2006Ryuutai Kougaku Bumon Kouenkai kouen rombunshuu/Ryutai Kogaku Bumon Koenkai koen ronbunshuOpen access

915 Behavior of Combustion Wave induced by Propagation of Shock Wave into Premixed Gas of Hydrogen and Oxygen(2)

Norihiro KURIHARA, Tatsuya Kamiya, Tetsuro OBARA, Shigeharu OHYAGI

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Abstract

Experiments were conducted in order to investigate a behavior of combustion wave when a shock wave was propagated into a combustible premixed gas of hydrogen and oxygen. A phenomenon occurring in the premixed gas might be classified into four types, i.e. (a) the shock wave just transmitted into the gas without causing ignition in case for low-Mach number of the shock wave, (b) the gas was ignited behind the shock wave and a deflagration wave was propagated following the shock wave, (c) the deflagration wave transited to a detonation wave behind the shock wave, (d) a detonation wave was directly initiated just behind incident shock wave of high-Mach number. In this study, a shock wave produced by a detonation-driven shock tube was transmitted into a hydrogen-oxygen premixed gas varied with an equivalence ratio φ, initial pressure p_1 and Mach number of the shock wave Msi using same tube of 20 mm in diameter. As a result, the phenomena observed in the gas was classified using a cell-size λ for steady detonation wave, since the cell-size was inversely proportional to a chemical reaction rate of the gas.

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Experiments were conducted in order to investigate a behavior of combustion wave when a shock wave was propagated into a combustible premixed gas of hydrogen and oxygen. A phenomenon occurring in the premixed gas might be classified into four types, i.e. (a) the shock wave just transmitted into the gas without causing ignition in case for low-Mach number of the shock wave, (b) the gas was ignited behind the shock wave and a deflagration wave was propagated following the shock wave, (c) the deflagration wave transited to a detonation wave behind the shock wave, (d) a detonation wave was directly initiated just behind incident shock wave of high-Mach number. In this study, a shock wave produced by a detonation-driven shock tube was transmitted into a hydrogen-oxygen premixed gas varied with an equivalence ratio φ, initial pressure p_1 and Mach number of the shock wave Msi using same tube of 20 mm in diameter. As a result, the phenomena observed in the gas was classified using a cell-size λ for steady detonation wave, since the cell-size was inversely proportional to a chemical reaction rate of the gas.

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Available abstract

Experiments were conducted in order to investigate a behavior of combustion wave when a shock wave was propagated into a combustible premixed gas of hydrogen and oxygen. A phenomenon occurring in the premixed gas might be classified into four types, i.e. (a) the shock wave just transmitted into the gas without causing ignition in case for low-Mach number of the shock wave, (b) the gas was ignited behind the shock wave and a deflagration wave was propagated following the shock wave, (c) the deflagration wave transited to a detonation wave behind the shock wave, (d) a detonation wave was directly initiated just behind incident shock wave of high-Mach number. In this study, a shock wave produced by a detonation-driven shock tube was transmitted into a hydrogen-oxygen premixed gas varied with an equivalence ratio φ, initial pressure p_1 and Mach number of the shock wave Msi using same tube of 20 mm in diameter. As a result, the phenomena observed in the gas was classified using a cell-size λ for steady detonation wave, since the cell-size was inversely proportional to a chemical reaction rate of the gas.

Key concepts: Deflagration, Detonation, Shock tube, Deflagration to detonation transition, Shock wave, Mach number, Moving shock, Mach wave

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915 Behavior of Combustion Wave induced by Propagation of Shock Wave into Premixed Gas of Hydrogen and Oxygen(2) — Research Paper | ScholarLens