Abstract
In part II we constructed the lower bound, in the spirit of - 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 and is a prescribed linear operator (for example, , and ). 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 -limit for the general class of anisotropic problems without a differential constraint (i.e., in the case ).
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