Wave splitting in a fluid of large heat capacity

Author:

Thompson Philip A.,Craves Humberto,Meier G. E. A.,Kim Yoon-Gon,Speckmann H.-D.

Abstract

The splitting of a single pressure discontinuity into a propagating two-wave system is studied for the case of saturated-liquid expansion (liquid-evaporation wave splitting) and vapour compression (vapour-condensation wave splitting). Experimental results from the Max-Planck-Institut für Strömungsforschung and from Rensselaer Polytechnic Institute show that splitting occurs in test fluids of large molar heat capacity, such as iso-octane (Cv0/R≈ 37). Each of the two forms of splitting results in a single-phase forerunner wave carrying a pressure discontinuity followed by a phase-change wave, also with a pressure discontinuity. The thermodynamic state between the forerunner wave and the phase-change wave is metastable (supersaturated liquid or vapour). The waves are quantitatively described by systems of adiabats, e.g. shock adiabats. It appears that nucleation processes are predominantly homogeneous.In vapour-compression shock-wave splitting, a combined wave (liquefaction shock) splits into discrete forerunner and condensation waves at a triple point, the intersection of a liquefaction shockfront, forerunner shock and condensation discontinuity: such a point occurs just at critical supersaturation (i.e. the Wilson-line state), where condensation is spontaneous and immediate. For shock waves that produce a metastable state of subcritical supersaturation, condensation is delayed, that is, the condensation discontinuity propagates more slowly; for a split-shock system, the condensation discontinuity propagates subsonically. The pressure amplitude of a real split-shock system is much larger than that predicted by an equilibrium model.In liquid-evaporation wave splitting, the forerunner wave is an acoustic expansion wave and the second wave an evaporation wave with a propagation velocity approximately determined by the Chapman-Jouguet condition for deflagration. Such evaporation wavefronts are increasingly distinct as the temperature approaches the critical-point value. The evaporation rates across the wavefront are comparable to those found in vapour explosions.

Publisher

Cambridge University Press (CUP)

Subject

Mechanical Engineering,Mechanics of Materials,Condensed Matter Physics

Reference31 articles.

1. Thompson, P. A. & Kim, Y.-G. 1983 Direct observation of shock splitting in a vapor-liquid system.Phys. Fluids 26,3211–3215.

2. Dettleff, G. , Meier, G. E. A. , Speckmann, H.-D. , Thompson, P. A. & Yoon, C. 1982 Experiments in shock liquefaction. InProc. 13th Intl Symp. on Shock Tubes and Waves (ed. C. E. Trainor & J. G. Hall ), pp.616–623.State University of New York Press,Albany.

3. Lighthill, M. J. 1956 Viscosity effects in sound waves of finite amplitude. InSurveys in Mechanics (ed. G. K. Batchelor & R. M. Davis ), pp.250–351.Cambridge University Press.

4. Shepherd, J. E. & Sturtevant, B. 1982 Rapid evaporation at the superheat limit.J. Fluid Mech. 121,379–402.

5. Chaves, H. 1980 Verdampfungswellen in retrograden Flüssigkeiten.Diplomarbeit, Georg-August-Universität.Göttingen.

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