2009
DOI: 10.1002/cpa.20285
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Well‐posedness for compressible Euler equations with physical vacuum singularity

Abstract: An important problem in the theory of compressible gas flows is to understand the singular behavior of vacuum states. The main difficulty lies in the fact that the system becomes degenerate at the vacuum boundary, where the characteristic speeds u˙c coincide and have unbounded spatial derivative since c behaves like x 1=2 close to the boundary. In this paper, we overcome this difficulty by presenting a new formulation and new energy spaces. We establish the local-in-time well-posedness of one-dimensional compr… Show more

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Cited by 146 publications
(153 citation statements)
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“…The only existence theory for the physical vacuum singularity that we are aware of can be found in the recent paper by Jang and Masmoudi [6] for the 1D compressible gas; we refer the interested reader to the introduction in that paper for a nice history of the analysis of the 1D compressible Euler equations with damping.…”
Section: History Of Prior Results For the Compressible Euler Equationmentioning
confidence: 99%
See 1 more Smart Citation
“…The only existence theory for the physical vacuum singularity that we are aware of can be found in the recent paper by Jang and Masmoudi [6] for the 1D compressible gas; we refer the interested reader to the introduction in that paper for a nice history of the analysis of the 1D compressible Euler equations with damping.…”
Section: History Of Prior Results For the Compressible Euler Equationmentioning
confidence: 99%
“…Letting ∂ 6We use Young's inequality and the fundamental theorem of calculus (with respect to t) for the last integral to find that for δ > 0,…”
Section: E(t))mentioning
confidence: 99%
“…First, using the Taylor expansion, one may verify that for γ > 4/3, 13) provided (3.1) holds for a suitably small constant ǫ 0 , where C(γ) is a positive constant depending on γ. Also,…”
Section: Lower-order Estimatesmentioning
confidence: 99%
“…And the initial density is supposed to satisfy the following condition: (r) ∼ R 0 − r as r close to R 0 , (1.5) that is, the initial sound speed is C 1/2 -Hölder continuous across the vacuum boundary, which is called the physical vacuum for the compressible inviscid flows (cf. [2,3,13,25,42]). …”
Section: Introductionmentioning
confidence: 99%
“…[5,11]) and continuation arguments. The uniqueness of the smooth solutions can be obtained as in section 11 of [20].…”
Section: Proof Of Theorem 21mentioning
confidence: 99%