非混相和混相混合物的可容许状态方程

Gloria Faccanoni, H. Mathis
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引用次数: 8

摘要

研究了可压缩两相流的可容许状态方程的构造。我们研究了两种方法。在第一种方法中,混合物被视为具有复杂热力学的单一流体。大多数情况下,可用的方程是通过实验确定的,通常是不完整的方程,即我们只知道压强作为体积和温度的函数。在此,我们提出了一个基于这样一个不完整的EoS计算完整EoS的一般框架。在第二种方法中,每个阶段都由其自己的EoS来描述。根据吉布斯公式,混合熵是在平衡状态下达到最大值的相熵的总和。根据混相的不同,得到的混相熵的几何性质也不同。最后,我们解决了混合EoS与uid动态的耦合问题。介绍了非混相和混相两相混合物的均匀平衡和松弛模型(HEM和HRM)。利用混合熵的凹性保证了双曲性。
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Admissible equations of state for immiscible and miscible mixtures
This paper addresses the construction of admissible Equations of State (EoS) for compressible two-phase ows. We investigate two approaches. In the first one, the mixture is treated as a single uid with a complex thermodynamic. Most of the time the available EoS are determined experimentally and are often incomplete EoS, i.e. we know only the pressure as a function of the volume and the temperature. We present here a general framework to compute a complete EoS based on such an incomplete EoS. In the second approach, each phase is depicted by its own EoS. Following the Gibbs formalism, the mixture entropy is the sum of the phasic entropies which achieves its maximum at equilibrium. Depending on the miscibility of the mixture, one gets different geometrical properties on the resulting mixture entropy. Eventually we address the coupling of mixture EoS with the dynamic of the uid. Homogeneous Equilibrium and Relaxation Models (HEM and HRM) are introduced for an immiscible and a miscible two-phase mixture. Hyperbolicity is ensured taking advantage of the concavity properties of the mixture entropies.
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