Articles

THE EXISTENCE OF A BOUNDED INVARIANT REGION FOR COMPRESSIBLE EULER EQUATIONS IN DIFFERENT GAS STATES

  • Weifeng JIANG ,
  • Zhen WANG
Expand
  • 1. College of Science, China Jiliang University, Hangzhou 310018, China;
    2. College of Science, Wuhan University of Technology, Wuhan 430071, China

Received date: 2019-08-24

  Revised date: 2020-05-13

  Online published: 2020-11-04

Supported by

The first author was supported by the Natural Science Foundation of Zhejiang (LQ18A010004), the second author was supported by the Fundamental Research Funds for the Central Universities (WUT: 2020IB011).

Abstract

In this article, by the mean-integral of the conserved quantity, we prove that the one-dimensional non-isentropic gas dynamic equations in an ideal gas state do not possess a bounded invariant region. Moreover, we obtain a necessary condition on the state equations for the existence of an invariant region for a non-isentropic process. Finally, we provide a mathematical example showing that with a special state equation, a bounded invariant region for the non-isentropic process may exist.

Cite this article

Weifeng JIANG , Zhen WANG . THE EXISTENCE OF A BOUNDED INVARIANT REGION FOR COMPRESSIBLE EULER EQUATIONS IN DIFFERENT GAS STATES[J]. Acta mathematica scientia, Series B, 2020 , 40(5) : 1229 -1239 . DOI: 10.1007/s10473-020-0505-y

References

[1] Tartar L. The compensated compactness method applied to systems of conservation laws//Syst Nonlin Part Differ Equ. Springer, 1983:263-285
[2] DiPerna R J. Convergence of the viscosity method for isentropic gas dynamics. Commun Math Phys, 1983, 91:1-30
[3] DiPerna R J. Convergence of approximate solutions to conservation laws. Arch Ration Mech Anal, 1983, 82:27-70
[4] Ding X X, Chen G Q, Luo P Z. A supplement to the papers convergence of the Lax-Friedrichs scheme for isentropic gas dynamics (Ⅱ)-(Ⅲ). Acta Math Sci, 1989, 9(1):43-44
[5] Ding X X, Chen G Q, Luo P Z. Convergence of the fractional step Lax-Friedrichs scheme and Godunov scheme for the isentropic system of gas dynamics. Commun Math Phys Anal, 1989, 121:63-84
[6] Barles G, Souganidis P E. Convergence of approximation schemes for fully nonlinear second order equations. Asymototic Anal, 1991, 4(3):271-283
[7] Lions P L, Perthame B, Souganidis P E. Existence and stability of entropy solutions for the hyperbolic systems of isentropic gas dynamics in Eulerian and Lagrangian coordinates. Commun Pure Appl Math, 1996, 49(6):599-638
[8] Lions P L, Perthame B, Tadmor E. Kinetic formulation of the isentropic gas dynamics and p-systems. Commun Math Phys Anal, 1994, 163(2):415-431
[9] Huang F M, Wang Z. Convergence of viscosity solutions for isothermal gas dynamics. SIAM J Math Anal, 2002, 34(3):595-610
[10] Li J Q, Sheng W C, Zhang T, et al. Two-dimensional Riemann problems:from scalar conservation laws to compressible Euler equations. Acta Math Sci, 2009, 29(4):777-802
[11] Lu Y G. Convergence of the viscosity method for a nonstrictly hyperbolic system. Acta Math Sci, 1992, 12(2):230-239
[12] Frid H. Invariant regions under Lax-Friedrichs scheme for multidimensional systems of conservation laws. Discrete Contin Dyn Syst, 1995, 1(4):585-593
[13] Frid H. Maps of convex sets and invariant regions for finite-difference systems of conservation laws. Arch Ration Mech Anal, 2001, 160(3):245-269
[14] Tadmor E. A minimum entropy principle in the gas dynamics equations. Appl Numer Math, 1986, 2(3/5):211-219
[15] Chueh K N, Conley C C, Smoller J A. Positively invariant regions for systems of nonlinear diffusion equations. Indiana Univ Math J, 1977, 26(2):373-392
[16] Jiang W F, Wang Z. The invariant region for the equations of nonisentropic gas dynamics. ANZIAM J, 2017, 58(3/4):428-435
[17] Smoller J. Shock Waves and Reaction-Diffusion Equations. Springer, 2012
Options
Outlines

/