Titlebook: Dynamic Structure of Detonation in Gaseous and Dispersed Media; Anatoly A. Borissov Book 1991 Kluwer Academic Publishers 1991 Explosion.po

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Deutsche Auswärtige Kulturpolitikuce a sfightly subsonic flow relative to the wave at some point do characteristics begin to travel faster than the wave, quickly giving rise to a shock-wave. As this shock progressively moves through the wave, it transforms the structure from a weak to a ‘strong’ Zel’dovich, Von Neuman, Döring deton

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Book 1991upported by Chairman of Organizing Committee academician Prof. V.Titov from Hydrodynamics Institute, and academician Prof. V. Nakoryakov and also his Institute of Thermophysics. The main ideas discussed at the Round Table were presented in the form of papers which reflected present situation of the

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Dynamic Structure of Gaseous Detonation,aswell as numerical simulations, have confirmed the essential role of transverse waves on the propagation mechanism. Damping of the transverse waves of an established C-J detonation by acoustic absorbing walls leads to decoupling of the reaction zone from the leading shock. Absorbing walls also supp

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Theoretical Description of Direct Initiation of Detonation for One-Step Chemistry,uce a sfightly subsonic flow relative to the wave at some point do characteristics begin to travel faster than the wave, quickly giving rise to a shock-wave. As this shock progressively moves through the wave, it transforms the structure from a weak to a ‘strong’ Zel’dovich, Von Neuman, Döring deton

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The Limits of Stationary Propagation of Gaseous Detonation,tanding of many aspects of this field of knowledge. The structure of detonation wave (DW) in gaseous and heterogeneous systems, detonation initiation in chemically active media, DW behavior in nearcritical regimes of propagation and many other problems were studied during the last forty years. Some

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Propagation of Gas Explosion in Channels with Uneven Walls and in Porous Media, Tubes of 35 and 20 mm i.d. packed with river sand, gravel or metal balls and two-dimensional models of a porous medium in the form of planar channels with regular 4-fold widening and narrowing of the width were used in the experiments. The sizes of grains of the porous medium . ranged from 10. to 1