FORMATION OF SINGULARITIES AND EXISTENCE OF GLOBAL CONTINUOUS SOLUTIONS FOR THE COMPRESSIBLE EULER EQUATIONS*

被引:8
|
作者
Chen, Geng [1 ]
Chen, Gui-Qiang G. [2 ]
Zhu, Shengguo [3 ,4 ]
机构
[1] Univ Kansas, Sch Math, Lawrence, KS 66045 USA
[2] Univ Oxford, Math Inst, Oxford OX2 6GG, England
[3] Shanghai Jiao Tong Univ, Sch Math Sci, Shanghai 200240, Peoples R China
[4] Shanghai Jiao Tong Univ, MOE LSC, Shanghai 200240, Peoples R China
基金
中国国家自然科学基金; 澳大利亚研究理事会; 英国工程与自然科学研究理事会; 美国国家科学基金会;
关键词
Key words; Euler equations; nonisentropic; compressible flow; continuous solution; singularity; WAVE-PROPAGATION; GAS-DYNAMICS; SHOCK; DENSITY;
D O I
10.1137/20M1316603
中图分类号
O29 [应用数学];
学科分类号
070104 ;
摘要
We are concerned with the formation of singularities and the existence of global continuous solutions of the Cauchy problem for the one-dimensional nonisentropic Euler equations for compressible fluids. For the isentropic Euler equations, we pinpoint a necessary and sufficient condition for the formation of singularities of solutions with large initial data that allow a far-field vacuum-there exists a compression in the initial data. For the nonisentropic Euler equations, we identify a sufficient condition for the formation of singularities of solutions with large initial data that allow a far-field vacuum-there exists a strong compression in the initial data. Furthermore, we identify two new phenomena-decompression and de-rarefaction-for the nonisentropic Euler flows, different from the isentropic flows, via constructing two respective solutions. For the decompression phenomenon, we construct a first global continuous nonisentropic solution, even though the initial data contain a weak compression, by solving a backward Goursat problem, so that the solution is smooth, except on several characteristic curves across which the solution has a weak discontinuity (i.e., only Lipschitz continuity). For the de-rarefaction phenomenon, we construct a continuous nonisentropic solution whose initial data contain isentropic rarefactions (i.e., without compression) and a locally stationary varying entropy profile, for which the solution still forms a shock wave in a finite time.
引用
收藏
页码:6280 / 6325
页数:46
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