On the ΓΓ-limit of singular perturbation problems with optimal profiles which are not one-dimensional. Part II: The lower bound

preprint2013arXivOpen access

Abstract

In part II we constructed the lower bound, in the spirit of ΓΓ- lim inf⁡\liminf for some general classes of singular perturbation problems, with or without the prescribed differential constraint, taking the form E_\e(v):=\int_Ω\frac{1}{\e}F\Big(\e^n\nabla^n v,...,\e\nabla v,v\Big)dx\quad\text{for}\;\; v:Ω\subset\R^N\to\R^k\;\;\text{such that}\;\; A\cdot\nabla v=0, where the function F≥0F\geq 0 and A:Rk×N→RmA:\R^{k\times N}\to\R^m is a prescribed linear operator (for example, A:≡0A:\equiv 0, A⋅∇v:=curl vA\cdot\nabla v:=\text{curl}\, v and A⋅∇v=divvA\cdot\nabla v=\text{div} v). Furthermore, we studied the cases where we can easy prove the coinciding of this lower bound and the upper bound obtained in [33]. In particular we find the formula for the ΓΓ-limit for the general class of anisotropic problems without a differential constraint (i.e., in the case A:≡0A:\equiv 0).

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