Abstract
When multiple blasts occur at different times, the situation arises in which a blast wave is propagating into a medium that has already been shocked. Determining the evolution in the shape of the second shock is not trivial, as it is propagating into air that is not only non-uniform, but also non-stationary. To accomplish this task, we employ the method of Kompaneets to determine the shape of a shock in a non-uniform media. We also draw from the work of Korycansky (Astrophys J 398:184–189. https://doi.org/10.1086/171847, 1992) on an off-center explosion in a medium with radially varying density. Extending this to treat non-stationary flow, and making use of approximations to the Sedov solution for the point blast problem, we are able to determine an analytic expression for the evolving shape of the second shock. In particular, we consider the case of a shock in air at standard ambient temperature and pressure, with the second shock occurring shortly after the original blast wave reaches it, as in a sympathetic detonation.
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Notes
Note that it is not necessary that the sources be equal. The results of changing the source sizes will be similar to those seen by changing the time of detonation for the second source, with a larger second source being similar to a smaller \(t_0\).
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This work was funded in part by Sandia National Laboratories.
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Communicated by F. Zhang and G. Ciccarelli.
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Duncan-Miller, G.C., Stone, W.D. Off-center blast in a shocked medium. Shock Waves 28, 631–640 (2018). https://doi.org/10.1007/s00193-017-0747-3
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DOI: https://doi.org/10.1007/s00193-017-0747-3