Regularity of the Optimal Sets for a Class of Integral Shape Functionals

IF 4.6 Q2 MATERIALS SCIENCE, BIOMATERIALS ACS Applied Bio Materials Pub Date : 2024-05-15 DOI:10.1007/s00205-024-01984-y
Giuseppe Buttazzo, Francesco Paolo Maiale, Dario Mazzoleni, Giorgio Tortone, Bozhidar Velichkov
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Abstract

We prove the first regularity theorem for the free boundary of solutions to shape optimization problems involving integral functionals, for which the energy of a domain \(\Omega \) is obtained as the integral of a cost function j(ux) depending on the solution u of a certain PDE problem on \(\Omega \). The main feature of these functionals is that the minimality of a domain \(\Omega \) cannot be translated into a variational problem for a single (real or vector valued) state function. In this paper we focus on the case of affine cost functions \(j(u,x)=-g(x)u+Q(x)\), where u is the solution of the PDE \(-\Delta u=f\) with Dirichlet boundary conditions. We obtain the Lipschitz continuity and the non-degeneracy of the optimal u from the inwards/outwards optimality of \(\Omega \) and then we use the stability of \(\Omega \) with respect to variations with smooth vector fields in order to study the blow-up limits of the state function u. By performing a triple consecutive blow-up, we prove the existence of blow-up sequences converging to homogeneous stable solution of the one-phase Bernoulli problem and according to the blow-up limits, we decompose \(\partial \Omega \) into a singular and a regular part. In order to estimate the Hausdorff dimension of the singular set of \(\partial \Omega \) we give a new formulation of the notion of stability for the one-phase problem, which is preserved under blow-up limits and allows to develop a dimension reduction principle. Finally, by combining a higher order Boundary Harnack principle and a viscosity approach, we prove \(C^\infty \) regularity of the regular part of the free boundary when the data are smooth.

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一类积分形状函数最优集的规律性
我们证明了涉及积分函数的形状优化问题解的自由边界的第一个正则定理,对于这些积分函数,域 \(\Omega \)的能量是作为成本函数 j(u, x) 的积分得到的,而成本函数 j(u, x) 取决于某个 PDE 问题在 \(\Omega \)上的解 u。这些函数的主要特点是域 \(\Omega \)的最小性不能转化为单一(实值或向量值)状态函数的变分问题。在本文中,我们将重点放在仿射成本函数 (j(u,x)=-g(x)u+Q(x))的情况上,其中 u 是具有 Dirichlet 边界条件的 PDE (-\Delta u=f\)的解。我们从\(\ω \)的向内/向外最优性中得到最优u的Lipschitz连续性和非退化性,然后利用\(\ω \)相对于光滑矢量场变化的稳定性来研究状态函数u的炸毁极限。通过进行三重连续吹胀,我们证明了收敛于单相伯努利问题同质稳定解的吹胀序列的存在性,并根据吹胀极限将 \(\partial \Omega \)分解为奇异部分和规则部分。为了估算 \(\partial \Omega \)奇异集的豪斯多夫维度,我们给出了单相问题稳定性概念的新表述,它在炸毁极限下保持不变,并允许发展维度缩减原理。最后,通过结合高阶边界哈纳克原理和粘度方法,我们证明了当数据光滑时自由边界规则部分的(C^\infty \)正则性。
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来源期刊
ACS Applied Bio Materials
ACS Applied Bio Materials Chemistry-Chemistry (all)
CiteScore
9.40
自引率
2.10%
发文量
464
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