Laboratory observation of secondary shock formation ahead of a strongly radiative blast wave
Author(s) -
J. F. Hansen,
M. J. Edwards,
D. H. Froula,
G. Gregori,
Aaron Edens,
T. Ditmire
Publication year - 2006
Publication title -
physics of plasmas
Language(s) - English
Resource type - Journals
SCImago Journal Rank - 0.75
H-Index - 160
eISSN - 1089-7674
pISSN - 1070-664X
DOI - 10.1063/1.2168157
Subject(s) - physics , shock wave , blast wave , mach number , shock (circulatory) , moving shock , radiative transfer , mach wave , supersonic speed , mechanics , shock diamond , oblique shock , momentum (technical analysis) , shock tube , bow shock (aerodynamics) , shock waves in astrophysics , optics , medicine , finance , economics
High Mach number blast waves were created by focusing a laser pulse on a solid pin, surrounded by nitrogen or xenon gas. In xenon, the initial shock is strongly radiative, sending out a supersonic radiative heat wave far ahead of itself. The shock propagates into the heated gas, diminishing in strength as it goes. The radiative heat wave also slows, and when its Mach number drops to two with respect to the downstream plasma, the heat wave drives a second shock ahead of itself to satisfy mass and momentum conservation in the heat wave reference frame; the heat wave becomes subsonic behind the second shock. For some time both shocks are observed simultaneously. Eventually the initial shock diminishes in strength so much that it can longer be observed, but the second shock continues to propagate long after this time. This sequence of events is a new phenomenon that has not previously been discussed in the literature. Numerical simulation clarifies the origin of the second shock, and its position is consistent with an analytical estimate. © 2006 American Institute of Physics
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