通量近似条件下广义查普利金气体方程黎曼解的浓缩和空化现象

Zhiqiang Shao, Meixiang Huang
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摘要

本文研究了存在通量近似的广义查普利金气体方程黎曼解的浓缩和空化现象。集中和空化是流体动力学中的基本物理现象,可分别用三角冲击波和真空(或恒定密度态)进行数学描述。本文的主要目的是对三角冲击波和恒定密度态的形成进行严格研究,并观察浓缩和空化现象。首先,构造性地求解了通量近似下广义查普利金气体方程的黎曼问题。虽然该系统是严格双曲的,而且其两个特征场是真正非线性的,但在黎曼解中出现了三角冲击波。分析了三角冲击波的形成机理,即 1-冲击波曲线和 2-冲击波曲线在相平面上不相交。其次,严谨地证明了当压力消失时,通量近似下广义查普利金气体方程的黎曼解趋向于通量近似下零压流中输运方程的两种黎曼解,其中包括由加权δ测量和恒定密度状态形成的三角冲击波。
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Concentration and cavitation phenomena of Riemann solutions for the generalized Chaplygin gas equations under the flux approximation
In this paper, we investigate the concentration and cavitation phenomena of Riemann solutions for the generalized Chaplygin gas equations in the presence of flux approximation. The concentration and cavitation are fundamental and physical phenomena in fluid dynamics, which can be mathematically described by delta shock waves and vacuums (or constant density states), respectively. The main objective of this paper is to rigorously investigate the formation of delta shock waves and constant density states and observe the concentration and cavitation phenomena. First, the Riemann problem for the generalized Chaplygin gas equations under the flux approximation is solved constructively. Although the system is strictly hyperbolic and its two characteristic fields are genuinely nonlinear, the delta shock wave arises in Riemann solutions. The formation of mechanism for delta shock wave is analyzed, that is, the 1-shock wave curve and the 2-shock wave curve do not intersect each other in the phase plane. Second, it is rigorously proved that, as the pressure vanishes, the Riemann solutions for the generalized Chaplygin gas equations under the flux approximation tend to the two kinds of Riemann solutions to the transport equations in zero-pressure flow under the flux approximation, which include a delta shock wave formed by a weighted δ-measure and a constant density state.
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