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Detonation waves in gases and in many homogeneous liquid explosives
form complex multidimensional structures characterized by detonation
cell sizes and regularities that depend on the kinetics of energy
release and the thermodynamic parameters of the system. Experimental
studies of gaseous detonations (see, for example, [1,2]) and
multidimensional numerical simulations of the detonations using
a one-step Arrhenius kinetics [3] have shown that an increase
in activation energy leads to more irregular cellular structures.
The experiments also indicate that small secondary cells can
appear inside the main structure when the activation energy
is high enough [1,2]. An analysis [4,5] of similar phenomena
in liquid explosives has shown that the secondary cells may
occur when the overdriven parts of the cellular detonation front
become unstable enough to form secondary triple points during
the time between two collisions of the primary triple-shock
configurations. Two-dimensional numerical simulations [6] confirmed
that the secondary cellular structure can exist in reactive
systems with a one-step Arrhenius kinetics and a high activation
energy. The results of numerical simulations presented here
show the evolution of the cellular detonations for different
activation energies, the formation of different types of the
secondary cells, and the influence of the diffusive transport
properties which stabilize the detonation front at small scales.
References
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