Continuous Detonation Engine and Effects of Different Types of Nozzle on Its Propulsion Performance

The rotating propagation of a continuous detonation engine (CDE) with different types of nozzles is investigated in three-dimensional numerical simulation using a one-step chemical reaction model. Flux terms are solved by the so-called monotonicity-preserving weighted essentially non-oscillatory (MPWENO) scheme. The simulated flow field agrees well with the previous experimental results. Once the initial transient effects die down, the detonation wave maintains continuous oscillatory propagation in the annular chamber as long as fuel is continuously injected. Using a numerical flow field, the propulsion performance of a CDE is computed for four types of nozzles, namely the constant-area nozzle, Laval nozzle, diverging nozzle and converging nozzle. The gross specific impulse of the CDE ranges 1 540-1 750 s and the mass flux per square meter ranges 313-330 kg/(m2·s) for different nozzles. Among these four types of nozzles, Laval nozzle performs the best, and these parameters are 1 800 N, 1 750 s and 313 kg/(m2·s). A nozzle can greatly improve the propulsion performance.

[1]  Chi-Wang Shu,et al.  Monotonicity Preserving Weighted Essentially Non-oscillatory Schemes with Increasingly High Order of Accuracy , 2000 .

[2]  Shi Tian-yi Three-dimensional numerical simulation of continuous rotating detonation engine flowfields , 2010 .

[3]  Z. H. Chen,et al.  Numerical Investigations on the Three-dimensional Flow Patterns of the Continuous Rotation Detonation , 2009 .

[4]  P. Wolański,et al.  Fundamentals of rotating detonations , 2009 .

[5]  S. A. Zhdan,et al.  Mathematical modeling of a rotating detonation wave in a hydrogen-oxygen mixture , 2007 .

[6]  Z. Gut,et al.  Experimental research on the rotating detonation in gaseous fuels–oxygen mixtures , 2011 .

[7]  Vigor Yang,et al.  Propulsive performance of airbreathing pulse detonation engines , 2006 .

[8]  S. A. Zhdan,et al.  Continuous Spin Detonations , 2006 .

[9]  Elaine S. Oran,et al.  Two-dimensional reactive flow dynamics in cellular detonation waves , 1999 .

[10]  Wang Jian-ping,et al.  Change in Continuous Detonation Wave Propagation Mode from Rotating Detonation to Standing Detonation , 2010 .

[11]  Wei Fan,et al.  Experimental Investigation on Performance of Pulse Detonation Rocket Engine Model , 2007 .

[12]  邵业涛,et al.  Change in Continuous Detonation Wave Propagation Mode from Rotating Detonation to Standing Detonation , 2010 .

[13]  A. A. Borisov,et al.  Pulse detonation propulsion : challenges, current status, and future perspective , 2004 .

[14]  Francois Falempin,et al.  A Contribution to the Development of Actual Continuous Detonation Wave Engine , 2008 .

[15]  F. A. Bykovskii,et al.  Continuous Detonation of a Subsonic Flow of a Propellant , 2003 .

[16]  V. V. Mitrofanov,et al.  Continuous detonation combustion of fuel-air mixtures , 1997 .