1992
DOI: 10.1007/bf02099268
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Convergence to nonlinear diffusion waves for solutions of a system of hyperbolic conservation laws with damping

Abstract: We consider a model of hyperbolic conservation laws with damping and show that the solutions tend to those of a nonlinear parabolic equation timeasymptotically. The hyperbolic model may be viewed as isentropic Euler equations with friction term added to the momentum equation to model gas flow through a porous media. In this case our result justifies Darcy's law timeasymptotically. Our model may also be viewed as an elastic model with damping.

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Cited by 362 publications
(310 citation statements)
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“…We will see that an easy lemma plays an important role. It should be pointed out that the key approach in [13][14][15][16][17][18][19][20][21] is to compare the solution of (1.2)-(1.3) with the similarity solution of (1.4) via energy estimates. Unfortunately, the exponential decay rate cannot be achieved by this approach, due to the boundary effects.…”
Section: Preliminaries and Main Resultsmentioning
confidence: 99%
See 1 more Smart Citation
“…We will see that an easy lemma plays an important role. It should be pointed out that the key approach in [13][14][15][16][17][18][19][20][21] is to compare the solution of (1.2)-(1.3) with the similarity solution of (1.4) via energy estimates. Unfortunately, the exponential decay rate cannot be achieved by this approach, due to the boundary effects.…”
Section: Preliminaries and Main Resultsmentioning
confidence: 99%
“…In this direction, the readers are referred to [31], [13], [14] and [12] for existence of small smooth solutions; to [27], [4], and [6] for solutions in BV ; to [7] and [20] for L ∞ solutions. For large time behavior of solutions, we refer [13], [14], [33], [34] and [45] fore small smooth solutions; and we refer [19], [21], [39] and [47] for weak solutions. For initial boundary value problems, see [16], [28] and [35] for small smooth solutions.…”
Section: Introductionmentioning
confidence: 99%
“…[8,9,10,17]): so that the Barenblatt self-similar solution defined in I b (t) has the same total mass as that for the solution of (1.1):…”
Section: γ(T) = U(γ(t) T)mentioning
confidence: 99%
“…When there are no phase transitions in the flow, then the third equation is missing and p only depends on v. The corresponding 2 × 2 system has been studied by many authors: see [36,13,28,29,37,14,30], for the homogeneous case or with continuous source terms and [32,33] for the case of discontinuous source terms.…”
Section: Introductionmentioning
confidence: 99%