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Phys. Fluids 18, 027106 (2006); doi:10.1063/1.2174567 (8 pages)
First and second type self-similar solutions of implosions and explosions containing ultrarelativistic shocks
(Received 27 December 2005; accepted 12 January 2006; published online 24 February 2006)
. In addition we find new, hollow (with evacuated interior), first type solutions that may be applicable for 4<k<17/4. This “sequence” with increasing k of first type solutions, hollow first type solutions, and then second type solutions is reminiscent of the nonrelativistic sequence. However, although in the nonrelativistic case there is a range of k which corresponds to a “gap”—a range in k with neither first nor second type solution which separates the hollow first type solutions and the second type solutions, here there is an “overlap”: a range of k for which current considerations allow for both hollow first and second type solutions. Further understanding is needed to determine which of the two solutions apply in this overlap regime. We provide similar exploration for the other geometries and for imploding configurations. Interestingly, we find a gap for imploding spherical shocks and exploding planar shocks and an overlap for imploding planar solutions. Cylindrical configurations have no hollow solutions and exhibit a direct transition from first type to second type solutions, without a gap or an overlap region.© 2006 American Institute of Physics
Article Outline
- INTRODUCTION
- THE SELF-SIMILAR EQUATIONS IN ARBITRARY DIMENSIONS
- FIRST TYPE SOLUTIONS
- SECOND TYPE SOLUTIONS
- THE TYPE-I TO TYPE-II TRANSITION
- DISCUSSION
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