Abstract

All finite element methods, as well as much of the Hilbert-space theory for partial differential equations, rely on variational formulations, that is, problems of the type: find $u\in V$ such that $a(v,u) = l(v)$ for each $v\in L$, where $V, L$ are Sobolev spaces. However, for systems of Friedrichs type, there is a sharp disparity between established well-posedness theories, which are not variational, and the very successful discontinuous Galerkin methods that have been developed for such systems, which are variational. In an attempt to override this dichotomy, we present, through three specific examples of increasing complexity, well-posed variational formulations of boundary and initial--boundary-value problems of Friedrichs type. The variational forms we introduce are generalizations of those used for discontinuous Galerkin methods, in the sense that inhomogeneous boundary and initial conditions are enforced weakly through integrals in the variational forms. In the variational forms we introduce, the solution space is defined as a subspace $V$ of the graph space associated with the differential operator in question, whereas the test function space $L$ is a tuple of $L^2$ spaces that separately enforce the equation, boundary conditions of characteristic type, and initial conditions.

Highlights

  • Many mathematical models in applications are most naturally derived and formulated as systems of first-order partial differential equations, for instance the Maxwell equations and the linearized Euler equations of gas dynamics

  • D. thesis [13], there has been a renewed interest in the theory of Friedrichs systems, due to the development of discontinuous Galerkin methods, which have emerged as suitable numerical methods for systems written in first-order form

  • We address specificboundary-value problems for operators characterized by property (1.2) and employ closely related variational formulations in order to specify precisely in what sense theboundary-value problem is set and to establish well-posedness in this sense

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Summary

Introduction

Many mathematical models in applications are most naturally derived and formulated as systems of first-order partial differential equations, for instance the Maxwell equations and the linearized Euler equations of gas dynamics. Through three increasingly complex examples of Friedrichs systems (§ 3–§ 5), the aim of our contribution is to introduce well-posed variational formulations in the sense of (1.6), in which boundary and initial conditions are imposed weakly, as in discontinuous Galerkin methods. The analysis of the elliptic problem is simplified by the fact that the graph space can be characterized as a Cartesian product of standard Sobolev spaces This simplification is not available in the last and most complex example, the acoustic wave equation, which involves inhomogeneous boundary as well as initial conditions. We believe that having access to true variational formulations of Friedrichs-type systems is in itself of interest and closes a “gap” in the classical Hilbert-space approach to the analysis of partial differential equations. The variational forms presented below constitute variations of the ones used for discontinuous Galerkin discretizations, and may serve as an inspiration for the development of new numerical methods for Friedrichs systems

Well-posedness of variational problems
Example 1: steady advection
The Discontinuous Galerkin method
An ill-posed variational formulation
A well-posed variational formulation
Example 2: an elliptic model problem
W γnξ 1
Example 3: the acoustic wave equation
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