Hostname: page-component-848d4c4894-cjp7w Total loading time: 0 Render date: 2024-06-25T14:11:41.586Z Has data issue: false hasContentIssue false

Normal shock-wave structure in two-phase vapour-droplet flows

Published online by Cambridge University Press:  26 April 2006

J. B. Young
Affiliation:
Whittle Laboratory, University of Cambridge, Madingley Road, Cambridge, CB3 0DY, UK
A. Guha
Affiliation:
Whittle Laboratory, University of Cambridge, Madingley Road, Cambridge, CB3 0DY, UK

Abstract

A study of the structure of stationary, fully and partly dispersed, normal shock waves in steady vapour–droplet, two-phase flow is presented. Pure substances only are considered, but, unlike most previous work, the droplet population is allowed to be polydispersed. It is shown how the effects of thermal relaxation for such a mixture can be elegantly incorporated into the analysis.

Three types of fully dispersed wave are identified. Type I waves are dominated by thermal relaxation and an approximate analytical solution is presented which gives results in close agreement with accurate numerical solutions of the governing equations. The analysis predicts some unexpected behaviour of the thermodynamic variables and demonstrates the correct scaling parameters for such flows. An approximate analysis is also presented for Type II waves, dominated by both velocity and thermal relaxation. Type III waves, where all three relaxation processes are important, are of little practical significance and are only briefly discussed. Partly dispersed waves are also considered and the results of a numerical simulation of the relaxation zone are presented. A linearized solution of this problem is possible but, unlike other relaxing gas flows, does not give good agreement with the more exact numerical calculations.

The apparent discontinuity in the speed of sound in a vapour–droplet mixture as the wetness fraction tends to zero has been responsible for some confusion in the literature. This problem is reconsidered and it is shown that the transition from the two-phase equilibrium to the single-phase frozen shock wave speed is continuous.

Type
Research Article
Copyright
© 1991 Cambridge University Press

Access options

Get access to the full version of this content by using one of the access options below. (Log in options will check for institutional or personal access. Content may require purchase if you do not have access.)

References

Bakhtar, F. & Tochai, M. 1980 An investigation of two-dimensional flows of nucleating and wet steam by the time-marching method. Intl J. Heat Fluid Flow, 2, 518.Google Scholar
Bakhtar, F. & Yousif, F. H. 1974 Behaviour of wet steam after disruption by a shock wave. Symp. on Multi-Phase Flow Systems, University of Strathcyde, Paper G3. Inst. Chem. Engrs.
Barschdorff, D. 1970 Droplet formation, influence of shock waves and instationary flow patterns by condensation phenomena at supersonic speeds. Proc. 3rd Intl Conf. on Rain Erosion and Associated Phenomena, R.A.E., Farnborough, pp. 691705.
Becker, E. & Bohme, G. 1969 In Nonequilibrium Flows, vol. 1 (ed. P. P. Wegener), chap. 2.
Cole, J. E. & Dobbins, R. A. 1970 Propagation of sound through atmospheric fog. J. Atmos. Sci. 27, 426434.Google Scholar
Cunningham, E. 1910 On the velocity of steady fall of spherical particles through fluid medium.. Proc. R. Soc. Lond. A 83, 357365.Google Scholar
Goossens, H. W. J., Cleijne, J. W., Smolders, H. J. & Dongen, M. E. H. van 1988 Shock wave induced evaporation of water droplets in a gas-droplet mixture. Exp. Fluids 6, 561568.Google Scholar
Gumerov, N. A., Ivandaev, A. I. & Nigmatulin, R. I. 1988 Sound waves in monodisperse gas—particle or vapour—droplet mixtures. J. Fluid Mech. 193, 5374.Google Scholar
Gyarmathy, G. 1964 Bases for a theory for wet steam turbines. Bull. 6 Inst. for Thermal Turbomachines, Federal Technical University, Zurich.Google Scholar
Gyarmathy, G. 1976 In Two-Phase Steam Flow in Turbines and Separators (ed. M. J. Moore & C. H. Sieverding), chap. 3. Hemisphere.
Jackson, R. & Davidson, B. J. 1983 An equation set for non-equilibrium two-phase flow, and an analysis of some aspects of chocking, acoustic propagation, and losses in low pressure wet steam, Intl J. Multiphase Flow 9, 491510.Google Scholar
Konorski, A. 1971 Shock waves in wet steam flow. PIMP (Trans. Inst. Fluid Flow Machinery, Polish Acad. Sci.) 57, 101109.Google Scholar
Labuntsov, D. A. & Kryukov, A. D. 1979 Analysis of intensive evaporation and condensation. Intl J. Heat Mass Transfer 22, 9891002.Google Scholar
Marble, F. E. 1969 Some gas dynamic problems in the flow of condensing vapours, Astronautica Acta 14, 585614.Google Scholar
Moheban, M. & Young, J. B. 1985 A study of thermal nonequilibrium effects in low-pressure wet steam turbines using a blade-to-blade time-marching technique. Intl J. Heat Fluid Flow 6, 269278.Google Scholar
Mozurkewich, M. 1986 Aerosol growth and the condensation coefficient for water: A review. Aerosol Sci. Technol. 5, 223236.Google Scholar
Petr, V. 1973 Variation of sound velocity in wet steam. Wet Steam 4, Conf., University of Warwick, April 1973, pp. 1720. Inst. Mech. Engrs.
Petr, V. 1979 Non-linear wave phenomena in wet steam. Eighth Conf. on Steam Turbines of Large Output, Plsen, pp. 248265.
Schnerr, G. 1989 2-D transonic flow with energy supply by homogeneous condensation: onset condition and 2-D structure of steady Laval Nozzle flow. Exp. Fluids 7, 145156.Google Scholar
Skillings, S. A. 1989 Condensation phenomena in a turbine blade passage. J. Fluid Mech. 200, 409424.Google Scholar
Vincenti, W. G. & Kruger, C. H. 1965 Introduction to Physical Gas dynamics, Chap. 8. R. E. Kreiger.
Young, J. B. 1982 The spontaneous condensation of steam in supersonic nozzles. PhysicoChem. Hydrodyn. 3, 5782.Google Scholar
Young, J. B. 1984 Semi-analytical techniques for investigating thermal non-equilibrium effects in wet steam turbines. Intl J. Heat Fluid Flow, 5, 8191.Google Scholar