We propose a discontinuous Galerkin method for the Poisson equation on polygonal tessel- lations in two dimensions, stabilized by penalizing, locally in each element K, a residual term involving the fluxes, measured in the norm of the dual of H1(K). The scalar product corresponding to such a norm is numerically realized via the introduction of a (minimal) auxiliary space inspired by the Virtual Element Method. Stability and optimal error estimates in the broken H1 norm are proven under a weak shape regularity assumption allowing the presence of very small edges. The results of numerical tests confirm the theoretical estimates.

A polygonal discontinuous Galerkin method with minus one stabilisation

S Bertoluzza;D Prada
2021

Abstract

We propose a discontinuous Galerkin method for the Poisson equation on polygonal tessel- lations in two dimensions, stabilized by penalizing, locally in each element K, a residual term involving the fluxes, measured in the norm of the dual of H1(K). The scalar product corresponding to such a norm is numerically realized via the introduction of a (minimal) auxiliary space inspired by the Virtual Element Method. Stability and optimal error estimates in the broken H1 norm are proven under a weak shape regularity assumption allowing the presence of very small edges. The results of numerical tests confirm the theoretical estimates.
2021
Istituto di Matematica Applicata e Tecnologie Informatiche - IMATI -
Inglese
55
785
810
26
https://www.esaim-m2an.org/articles/m2an/abs/2021/01/m2an190190/m2an190190.html
Sì, ma tipo non specificato
Discontinuous Galerkin method
polygonal tessellation
minus one stabilization
Pubblicato online: 26 febbraio 2021
Elettronico
2
info:eu-repo/semantics/article
262
Bertoluzza, S; Prada, D
01 Contributo su Rivista::01.01 Articolo in rivista
open
   New CHallenges for (adaptive) PDE solvers: the interplay of ANalysis and GEometry
   CHANGE
   H2020
   694515
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Utilizza questo identificativo per citare o creare un link a questo documento: https://hdl.handle.net/20.500.14243/424055
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