation flow

Filip Rindler

Abstract

This work rigorously implements a recent model of large-strain elasto-plastic evolution in single crystals where the plastic flow is driven by the movement of discrete dislocation lines. The model is geometrically and elastically nonlinear, that is, the total deformation gradient splits multiplicatively into elastic and plastic parts, and the elastic energy density is polyconvex. There are two internal variables: The system of all dislocations is modeled via $1$-dimensional boundaryless integral currents, whereas the history of plastic flow is encoded in a plastic distortion matrix-field. As our main result we construct an energetic solution in the case of a rate-independent flow rule. Besides the classical stability and energy balance conditions, our notion of solution also accounts for the movement of dislocations and the resulting plastic flow. Because of the path-dependence of plastic flow, a central role is played by so-called ``slip trajectories'', that is, the surfaces traced out by moving dislocations, which we represent as integral $2$-currents in space-time. The proof of our main existence result further crucially rests on careful a-priori estimates via a nonlinear Gronwall-type lemma and a rescaling of time. In particular, we have to account for the fact that the plastic flow may cause the coercivity of the elastic energy functional to decay along the evolution, and hence the solution may blow up in finite time.

Energetic solutions to rate-independent large-strain elasto-plastic evolutions driven by discrete dislocation flow

Abstract

This work rigorously implements a recent model of large-strain elasto-plastic evolution in single crystals where the plastic flow is driven by the movement of discrete dislocation lines. The model is geometrically and elastically nonlinear, that is, the total deformation gradient splits multiplicatively into elastic and plastic parts, and the elastic energy density is polyconvex. There are two internal variables: The system of all dislocations is modeled via -dimensional boundaryless integral currents, whereas the history of plastic flow is encoded in a plastic distortion matrix-field. As our main result we construct an energetic solution in the case of a rate-independent flow rule. Besides the classical stability and energy balance conditions, our notion of solution also accounts for the movement of dislocations and the resulting plastic flow. Because of the path-dependence of plastic flow, a central role is played by so-called ``slip trajectories'', that is, the surfaces traced out by moving dislocations, which we represent as integral -currents in space-time. The proof of our main existence result further crucially rests on careful a-priori estimates via a nonlinear Gronwall-type lemma and a rescaling of time. In particular, we have to account for the fact that the plastic flow may cause the coercivity of the elastic energy functional to decay along the evolution, and hence the solution may blow up in finite time.

Paper Structure

This paper contains 25 sections, 37 theorems, 357 equations.

Key Result

Lemma 2.1

Let $w \in \mathrm{BV}([0,T];X)$. Then, for every $t \in [0,T]$, the left and right limits exist (only the left limit at $0$ and only the right limit at $T$). For all but at most countably many jump points$t \in (0,T)$, it also holds that $w(t+) = w(t-) =: w(t)$.

Theorems & Definitions (84)

  • Lemma 2.1
  • Proposition 2.2
  • Lemma 2.3
  • Example 2.4
  • Lemma 2.5
  • Proposition 2.6
  • Proposition 2.7
  • Example 3.1
  • Lemma 3.2
  • proof
  • ...and 74 more