Effects of air injection throat width on a non-premixed rotating detonation engine

被引:49
作者
Sun, Jian [1 ]
Zhou, Jin [1 ]
Liu, Shijie [1 ]
Lin, Zhiyong [1 ]
Lin, Wei [2 ]
机构
[1] Natl Univ Def Technol, Sci & Technol Scramjet Lab, Changsha 410073, Hunan, Peoples R China
[2] Space Engn Univ, Dept Aerosp Sci & Technol, Beijing 101416, Peoples R China
基金
中国国家自然科学基金;
关键词
Rotating detonation wave; Air injection throat width; Total mass flow rate; Propagation mode; NUMERICAL-SIMULATION; HOLLOW CHAMBER; HYDROGEN; WAVE; PERFORMANCE; COMBUSTOR; ETHYLENE; FUEL; FLOW; OPERATION;
D O I
10.1016/j.actaastro.2019.03.067
中图分类号
V [航空、航天];
学科分类号
08 ; 0825 ;
摘要
Rotating detonation engines are widely studied because of their compact configurations and high thermal cycle efficiency. For simplification, most of the numerical simulations of rotating detonation engines used premixed reactant mixtures. The rotating detonation waves under non-premixed conditions are not studied enough. The width of air injection throat is an important design parameter for a non-premixed rotating detonation engine. Here, a series of three-dimensional numerical simulations of a non-premixed rotating detonation engine with different air injection throat widths are performed. Cases with three different throat widths of 0.4 mm, 1.0 mm and 2.0 mm are calculated. The transient explicit density-based solver in ANSYS Fluent is used to perform the simulations. Detonation combustion happens in different radial domains for different air injection throat widths. When the air injection throat width is 1.0 mm, there is only one rotating detonation wave in the combustion chamber when the total mass flow rate is 272.3 g/s or 500 g/s. When the total mass flow rate is further increased to 1000 g/s, there are two co-rotating detonation waves in the combustion chamber. While for air injection throat width 0.4 mm, the transition to two-wave mode happens at a smaller total mass flow rate of 500 g/s. When the air injection throat width is too large, the interaction between the injection process and the propagating of rotating detonation wave becomes very strong, and the detonation wave quenches due to the insufficient injected reactants. The engine requires a larger total mass flow rate to sustain the continuous propagation of the rotating detonation wave.
引用
收藏
页码:189 / 198
页数:10
相关论文
共 54 条
[1]   Rotating detonation wave mechanics through ethylene-air mixtures in hollow combustors, and implications to high frequency combustion instabilities [J].
Anand, Vijay ;
George, Andrew St. ;
de Luzan, Charles Farbos ;
Gutmark, Ephraim .
EXPERIMENTAL THERMAL AND FLUID SCIENCE, 2018, 92 :314-325
[2]   Investigation of rotating detonation combustor operation with H2-Air mixtures [J].
Anand, Vijay ;
George, Andrew St. ;
Driscoll, Robert ;
Gutmark, Ephraim .
INTERNATIONAL JOURNAL OF HYDROGEN ENERGY, 2016, 41 (02) :1281-1292
[3]   Characterization of instabilities in a Rotating Detonation Combustor [J].
Anand, Vijay ;
St George, Andrew ;
Driscoll, Robert ;
Gutmark, Ephraim .
INTERNATIONAL JOURNAL OF HYDROGEN ENERGY, 2015, 40 (46) :16649-16659
[4]   Continuous detonation of a subsonic flow of a propellant [J].
Bykovskii, FA ;
Vedernikov, EF .
COMBUSTION EXPLOSION AND SHOCK WAVES, 2003, 39 (03) :323-334
[5]  
Cocks P.A.T., 2016, 54 AIAA AER SCI M 4
[6]   Numerical investigation of injection within an axisymmetric rotating detonation engine [J].
Driscoll, Robert ;
St George, Andrew ;
Gutmark, Ephraim J. .
INTERNATIONAL JOURNAL OF HYDROGEN ENERGY, 2016, 41 (03) :2052-2063
[7]   INFLUENCE OF CHEMICAL-KINETICS AND UNMIXEDNESS ON BURNING IN SUPERSONIC HYDROGEN FLAMES [J].
EVANS, JS ;
SCHEXNAYDER, CJ .
AIAA JOURNAL, 1980, 18 (02) :188-193
[8]  
Folusiak M., 2013, 24 ICDERS
[9]   Study of the ignition process in a laboratory scale rotating detonation engine [J].
Fotia, M. L. ;
Hoke, J. ;
Schauer, F. .
EXPERIMENTAL THERMAL AND FLUID SCIENCE, 2018, 94 :345-354
[10]   Large-scale hydrogen-air continuous detonation combustor [J].
Frolov, S. M. ;
Aksenov, V. S. ;
Lvanov, V. S. ;
Shamshin, I. O. .
INTERNATIONAL JOURNAL OF HYDROGEN ENERGY, 2015, 40 (03) :1616-1623