Introduction to Detonation TheoryThis title is part of UC Press's Voices Revived program, which commemorates University of California Press’s mission to seek out and cultivate the brightest minds and give them voice, reach, and impact. Drawing on a backlist dating to 1893, Voices Revived makes high-quality, peer-reviewed scholarship accessible once again using print-on-demand technology. This title was originally published in 1985. |
Contents
Fig 1A1 Shock driven by a constantvelocity piston | 5 |
Fig 7 | 7 |
equations of motion for compressible flow with chemical reaction with | 13 |
Fig 2B1 Initial data and the solution region determined by it | 21 |
NONREACTIVE FLOW | 24 |
Fig | 27 |
Fig 2D3 Degradation of a shock by an overtaking | 33 |
2F Continuous Steady Solutions | 39 |
Fig | 107 |
Fig 5C1 Steady deflagration | 113 |
STEADY SOLUTIONS | 116 |
Fig 6B2 Significance of the total heat release Q The constantQ | 121 |
Fig | 127 |
Fig 6C3 Rayleigh line WS for the following shock | 133 |
Fig | 145 |
Fig | 152 |
Fig 2E1 Shockchange relation | 41 |
REACTIVE FLOW | 48 |
Fig 3B1 Fixed and equilibriumcomposition curves | 50 |
Fig 3E1 Acousticwave structure in a medium at equilibrium | 65 |
Fig 3H1 Coordinate frames for the steady solution | 73 |
10 | 84 |
1 | 86 |
THE SIMPLEST DETONATION | 96 |
Fig 5A1 Allowed shock states for the instantaneousreaction | 99 |
Fig | 158 |
Fig 7A1 The original frame left and the shocktime frame | 164 |
STABILITY OF THE REACTION ZONE | 206 |
Fig | 210 |
APPENDICES | 214 |
Fig | 221 |
Fig | 229 |
Fig | 235 |
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Common terms and phrases
analog axis boundary condition boundary problem centered rarefaction wave Chapter characteristic CJ detonation CJ point coefficient compression wave consider constant critical point decay decreases deflagration denote density derivative dx/dt eigenvalue detonation eigenvalue solution endothermic equation of motion equilibrium curve equilibrium sound speed example exothermic exponentially final finite following flow frozen sound speed given gives governing equations Hugoniot integral curve intersection isentrope jump kinematic wave Laplace transform lead shock linear negative obtain one-way reaction ordinary differential equation overdriven detonation P₁ parameter perturbation phase plane physical system propagation velocity properties r₁ rate equation Rayleigh line reaction rate result separatrix shock speed shock strength shock velocity shock-time frame shown in Fig slope sonic locus standard equation steady detonation steady reaction zone steady solution strong branch subsonic supersonic tangent term transformation two-way reaction vanishes variable velocity problem viscosity wave path zero


