In this paper, we study the pressureless limit of the Riemann solutions for a reduced two-phase mixtures model with non-isentropic logarithmic gas state. We construct the Riemann solutions using the $ p-u $ plane projection method and study the formation of delta shock waves and vacuum as the pressure vanishes. We prove that, as pressure vanishes, the limit of Riemann solutions is the Riemann solutions of the reduced 2-dimensional pressureless gas dynamics model, where the evacuation is strictly determined by the state with higher entropic stiffness. In particular, we compare the rates at which the density of the intermediate state tends to singularity, such as infinity or vacuum, when the model is with logarithmic gas, polytropic gas, and generalized Chaplygin gas as the pressure vanishes. Then, we quantitatively demonstrated that logarithmic gases can be regarded as a transitional form between polytropic gases and generalized Chaplygin gases. Finally, numerical simulations employing essentially non-oscillatory schemes with third-order Runge-Kutta methods are used to validate the theoretical convergence behaviors.
Citation: Yiming Gao, Weifeng Jiang, Chengkai Tu. Formation mechanism of concentration and entropy-related cavitation in the pressureless limit for non-isentropic logarithmic gas dynamics[J]. AIMS Mathematics, 2026, 11(8): 24033-24059. doi: 10.3934/math.2026969
In this paper, we study the pressureless limit of the Riemann solutions for a reduced two-phase mixtures model with non-isentropic logarithmic gas state. We construct the Riemann solutions using the $ p-u $ plane projection method and study the formation of delta shock waves and vacuum as the pressure vanishes. We prove that, as pressure vanishes, the limit of Riemann solutions is the Riemann solutions of the reduced 2-dimensional pressureless gas dynamics model, where the evacuation is strictly determined by the state with higher entropic stiffness. In particular, we compare the rates at which the density of the intermediate state tends to singularity, such as infinity or vacuum, when the model is with logarithmic gas, polytropic gas, and generalized Chaplygin gas as the pressure vanishes. Then, we quantitatively demonstrated that logarithmic gases can be regarded as a transitional form between polytropic gases and generalized Chaplygin gases. Finally, numerical simulations employing essentially non-oscillatory schemes with third-order Runge-Kutta methods are used to validate the theoretical convergence behaviors.
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