1. Extended Noble–Abel Stiffened-Gas Equation of State for Sub-and-Supercritical Liquid-Gas Systems Far from the Critical Point
- Author
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Alexandre Chiapolino, Richard Saurel, Laboratoire de Mécanique et d'Acoustique [Marseille] (LMA ), Centre National de la Recherche Scientifique (CNRS)-Aix Marseille Université (AMU)-École Centrale de Marseille (ECM), Recherche Scientifique et Simulation Numérique [Roquevaire] (RS2N), and Aix Marseille Université (AMU)-École Centrale de Marseille (ECM)-Centre National de la Recherche Scientifique (CNRS)
- Subjects
Materials science ,Thermodynamic equilibrium ,phase change ,Computation ,Thermodynamics ,Noble-Abel ,lcsh:Thermodynamics ,01 natural sciences ,two-phase flows ,010305 fluids & plasmas ,Critical point (thermodynamics) ,lcsh:QC310.15-319 ,0103 physical sciences ,[PHYS.MECA.MEFL]Physics [physics]/Mechanics [physics]/Fluid mechanics [physics.class-ph] ,0101 mathematics ,lcsh:QC120-168.85 ,Phase diagram ,Fluid Flow and Transfer Processes ,convexity ,Liquid gas ,Mechanical Engineering ,Condensed Matter Physics ,sub-supercritical flows ,Ideal gas ,Supercritical fluid ,010101 applied mathematics ,stiffened-gas ,[PHYS.MECA.THER]Physics [physics]/Mechanics [physics]/Thermics [physics.class-ph] ,lcsh:Descriptive and experimental mechanics ,Noble–Abel ,hyperbolic systems ,Cubic function - Abstract
International audience; The Noble-Abel-Stiffened-Gas (NASG) equation of state (Le Métayer and Saurel, 2016) is extended to variable attractive and repulsive effects to improve the liquid phase accuracy when large temperature and pressure variation ranges are under consideration. The transition from pure phase to supercritical state is of interest as well. The gas phase is considered through the ideal gas assumption with variable specific heat rendering the formulation valid for high temperatures. The liquid equation-of-state constants are determined through the saturation curves making the formulation suitable for two-phase mixtures at thermodynamic equilibrium. The overall formulation is compared to experimental characteristic curves of the phase diagram showing good agreement for various fluids (water, oxygen). Compared to existing cubic equations of state the present one is convex, a key feature for computations with hyperbolic flow models.
- Published
- 2018
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