By P. Manneville, H. R. Brand, J. E. Wesfreid (auth.), Dr. José E. Wesfreid, Dr. Helmut R. Brand, Dr. Paul Manneville, Dr. Gilbert Albinet, Professor Nino Boccara (eds.)
Macroscopic physics offers us with an exceptional number of pattern-forming structures showing propagation phenomena, from reactive fronts in combustion, to wavy constructions in convection and to shear movement instabilities in hydrodynamics. those lawsuits list development during this swiftly increasing box. The contributions have the next significant topics: - the issues of speed choice and entrance morphology of propagating interfaces in multiphase media, with emphasis on fresh theoretical and experimental effects on dendritic crystal development, Saffman-Taylor fingering, directional solidification and chemical waves. - The "unfolding" of large-scale, low-frequency habit in weakly constrained homogeneous structures pushed faraway from equilibrium, and extra in particular, the envelope method of the mathematical description of textures in numerous situations: regular cells, propagating waves, structural defects, and section instabilities. - the consequences of the presence of worldwide downstream delivery in open flows for the character, convective or absolute, of shear circulation instabilities, with functions to genuine boundary layer flows or shear layers, as suggested in contributions overlaying experimental occasions of primary and/or engineering interest.
Read or Download Propagation in Systems Far from Equilibrium: Proceedings of the Workshop, Les Houches, France, March 10–18, 1987 PDF
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Additional resources for Propagation in Systems Far from Equilibrium: Proceedings of the Workshop, Les Houches, France, March 10–18, 1987
Sample text
The flrst branch (n=O), which correspond to the fastest solution, is the only one not unstable /9,10/. It is characterized at small e by G /2 = Go e 7/4 ; (19) Go is a number of order unity. s. (19). This means that the selected velocity y* is twice as large in the one-sided model as in the symmetric one. It has been shown, both in the symmetric /20/ and the one-sided /21/ models, that the present result (19) is strictly valid for all P values. That is to say, the selected velocity should scale as p2 for all undercoolings.
Kessler, J. Koplik, and H. Levine, Pattern Selection in Fingered Growth Phenomena, to appear in Advances in Physics On Growth and Form, ed. Stanley, H. E. and Ostrowsky, N. (Dordrecht: Martinus Nijhoff G. M. Homsy, Ann. Rev. Fluid Mech. 19, 271 (1987) G. 1. Sivashinsky, Ann. Rev. Fluid Mech. 15, 179 (1983) 7. 8. D. P Woodruff, The Solid-Liquid Interface (Cambridge University Press, 1973) J. S. Langer, Rev. Mod. Phys. 52, 1 (1981) 9. 10. 11. M. E. Glicksman Matl. Sci. and Engr. 65, 45 (1984) and references therein W.
49. 50. 51. 52. 53. 54. & EPS SllmmerschQol and Conference on PhysicQ-chemical Hydrodynamics, (Plenum Press, New York, 1987) M. A. Trivedi: to be published M. S. A. Turski: Acta Metall. S. Langer: Acta Metall 25, 1121 (1977) G. Dee: Physica 12D, 270 (1984) M. Kerszberg: Phys Rev B 27, 3909 (1983) M. Kerszberg: Phys Rev B 27, 6796 (1983) M. B. R. H. A. H. A. H. A. H. A. Brown: Phys Rev B 31, 5931 (1985) A. Levine: present volume Y. Couder, o. Cardoso, D. Dupuy, P. Tavernier and W. Thorn: Europhys.
