Abstract

Let $M^{N\times n}$ be the space of real $N\times n$ matrices. We construct non-negative quasiconvex functions $F:M^{N\times n}\to R_+$ of quadratic growth whose zero sets are the graphs $\Gamma_f$ of certain Lipschitz mappings $f:K\subset E\to$ $E^$⊥, where $E\subset M^{N\times n}$ is a linear subspace without rank-one matrices, $K$ a compact subset of $E$ with $E^$⊥ its orthogonal complement. We show that the gradients $DF:M^{N\times n}\to M^{N\times n}$are strictly quasimonotone mappings and satisfy certain growth and coercivity conditions so that the variational integrals $u\to \int_{\Omega}F(Du(x))dx$ satisfythe Palais-Smale compactness condition in $W^{1,2}$.If $K$ is a smooth compact manifold of $E$ withoutboundary and the Lipschtiz mapping $f$ is of class $C^2$, then the closed $\epsilon$-neighbourhoods $(\Gamma_f)_\epsilon$ for small $\epsilon>0$ are quasiconvex sets.

Highlights

  • M N×n are strictly quasimonotone mappings and satisfy certain growth and coercivity conditions so that the variational integrals u

  • Similar results were obtained in [Z8] for a double well energy arising in material microstructure models based on geometrically linear elasticity [BJ1,BJ2,BFJK,K]

  • Let M N×n be the linear space of N × n matrices equipped with the usual Euclidean inner product of RNn, that is, A · B = tr(AT B), where tr is the trace of a square matrix

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Summary

Lipschitz constant

For λ satisfying α < λ/2 ≤ λE/2, the quasiconvex function Fλ(X) given by Theorem 1 satisfies (i) Fλ ∈ C1,1(M N×n) and. (i) the function Fλ(·) satisfies c0|X|2 − C1 ≤ Fλ(X) ≤ C(|X|2 + 1), X ∈ M N×n, where c0, C1 and C are positive constants; (ii) the gradient mapping DFλ(·) satisfies the coercivity conditions. The function F (X) = dist2(X, Γf ) − σqλ(X) satisfies all other requirements of [BKK,Th.5.5] as it is of quadratic growth and satisfies the upper-differentiability condition, that is, for each fixed X there is some U (X) ∈ M N×n such that. Since H2(·) is already a convex function, we only need to calculate the convex envelope C[H1(PE⊥ (X)] to obtain a lower bound of Gλ(X) = C(dist2(X, Γf ) − σqλ(X)), that is. The upper bound in Theorem 3(i) is obtained

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