1998
DOI: 10.2172/350869
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Extensions to DSD theory: Analysis of PBX 9502 rate stick data

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Cited by 24 publications
(30 citation statements)
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“…For lower detonation speeds, this extended theory gives results which are significantly different to the higher DSD theory (J. Bdzil, private communication), and which are in much better agreement with the results for front shapes and speeds from numerical simulations [14]. However, this shock-change equation based theory is essentially only a front propagation law, and one cannot reconstruct the flow field behind the shock (e.g.…”
Section: Introductionmentioning
confidence: 53%
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“…For lower detonation speeds, this extended theory gives results which are significantly different to the higher DSD theory (J. Bdzil, private communication), and which are in much better agreement with the results for front shapes and speeds from numerical simulations [14]. However, this shock-change equation based theory is essentially only a front propagation law, and one cannot reconstruct the flow field behind the shock (e.g.…”
Section: Introductionmentioning
confidence: 53%
“…corresponding to different charge diameters) do all lie close to one another or overlay, at least for sufficiently small curvatures [11][12] [13], indicating that the dynamics of curved detonation fronts in such explosives are, to leading order, well described by a single D n − κ law as predicted by the first order theory. Indeed, the D n − κ law determined from ratestick experiments for a given explosive can then be used to theoretically determine the shock front dynamics for the explosive in more complex geometries [5] [14]. For the more non-ideal explosives, however, such as PBXN 1111 and ANFOs, the D n − κ relations along individual shock fronts lie along different curves for different diameters, and these curves do not intersect or overlap [12][15] [16].…”
Section: Introductionmentioning
confidence: 99%
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