2006
DOI: 10.1093/acprof:oso/9780199211234.001.0001
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Multi-dimensional hyperbolic partial differential equations

Abstract: This book presents a view of the state of the art in multi-dimensional hyperbolic partial differential equations, with a particular emphasis on problems in which modern tools of analysis have proved useful. Ordered in sections of gradually increasing degrees of difficulty, the text first covers linear Cauchy problems and linear initial boundary value problems, before moving on to nonlinear problems, including shock waves. The book finishes with a discussion of the application of hyperbolic PDEs to gas dynamics… Show more

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Cited by 168 publications
(254 citation statements)
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“…To analyze (1.7) one uses pseudo-differential calculus. We have the following well-posedness result, see [3], Theorem 2.6. …”
Section: The Continuous Problemmentioning
confidence: 98%
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“…To analyze (1.7) one uses pseudo-differential calculus. We have the following well-posedness result, see [3], Theorem 2.6. …”
Section: The Continuous Problemmentioning
confidence: 98%
“…The standard procedure for hyperbolic equations in multi space dimensions is to symmetrize the system and derive an energy estimate. In order to do this we introduce the operator a · ∇ = a 1 ∂ x + a 2 ∂ y + a 3 Then we see that a simple way to symmetrize (1.1) is to add a "source" term: (which is supposed to be zero anyway!) −udivB, resulting in ∂ t B + curl(B × u) = −udivB.…”
Section: The Continuous Problemmentioning
confidence: 99%
“…Note that standard approaches to hyperbolic PDEs such as the linearisation approach described in Benzoni et al [3], or the addition of non-degenerate artificial viscosity as described in Evans [14], are not directly applicable to our problem as they destroy the structure of the equations on which our energy estimate relies.…”
Section: Existing Results and Methodology For Similar Problemsmentioning
confidence: 99%
“…For a vector w ∈ R 3 , we will write w for the first 2 components of w, so that w = (w , w 3 ). For example, x = (x , x 3 ), so that x denotes horizontal position, u = (u , u 3 ), so that u denotes horizontal velocity, and ∇ = (∇ , ∂ x 3 ), so that ∇ denotes horizontal gradient.…”
Section: Notationmentioning
confidence: 99%
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