Abstract
We consider finite element approximations to the optimal constant for the Hardy inequality with exponent in bounded domains of dimension or . For finite element spaces of piecewise linear and continuous functions on a mesh of size , we prove that the approximate Hardy constant converges to the optimal Hardy constant at a rate proportional to . This result holds in dimension , in any dimension if the domain is the unit ball and the finite element discretization exploits the rotational symmetry of the problem, and in dimension for general finite element discretizations of the unit ball. In the first two cases, our estimates show excellent quantitative agreement with values of the discrete Hardy constant obtained computationally.
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