Prologue.
I. Shortcomings in the macroscopic plane-wave mode l of detonation.
II. Impedance mirror photography of H. Dean Mallory.
III. Pressure generating mechanis.
IV. Equations.
V. Pressure sources for modeling.
VI . Rayleigh's bubble model.
VII. Losses by volume variations.
VIII. Variety of initiation modes by bubbles.
I X. Various approaches to describe bubble dynamic phenomena.
X. Sensitivity testing.
XI. Low- (LVD) and slow-velocity det onation (SVD) of liquid explosives.
XII. Low velocity detona tion of solid explosives.
XIII. Case histories. XIV.
Dipole scattering.
XV. Finite shock rise.
X VI. Void precursors.
XVII. Alterations of hugoniots by bubbl e flow.
XVIII. Critical dimensions.
XIX. Critica l diameter(s) of nitromethane (NM).
XX. Smooth and rough pre ssure fronts, dark waves and DDT.
XXI. Shock tubes.
XXII. Detonation phenomena in charges with an axial cavity.
I. Shortcomings in the macroscopic plane-wave mode l of detonation.
II. Impedance mirror photography of H. Dean Mallory.
III. Pressure generating mechanis.
IV. Equations.
V. Pressure sources for modeling.
VI . Rayleigh's bubble model.
VII. Losses by volume variations.
VIII. Variety of initiation modes by bubbles.
I X. Various approaches to describe bubble dynamic phenomena.
X. Sensitivity testing.
XI. Low- (LVD) and slow-velocity det onation (SVD) of liquid explosives.
XII. Low velocity detona tion of solid explosives.
XIII. Case histories. XIV.
Dipole scattering.
XV. Finite shock rise.
X VI. Void precursors.
XVII. Alterations of hugoniots by bubbl e flow.
XVIII. Critical dimensions.
XIX. Critica l diameter(s) of nitromethane (NM).
XX. Smooth and rough pre ssure fronts, dark waves and DDT.
XXI. Shock tubes.
XXII. Detonation phenomena in charges with an axial cavity.
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