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Global Continuation via Higher-Gradient Regularization and Singular Limits in Forced One-Dimensional Phase Transitions
We consider a standard "higher-gradient" model for forced phase transitions in one-dimensional, shape-memory solids. We prescribe a parameter-dependent body forcing. The component of the potential energy corresponding to conventional elasticity is characterized by a nonconvex stored energy...
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Published in: | SIAM journal on mathematical analysis 2000, Vol.31 (6), p.1307-1331 |
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Main Authors: | , |
Format: | Article |
Language: | English |
Subjects: | |
Citations: | Items that this one cites Items that cite this one |
Online Access: | Get full text |
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Summary: | We consider a standard "higher-gradient" model for forced phase transitions in one-dimensional, shape-memory solids. We prescribe a parameter-dependent body forcing. The component of the potential energy corresponding to conventional elasticity is characterized by a nonconvex stored energy function of the strain. Our main goal is to show that global solution branches of the regularized problem converge to a global branch of weak solutions in the limit of vanishing "capillarity" (the coefficient of the higher-gradient term). The existence of global branches for the regularized, semilinear problem is routine, based upon the Leray--Schauder degree. In the physically meaningful case when the body force is everywhere nonnegative, we obtain uniform a priori bounds via a subtle maximum principle. This together with topological connectivity arguments yields the existence of global branches of weak solutions to the zero-capillarity problem. Moreover, by examining the singular limits of various supplementary conservation laws (satisfied by all solutions of the regularized problem), we show that the above-mentioned weak solutions also minimize the potential energy of the zero-capillarity problem. |
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ISSN: | 0036-1410 1095-7154 |
DOI: | 10.1137/S0036141098340065 |