1989
DOI: 10.1103/revmodphys.61.75
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The Riemann problem for fluid flow of real materials

Abstract: The Riemann problem for fluid flow of real materials is examined. An arbitrary equation of state is allowed, subject only to the physical requirements of thermodynamics. The properties of the isentropes and the shock Hugoniot loci that follow from conditions imposed on the equation of state are reviewed systematically. Important properties of these wave curves are determined by three dimensionless variables characterizing the equation of state: the adiabatic exponent y, the Gruneisen coefficient T, and the fun… Show more

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Cited by 652 publications
(569 citation statements)
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References 79 publications
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“…In the NASG formulation, the parameters b and p ∞ are considered constant, yielding simplicity while ensuring presence of the main molecular forces present in a fluid. In addition, as the formulation is close to the ideal gas expression, it facilitates the resolution of the Riemann problem (Plohr [24], Menikoff and Plohr [25], Cocchi and Saurel [26]). The Riemann problem is indeed the cornerstone of numerical methods used to solve hydrodynamic problem (see Toro [27] for example).…”
Section: Extended Nasg Eosmentioning
confidence: 99%
See 1 more Smart Citation
“…In the NASG formulation, the parameters b and p ∞ are considered constant, yielding simplicity while ensuring presence of the main molecular forces present in a fluid. In addition, as the formulation is close to the ideal gas expression, it facilitates the resolution of the Riemann problem (Plohr [24], Menikoff and Plohr [25], Cocchi and Saurel [26]). The Riemann problem is indeed the cornerstone of numerical methods used to solve hydrodynamic problem (see Toro [27] for example).…”
Section: Extended Nasg Eosmentioning
confidence: 99%
“…Convexity of the equation of state requires fulfillment of five different conditions (Godunov et al [33], Menikoff and Plohr [25] that are analyzed hereafter,…”
Section: Appendix a Convexity Of The Enasg Formulationmentioning
confidence: 99%
“…The Rankine-Hugoniot relations must be supplemented with suitable admissibility criteria in order to rule out unphysical solutions. One sufficient condition is that shock waves arise as limits of travelling-wave profiles including viscosity and heat conduction (see Menikoff & Plohr 1989;Kluwick 2001). This admissibility criterion has a direct and convenient graphical interpretation: the straight segment connecting the pre-shock and post-shock states in the P-v plane (commonly referred to as the Rayleigh line) must be located either completely above or completely below the shock adiabat centred on the pre-shock state.…”
Section: Problem Formulationmentioning
confidence: 99%
“…Isentropes in figure 1(a) intersect the liquid-vapour phase boundary along curve labelled M sat . A wide portion of the saturated vapour boundary of the fluid considered is retrograde (see Thompson, Carofano & Kim 1986;Menikoff & Plohr 1989), meaning that isentropes cross the phase boundary from the mixed towards the pure phase, in the direction of decreasing density. However, all isentropes eventually enter the two-phase region crossing a non-retrograde saturated phase boundary.…”
Section: Isentropic Flowmentioning
confidence: 99%
“…On the other hand, there are several successful methods that account for the flow wave structure through a superposition of Riemann solutions. These are local solutions of the hyperbolic equations which are composed of elementary waves (Menikoff and Plhor, 1989). These methods are based on characteristic upwind differencing and have been applied from nuclear and oil industries to solid combustion.…”
Section: Introductionmentioning
confidence: 99%