2011
DOI: 10.1016/j.proci.2010.06.160
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Experimental study of detonation in a cryogenic two-phase H2–O2 flow

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Cited by 4 publications
(3 citation statements)
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“…This result leads to an important conclusion: a strong detonation blast may be initiated by a spark or injection of hot gas in an aerosol mixture, not just by a strong shock wave, as is the case for gaseous mixtures [8]. Note that this conclusion has been confirmed in the very recent studies of detonation initiation in two-phase GH2/ LOx mixtures [17]. Also note that the maximum pressure of the aerosol detonation wave can even exceed that of the detonation wave in gas mixtures.…”
Section: Deflagration-to-detonation Transition In Unconfined Aerosmentioning
confidence: 57%
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“…This result leads to an important conclusion: a strong detonation blast may be initiated by a spark or injection of hot gas in an aerosol mixture, not just by a strong shock wave, as is the case for gaseous mixtures [8]. Note that this conclusion has been confirmed in the very recent studies of detonation initiation in two-phase GH2/ LOx mixtures [17]. Also note that the maximum pressure of the aerosol detonation wave can even exceed that of the detonation wave in gas mixtures.…”
Section: Deflagration-to-detonation Transition In Unconfined Aerosmentioning
confidence: 57%
“…The laminar flame speed, which is determined by the conductive heat transfer in a quiescent gas, can be estimated as v D L D ∕τ burn κ air R burn ∕C air ρ air p ≃ 1.5 ÷ 2 m∕s where τ burn R −1 burn τ H2 ≃ 3 × 10 −6 s is the typical reaction time for the GH2/GOx/GN2 mixtures. Here we took advantage of a simplified model that takes into account that in the parameter regime of interest the reaction rate is mainly limited by the initiation reactions H 2 O 2 → OH OH and H 2 O 2 → HO 2 H [17]. The rate of these reactions may be written as R burn ATC H2 C Ox ≡ C H2 ∕τ burn [18] where AT 5.5 × 10 7 exp−19680∕T 0.74T 2.43 exp−26926∕T m 3 ∕mol • s and T is in degrees Kelvin.…”
Section: A Detonation and Deflagration Waves In Unconfined Gaseous Gmentioning
confidence: 99%
“…Therefore, we have to verify that the measurements of the head pressure can be used to infer pressure at an arbitrary location of the hole along the rocket axis. To do so we simulate the model of internal ballistics of the SRM in the off-nominal regime with the case breach area dynamics given by (17) at arbitrary location. The results of such simulations for the case breach at the middle of the SRM are shown in the Figure 8.…”
Section: Modeling Case Breach Faultmentioning
confidence: 99%