Detonation simulations in expanding channel with supersonic combustible mixture. (2nd March 2017)

• Record Type: Journal Article
• Authors: Chen, Weiqiang; Liang, Jianhan; Cai, Xiaodong; Lin, Zhiyong
• Is Part Of: International journal of hydrogen energy. Volume 42:Number 9(2017)
• Page Start: 6384
• Page End: 6393
• Publication Date: 2017-03-02
• Subjects: Supersonic combustible mixtures -- Expanding channel -- Hot jet initiation -- AMROC; Hydrogen as fuel -- Periodicals; Hydrogène (Combustible) -- Périodiques; Hydrogen as fuel; Periodicals; 665.81
• DOI: 10.1016/j.ijhydene.2017.01.102
• Languages: English
• ISSNs: 0360-3199

Abstract

Abstract: In order to investigate the mechanism of detonation combustion in expanding channel filled with supersonic combustible mixtures, the open-source program AMROC was adopted for high-resolution detonation simulations in a stoichiometric H2 /O2 /N2 mixture using a hot jet initiation. For the supersonic combustible mixture under the condition of pressure 6670 Pa and temperature 298 K, the hot jet with a width of 4.0 mm cannot initiate detonation directly in the 5.4° expanding channel. The jet induced bow shock continues rising up towards the incoming flow and finally forms Mach reflection. In the Mach stem, a local detonation is realized. An oblique shock deforms from the Mach stem near the wall and propagates forward with the Mach stem. The triple point between the Mach stem and the bow shock collides up and down, initiating the whole flow. The initiated detonation wave propagates forward at a relative speed of 55.9 m/s and the overdrive degree is 1.059, which indicates that the initiated detonation wave is almost a CJ detonation. The comparison of the reflecting structure between the numerical result and experimental observation indicates that the numerical result can give qualitatively correct conclusions. Highlights: Adaptive detonation simulations are conducted with a detailed reaction model in the supersonic combustible mixtures. The 4.0 mm wide hot jet cannot initiate detonation directly in the expanding channel. The detonation is realized through the Mach reflection of the hot jet induced bow shock. The numerical result is qualitatively correct by comparing with experimental observation.