By C. Cercignani (auth.), Professor Renée Gatignol, Professor Soubbaramayer (eds.)
ISBN-10: 3642502350
ISBN-13: 9783642502354
ISBN-10: 3642502377
ISBN-13: 9783642502378
This quantity includes the court cases of the symposium hung on Friday 6 July 1990 on the collage Pierre et Marie Curie (Paris VI), France, in honor of Professor Henri Cabannes at the social gathering of his retirement. there have been approximately 100 members from 9 nations: Canada, France, Germany, Italy, Japan, Norway, Portugal, the Netherlands, and america. a lot of his earlier scholars or his colleagues have been one of the individuals. The twenty-six papers during this quantity are written models submitted via the authors and canopy just about all the fields within which Professor Cabannes has actively labored for greater than forty-five years. The papers are awarded in 4 chapters: classical kinetic idea and fluid dynamics, discrete kinetic conception, utilized fluid mechanics, and continuum mechanics. The editors wish to take this chance to thank the beneficiant spon sors of the symposium: the collage Pierre et Marie Curie, Commissariat a l'Energie Atomique (especially Academician R. Dautray and Dr. N. Camarcat) and path des Recherches et Etudes recommendations (especially Professor P. Lallemand). Many thank you also are because of all of the contributors for making the symposium successful. eventually, we thank Professor W. Beiglbock and his group at Springer-Verlag for generating this volume.
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Additional resources for Advances in Kinetic Theory and Continuum Mechanics: Proceedings of a Symposium Held in Honor of Professor Henri Cabannes at the University Pierre et Marie Curie, Paris, France, on 6 July 1990
Example text
Mn, T /Tw) in Eq. (25) does not depend much on T /Tw, the solution M of Eq. (39) is insensitive to Twl/Tw2 and is mostly determined by Pwl/Pw2' REFERENCES 1. Y. Sone and Y. Onishi, J. Phys. Soc. Jpn. 44, 1981, (1978). 2. Y. Onishi and Y. Sone, J. Phys. Soc. Jpn. 47, 1676, (1979). 3. Y. Sone and K. Aoki, Transp. Theory Stat. Phys. 16, 189, (1987); Mem. Fac. Eng. Kyoto Univ. 49, 237, (1987). 4. Y. Sone, T. Ohwada, and K. Aoki, Phys. Fluids A 1, 1398, (1989). 5. Y. Sone, in Rarefied Gas Dynamics, edited by A.
In Sec. IV a generalization of this condition is discussed. A simple application of the fluid dynamic equation and its boundary condition is given in Sec. V. II. BASIC EQUATION The Boltzmann equation in a steady state is written in the following nondimensional form. ;7i/2) (fo/L), (1) (2) where (2RTo)1/2(j is the molecular velocity, LXi is the space rectangular coordinates, po(2RTo )-3/2 f is the velocity distribution function, Po is the reference density, To is the reference temperature, R is the gas constant per unit mass, L is the characteristic length of the system, fo is the mean free path of the reference equilibrium state at rest at density Po and temperature To,t Kn is the corresponding Knudsen number, and J(f, f) is the standard collision term.
Fac. Eng. Kyoto Univ. 49, pp. 237-248, 1987. 11. , "Temperature jump and Knudsen layer in a rarefied gas over a plane wall: Numerical analysis of the linearized Boltzmann equation for hard-sphere molecules", Phys. Fluids A 1, pp. 363-370, 1989; Erratum: Phys. 1077, 1989. 12. , "Numerical analysis of the shear and thermal creep flows of a rarefied gas over a plane wall on the basis of the linearized Boltzmann equation for hard-sphere molecules", Phys. Fluids A 1, pp. 1588-1599, 19S9. 13. , "Evaporation and condensation on a plane condensed phase: Numerical analysis ofthe linearized Boltzmann equation for hardsphere molecules", Phys.
Advances in Kinetic Theory and Continuum Mechanics: Proceedings of a Symposium Held in Honor of Professor Henri Cabannes at the University Pierre et Marie Curie, Paris, France, on 6 July 1990 by C. Cercignani (auth.), Professor Renée Gatignol, Professor Soubbaramayer (eds.)
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