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Optimization of the deflagration to detonation transition: reduction of length and time of transition

机译:从爆燃到爆轰过渡的优化:缩短过渡长度和时间

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摘要

The aim of this experimental investigation is the study of Deflagration to Detonation Transition (DDT) in tubes in order to (i) reduce both run-up distance and time of transition (L (DDT) and t (DDT)) in connection with Pulsed Detonation Engine applications and to (ii) attempt to scale L (DDT) with lambda(CJ) (the detonation cellular structure width). In DDT, the production of turbulence during the long flame run-up can lead to L (DDT) values of several meters. To shorten L (DDT), an experimental set-up is designed to quickly induce highly turbulent initial flow. It consists of a double chamber terminated with a perforated plate of high Blockage Ratio (BR) positioned at the beginning of a 26 mm inner diameter tube containing a "Shchelkin spiral" of BR approximate to 0.5. The study involves stoichiometric reactive mixtures of H-2, CH4, C3H8, and C2H4 with oxygen and diluted with N-2 in order to obtain the same cell width lambda(CJ) approximate to 10 mm at standard conditions. The results show that a shock-flame system propagating with nearly the isobaric speed of sound of combustion products, called the choking regime, is rapidly obtained. This experimental set-up allows a L (DDT) below 40 cm for the mixtures used and a ratio L (DDT)/lambda(CJ) ranging from 23 to 37. The transition distance seems to depend on the reduced activation energy (E (a)/RT (c)) and on the normalized heat of reaction (Q/a(0)2). The higher these quantities are, the shorter the ratio L (DDT)/lambda(CJ) is.
机译:这项实验研究的目的是研究管内的爆燃到爆轰过渡(DDT),以便(i)减少与脉冲有关的加速距离和过渡时间(L(DDT)和t(DDT))爆轰引擎的应用以及(ii)尝试用lambda(CJ)缩放L(DDT)(爆轰孔结构宽度)。在DDT中,长时间火焰燃烧期间产生的湍流可能导致L(DDT)值达到几米。为了缩短L(DDT),设计了一种实验装置来快速诱导高度湍流的初始流量。它由一个双腔室组成,该双腔室的末端是高阻塞率(BR)的多孔板,该多孔板位于内径为26 mm的管子的开始处,该管子的BR的“ Shchelkin螺旋”约为0.5。该研究涉及H-2,CH4,C3H8和C2H4与氧气的化学计量反应性混合物,并用N-2稀释,以便在标准条件下获得大约10 mm的相同单元宽度λ(CJ)。结果表明,迅速获得了一种以近似等速燃烧产物声传播的冲击火焰系统,称为窒息状态。该实验装置允许使用的混合物的L(DDT)低于40 cm,L(DDT)/ lambda(CJ)的比率范围为23至37。过渡距离似乎取决于降低的活化能(E( a)/ RT(c))和归一化反应热(Q / a(0)2)。这些数量越高,比率L(DDT)/λ(CJ)越短。

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