We consider a Dirichlet problem for the Poisson equation in a periodically perforated domain. The geometry of the domain is controlled by two parameters: A real number I > 0, proportional to the radius of the holes, and a map φ, which models the shape of the holes. So, if g denotes the Dirichlet boundary datum and f the Poisson datum, we have a solution for each quadruple ( I , φ , g , f ). Our aim is to study how the solution depends on ( I , φ , g , f ), especially when I is very small and the holes narrow to points. In contrast with previous works, we do not introduce the assumption that f has zero integral on the fundamental periodicity cell. This brings in a certain singular behavior for I close to 0. We show that, when the dimension n of the ambient space is greater than or equal to 3, a suitable restriction of the solution can be represented with an analytic map of the quadruple ( I , φ , g , f ) multiplied by the factor 1 / I n-2 . In case of dimension n = 2, we have to add log I times the integral of f / 2 I .

Singular behavior for a multi-parameter periodic Dirichlet problem

Luzzini P.;Musolino P.
2023

Abstract

We consider a Dirichlet problem for the Poisson equation in a periodically perforated domain. The geometry of the domain is controlled by two parameters: A real number I > 0, proportional to the radius of the holes, and a map φ, which models the shape of the holes. So, if g denotes the Dirichlet boundary datum and f the Poisson datum, we have a solution for each quadruple ( I , φ , g , f ). Our aim is to study how the solution depends on ( I , φ , g , f ), especially when I is very small and the holes narrow to points. In contrast with previous works, we do not introduce the assumption that f has zero integral on the fundamental periodicity cell. This brings in a certain singular behavior for I close to 0. We show that, when the dimension n of the ambient space is greater than or equal to 3, a suitable restriction of the solution can be represented with an analytic map of the quadruple ( I , φ , g , f ) multiplied by the factor 1 / I n-2 . In case of dimension n = 2, we have to add log I times the integral of f / 2 I .
2023
File in questo prodotto:
File Dimensione Formato  
2211.11631.pdf

accesso aperto

Tipologia: Preprint (submitted version)
Licenza: Accesso libero
Dimensione 621.25 kB
Formato Adobe PDF
621.25 kB Adobe PDF Visualizza/Apri
Pubblicazioni consigliate

I documenti in IRIS sono protetti da copyright e tutti i diritti sono riservati, salvo diversa indicazione.

Utilizza questo identificativo per citare o creare un link a questo documento: https://hdl.handle.net/11577/3495127
Citazioni
  • ???jsp.display-item.citation.pmc??? ND
  • Scopus 0
  • ???jsp.display-item.citation.isi??? 0
social impact