On an Anisotropic Fractional Stefan-Type Problem with Dirichlet Boundary Conditions

preprint2022arXivOpen access

Abstract

In this work, we consider the fractional Stefan-type problem in a Lipschitz bounded domain Ω⊂RdΩ\subset\mathbb{R}^d with time-dependent Dirichlet boundary condition for the temperature ϑ=ϑ(x,t)\vartheta=\vartheta(x,t), ϑ=g\vartheta=g on Ωc×]0,T[Ω^c\times]0,T[, and initial condition η0η_0 for the enthalpy η=η(x,t)η=η(x,t), given in Ω×]0,T[Ω\times]0,T[ by ∂η∂t+LAsϑ=f with η∈β(ϑ),\frac{\partial η}{\partial t} +\mathcal{L}_A^s \vartheta= f\quad\text{ with }η\in β(\vartheta), where LAs\mathcal{L}_A^s is an anisotropic fractional operator defined in the distributional sense by ⟨LAsu,v⟩=∫RdADsu⋅Dsv dx,\langle\mathcal{L}_A^su,v\rangle=\int_{\mathbb{R}^d}AD^su\cdot D^sv\,dx, ββ is a maximal monotone graph, A(x)A(x) is a symmetric, strictly elliptic and uniformly bounded matrix, and DsD^s is the distributional Riesz fractional gradient for 0<s<10<s<1. We show the existence of a unique weak solution with its corresponding weak regularity. We also consider the convergence as s↗1s\nearrow 1 towards the classical local problem, the asymptotic behaviour as t→∞t\to\infty, and the convergence of the two-phase Stefan-type problem to the one-phase Stefan-type problem by varying the maximal monotone graph ββ.

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