Hydrogen/air supersonic combustion for future hypersonic vehicles

Abstract In this work, supersonic hydrogen combustion in the Hyshot II scramjet engine is investigated. In particular, fundamental physics of mixing, combustion and vorticity generation as well as the interaction between shock waves, boundary layer and heat release are analyzed by means of 3D Large Eddy Simulations (LES) using detailed chemistry. Results show very complex structures due to the interaction between the four sonic H 2 crossflow injections and the airstream flowing at M  = 2.79. A bow shock forms ahead of each H 2 injector: the interaction between bow shocks and boundary layers leads to separation zones where H 2 recirculates. In these recirculation zones, OH radicals are produced, indicating that a flame already starts upstream of the injectors and downstream of the flow separation. The formation of barrel shocks due to the H 2 expansion and recompressions is also predicted. Comparison of pressure distribution along the wall centreline at 1.3 ms shows agreement with experimental results, mostly in the first part of the combustor, where the grid is very fine. The combustion is very fast and efficient: only 12.35% of hydrogen is found unburned at the combustor exit. This confirms that burning hydrogen is efficient and feasible also in supersonic flows and therefore it is a good candidate for hypersonic airbreathing applications.

[1]  G. D. Brewer Hydrogen usage in air transportation , 1978 .

[2]  T. Poinsot Boundary conditions for direct simulations of compressible viscous flows , 1992 .

[3]  Suresh Menon,et al.  Studies of shock/turbulent shear layer interaction using Large-Eddy Simulation , 2010 .

[4]  Fractal modelling of turbulent mixing , 1999 .

[5]  Y. Tsujikawa,et al.  Performance analysis of scramjet engine with quasi-one-dimensional flow model , 1991 .

[6]  Marcel Lesieur,et al.  Turbulence in fluids , 1990 .

[7]  Claudio Bruno,et al.  Fractal modelling of turbulent combustion , 2000 .

[8]  In-Seuck Jeung,et al.  Realization of contact resolving approximate Riemann solvers for strong shock and expansion flows , 2009 .

[9]  Joseph A. Schetz,et al.  Detailed flow physics of the supersonic jet interaction flow field , 2009 .

[10]  Luca Maddalena,et al.  Complex Wall Injector Array for High-Speed Combustors , 2008 .

[11]  Ulrich Maas,et al.  Ignition processes in hydrogenoxygen mixtures , 1988 .

[12]  Christer Fureby,et al.  CFD Analysis of the HyShot II scramjet combustor , 2011 .

[13]  Effects of Jet Swirl on Mixing of a Light Gas Jet in a Supersonic Airstream , 2013 .

[14]  S. Menon,et al.  Unsteady simulations of compressible spatial mixing layers , 1998 .

[15]  Graham V. Candler,et al.  Hybrid reynolds-averaged and large-eddy simulation of normal injection into a supersonic crossflow , 2010 .

[16]  L. T. Nguyen,et al.  NASA hypersonic flight demonstrators—overview, status, and future plans , 2004 .

[17]  James C. McDaniel,et al.  Experimental investigation of a supersonic swept ramp injector using laser-induced iodine fluorescence , 1994 .

[18]  T. N. Veziroglu,et al.  Hydrogen as aviation fuel: A comparison with hydrocarbon fuels , 1997 .

[19]  Claudio Bruno,et al.  The coupling of turbulence and chemistry in a premixed bluff-body flame as studied by LES , 2004 .

[20]  Alexandre Ern,et al.  Multicomponent transport algorithms , 1994 .

[21]  Alexandre Ern,et al.  Fast and accurate multicomponent transport property evaluation , 1995 .

[22]  Turbulent Combustion Characteristics in HyShot Model Combustor with Transverse Fuel Injection , 2007 .

[23]  Antonella Ingenito,et al.  LES of the HyShot scramjet combustor , 2010 .

[24]  In-Seuck Jeung,et al.  Numerical Investigation of Transverse Hydrogen Jet into Supersonic Crossflow Using Detached-Eddy Simulation , 2010 .

[25]  C. Winter,et al.  Hydrogen in high-speed air transportation , 1990 .

[26]  G. B. Northam,et al.  Effects of hydrogen active cooling on scramjet engine performance , 1996 .

[27]  Antonella Ingenito,et al.  Physics and Regimes of Supersonic Combustion , 2010 .

[28]  S. Osher,et al.  Efficient implementation of essentially non-oscillatory shock-capturing schemes,II , 1989 .

[29]  Manfred Aigner,et al.  Numerical Investigation of Mixing and Combustion Enhancement in Supersonic Combustors by Strut Induced Streamwise Vorticity , 2008 .

[30]  F. R. Picchia,et al.  A review of chemical diffusion: Criticism and limits of simplified methods for diffusion coefficient calculation , 2008 .

[31]  C. Wilke A Viscosity Equation for Gas Mixtures , 1950 .

[32]  G. D. Brewer,et al.  AVIATION USAGE OF LIQUID HYDROGEN FUEL -- PROSPECTS AND PROBLEMS , 1976 .

[33]  Ronald K. Hanson,et al.  Time evolution and mixing characteristics of hydrogen and ethylene transverse jets in supersonic crossflows , 2006 .

[34]  B. Hjertager,et al.  On mathematical modeling of turbulent combustion with special emphasis on soot formation and combustion , 1977 .

[35]  S. Saxena,et al.  Thermal conductivity of binary, ternary and quaternary mixtures of rare gases , 1967 .