Analytical approximation for the generalized laplace equation with step function coefficient

Many problems in science and engineering require the solution of thsteady-state diffusion equation with a highly oscillatory coefficient. In this paper, we propose an analytical approximation ũ(x) ε L ^P(ω), 1 ≥ p ≥ ∞, for the generalized Laplace equation ▼ · (Κ (x) ▼u(x)) = 0 in ω s{cyrillic} Rⁿ, with prescribed boundary conditions and the coefficient function Κ(x) ε L^P(ω) defined as a step function, not necessarily periodic. The proposed solution can be regarded as an approximation to theweak solution belonging to W^1,p (ω), the Sobolev space. When the coefficient function describes inclusions in a main matrix, then Κ(x) is a periodic function, and such formulation leads to an approximation, in L^p(ω), to the solution of the periodic cell-problem, ▼ · (Κ(ε^-1x) = ▼w(ε^-1 x)) = ▼ · (Κ(ε^-1 x)1). The solution to the cell-problem is the key information needed to obtain the upscaled coefficient and therefore the zeroth-order approximation for a generalized elliptic equation with highly oscillating coefficient in ω s{cyrillic} Rⁿ. Our numerical computation of the error between the proposed analytical approximation for the cell-problem, w̃(ε ^-1x) in L^p(Ω), and the solution w(ε ^-1x) in W^1,2 Ω), demonstrates to converge in the L² -norm, when the scale parameter ε approacheszero. The proposed approximation leads to the lower bound of the generalized Voigt-Reiss inequality, which is a more accurate two-sided estimate than the classical Voigt-Reiss inequality. As an application, we compute our approximate value for the homogenized coefficient when theheterogeneous coefficients are inclusions such as squares, circles, and lozenges, and we demonstrate that the results underestimate the effective coefficient with an error of 10% on average, when compared with publishednumerical results.