Modélisation de l'écoulement diphasique dans les injecteurs Diesel

168 BIBLIOGRAPHIE[116] R. SCHULZ. Entwicklung eines numerischen verfahrens zur simulation von wolkenkavitation, simulationvon wolkenkavitation. Stroemuntgstechnik, (274), 1995.[117] P.H. SCHWEITZER. Mechanism of disintegration of liquid jets. J. Apllied Physics, 8, 1937.[118] P. SMEREKA. Level set methods for two-fl uid fl ows. In Méthodes numériques pour les écoulementsdiphasiques. Ecoles CEA-EDF-INRIA, 1996.[119] M. SOMMERFELD, S. DECKER, and G. KOHNEN. Time-dependent calculation of bubble columnsbased on reynolds-averaged navier-stokes equations with k-ɛ turbulence model. In Proc. 2ndJapanese-German Symposium on multiphase fl ow, Tokyo, 1997.[120] C. SOTERIOU, R. ANDREWS, and M. SMITH. Direct injection diesel sprays and the effect ofcavitation and hydraulic fl ip on atomization. SAE paper 950080, 1995.[121] C. SOTERIOU, R. ANDREWS, and M. SMITH. Further studies of cavitation atomization in dieselinjection. SAE paper 1999-01-1486, 1999.[122] C. SOTERIOU, R. ANDREWS, M. SMITH, N. TORRES, and S. SANKHALPARA. The fl owpatterns and sprays of a variable orifice nozzle geometries for diesel injection. SAE paper 2000-01-0943, 2000.[123] C. SOTERIOU, R. ANDREWS, N. TORRES, M. SMITH, and R. KUNKULAGUNTA. Throughthe diesel nozzle hole - a journey of discovery. In ILASS - USA 2001, Dearborn, MI, USA, 2001.[124] C. SOTERIOU, R. ANDREWS, N. TORRES, M. SMITH, and R. KUNKULAGUNTA. Throughthe diesel nozzle hole - a journey of discovery ii. In ILASS - Europe 2001, Zurich, CH, 2001.[125] N. TAMAKI, M. SHIMIZU, K. NISHIDA, and H. HIROYASU. Effects of cavitation and internalfl ow on atomization of a liquid jet. Atomization and Sprays, 8 :179–197, 1998.[126] P.D. THOMAS and C.K. LOMBARD. Geometric conservation law and its application to fl owcomputations on moving grids. AIAA J., 17(10) :1030–1037, 1979.[127] K.W. THOMPSON. Time dependent boundary conditions for hyperbolic systems. Journal of computationalphysics, (68) :1–24, 1987.[128] K.W. THOMPSON. Time dependent boundary conditions for hyperbolic systems ii. Journal ofcomputational physics, (89) :439–461, 1990.[129] A. TOMIYAMA, Y. MAKINO, I. ZUN, and T. SAKAGUCHI. Bubble shape modelling for a 3dtwo-way bubble tracking method. In ICMF’98, Lyon, France, 1998.[130] G. TRYGGVASON. Direct numerical simulations of multiphase fl ows. In ICMF 2001, Saint Louis,Mi, USA, 2001.[131] H. UNVERDI and S. TRYGGVASON. A front-tracking method for viscous, incompressible, multifluid fl ow. Journal of Computational Physics, 100 :25–37, 1992.[132] A. VALLET. Contribution à la modélisation de l’atomisation d’un jet liquide haute pression. PhDthesis, Université de Rouen, 1997.[133] R. VON MISES. Berechnung von ausfl uss und überfallzahlen. Zeitschrift des Vereins deutscherIngenieure, 61, 1917.[134] WALLIS and GRAHAM. One-dimensional two-phase fl ow. Mc Graw-Hill, 1969.[135] J. WALTHER, J.K. SCHALLER, R. WIRTH, and C. TROPEA. Characterization of cavitatingfl ow fields in transparent diesel injection nozzles using fl uorescent particle image velocimetry (fpiv).In ILASS - Europe 2000, Darmstadt, Germany, 2000.[136] P. WALZEL. Advantages and limits in large scale modeling of atomizers. In ICLASS 82, pages187–194, 1982.[137] D. WARKEN and P. KREHL. Application of fl ash radiography to the study of breakup mechanismsof liquid jets into a high-density gas. In 19th International congress on high-speed photography andphotonics, 1990.[138] E. WINKLHOFER. Velocities and structure of atomizing diesel sprays. In 13th ILASS Proceedings,pages 89–93, Florence, Italie, 1997.[139] H. YAMAGUCHI. Private e-mail communication. may 1999.