Abstract
Strong local minimizers with surfaces of gradient discontinuity appear in variational problems when the energy density function is not rank-one convex. In this paper we show that the stability of such surfaces is related to the stability outside the surface via a single jump relation that can be regarded as an interchange stability condition. Although this relation appears in the setting of equilibrium elasticity theory, it is remarkably similar to the well-known normality condition that plays a central role in classical plasticity theory.
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Notes
The choice of the orientation of the unit normal is unimportant as long as it is smooth. By convention, the unit normal points to the region labeled “\(+\)”.
The choice of unit ball as a support of the test function \(\varvec{\phi }\) is arbitrary. \(\varvec{\phi }\) can be supported in any bounded domain of \(\mathbb { R}^{d}\), see Ball (1976).
Projection onto the second component defines the same surface because of the symmetry of equations under the phase interchange \(\varvec{ F}_{+}\rightarrow \varvec{ F}_{-}\), \(\varvec{ F}_{-}\rightarrow \varvec{ F}_{+}\), \(\varvec{ n}\rightarrow -\varvec{ n}\).
In fact, \(\varvec{ P}_\mathrm{tot}(t)=t\varvec{ P}_{+}+(1-t)\varvec{ P}_{-}\), as was shown in Ball et al. (2000).
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Acknowledgments
The authors are grateful to the anonymous referee for valuable comments and corrections. We also thank Bob Kohn for his suggestions. This material is based on work supported by the National Science Foundation under Grant 1008092 and the French ANR Grant EVOCRIT (2008–2012).
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Communicated by Robert V. Kohn.
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Grabovsky, Y., Truskinovsky, L. Normality Condition in Elasticity. J Nonlinear Sci 24, 1125–1146 (2014). https://doi.org/10.1007/s00332-014-9213-x
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DOI: https://doi.org/10.1007/s00332-014-9213-x