1992
DOI: 10.1017/s0308210500014955
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Initial boundary value problems for isentropic gas dynamics

Abstract: SynopsisFor piston problems for a system of isentropic gas dynamics, convergence theorems of a difference scheme are obtained by compensated compactness theory and by analysis of the difference scheme.

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Cited by 7 publications
(6 citation statements)
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“…Initial boundary value problems associated with (5)0 were studied by S. Takano [7]. On the other hand the initial value problem without boundary conditions for non-homogeneous systems (h ~ 0) was studied by X. Ding et al [3].…”
Section: (R < R)mentioning
confidence: 99%
See 1 more Smart Citation
“…Initial boundary value problems associated with (5)0 were studied by S. Takano [7]. On the other hand the initial value problem without boundary conditions for non-homogeneous systems (h ~ 0) was studied by X. Ding et al [3].…”
Section: (R < R)mentioning
confidence: 99%
“…Introducing the vector variable U ----t(p, rn), where m = pu, we can write ( The Riemann problem of (5)0' is the Cauchy problem for the initial condition u Ir=0 = ~ aL (x < 0) (7) uR (x > 0). This problem is solved uniquely in a standard manner.…”
Section: (R < R)mentioning
confidence: 99%
“…Once we have these generalized Riemann solutions, we can construct the Godunov scheme and prove the existence of the generalized solution for the mixed problem. The following theorem is given by Takeno [22]. More precisely, if the initial data belong to Ac, then the generalized solutions constructed by the Godunov scheme for the mixed problem (5.1) also belong to…”
Section: Extension To Initial Boundary Problemsmentioning
confidence: 98%
“…Liu ([8]) solved the free piston problem for gas dynamics in Lagrange coordinate provided that the total variation of the initial data is sufficiently small by using the Glimm method. In [13], the author recently solved initial boundary value problems, the so-called moving piston problem, by using a compensated compactness theory provided that 1 < ~/ ~ 5/3. Now, we shall prove the following theorem.…”
Section: [ (P(xo)u(xo))=(po(x)uo(x))mentioning
confidence: 99%
“…The proof of this theorem mainly follows [13]. In Section 2 we introduce notations and basic lemmas for the construction of the approximate solution.…”
Section: Where C 1 and C2 Ate Constants The Piston Path X(t) Is Contmentioning
confidence: 99%