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The simplest test of detonation is the one-dimensional gamma-law rarefaction wave burn, for which a slab of material is initiated on one side and a detonation propagates to the other side. For a Chapman-Jouget detonation speed of 0.8 cm/ s, it takes 6.25 us for the detonation to travel 5 cm. The rich structure of a multi-dimensional detonation is absent in the one-dimensional test problem, and a simple rarefaction wave follows the detonation front (Fickett & Davis 1979). Expansion of material in the rarefaction depends on the boundary condition where the detonation is initiated, which is usually modeled as a freely moving surface or a moving piston. For the Mader problem, a stationary piston is used. In this case, the head of the rarefaction remains at the detonation front since the flow is sonic there, and the tail of the rarefaction is halfway between the front and the piston. This code released under LA-CC-05-101.
Density uniform mesh:
Pressure uniform mesh:
Material Speed uniform mesh:
Density adaptive mesh:
Pressure adaptive mesh:
Material Speed adaptive mesh:
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Please cite the relevant references if you publish a piece of work that use these codes, pieces of these codes, or modified versions of them. If you're nice, offer co-authorship of the publication. At best, you'll love these programs so much that you'll send great wads of cash to me. |
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