Steady detonation waves for gases undergoing dissociation/recombination and bimolecular reactions

2004 ◽  
Vol 16 (1-2) ◽  
pp. 149-161 ◽  
Author(s):  
F. Conforto ◽  
M. Groppi ◽  
R. Monaco ◽  
G. Spiga
Keyword(s):  
Detonation Waves ◽  
Bimolecular Reactions ◽  
Steady Detonation

Steady detonation waves with losses

1985 ◽  
Vol 28 (9) ◽  
pp. 2735-2743 ◽  
Author(s):  
Manuel A. Huerta
Keyword(s):  
Detonation Waves ◽  
Steady Detonation

Steady detonation waves via the Boltzmann equation for a reacting mixture

2003 ◽  
Vol 36 (20) ◽  
pp. 5381-5398 ◽  
Author(s):  
F Conforto ◽  
R Monaco ◽  
F Sch rrer ◽  
I Ziegler
Keyword(s):  
Boltzmann Equation ◽  
Detonation Waves ◽  
The Boltzmann Equation ◽  
Steady Detonation

Magnetogasdynamic deflagration and detonation waves with ionization

1963 ◽  
Vol 16 (2) ◽  
pp. 243-261 ◽  
Author(s):  
J. B. Helliwell
Keyword(s):  
Shock Wave ◽  
Electromagnetic Field ◽  
Combustion Wave ◽  
Detonation Waves ◽  
Ionized Gas ◽  
One Dimensional ◽  
Jouguet Point ◽  
Electric And Magnetic Fields ◽  
The Waves ◽  
Steady Detonation

The propagation of a one-dimensional combustion wave into a non-ionized gas at rest in the presence of an electromagnetic field is considered when ionization of the gas occurs across either the combustion wave or a preceding shock wave. The electric and magnetic fields in the undisturbed gas ahead of the waves are mutually perpendicular and orthogonal to the direction of wave propagation. It is shown that steady detonation occurs at a point which is analogous to the Chapman-Jouguet point of ordinary gasdynamic combustion theory. Numerical calculations are made of the state of the gas between and behind the waves in two particlar models, in both of which the upstream electric field is zero. The models are then equivalent to magnetogasdynamic phenomena in a perfectly conducting gas. First, the case of steady detonation is studied. Secondly, steady deflagration in a tube, closed at one end, is discussed.

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