Unstable combustion induced by oblique shock waves at the non-attaching condition of the oblique detonation wave

2009 ◽  
Vol 32 (2) ◽  
pp. 2387-2396 ◽  
Author(s):  
Jeong-Yeol Choi ◽  
Edward J.-R. Shin ◽  
In-Seuck Jeung
2018 ◽  
Vol 846 ◽  
pp. 411-427 ◽  
Author(s):  
Zhaoxin Ren ◽  
Bing Wang ◽  
Gaoming Xiang ◽  
Longxi Zheng

An oblique detonation wave in two-phase kerosene–air mixtures over a wedge is numerically studied for the first time. The features of initiation and stabilisation of the two-phase oblique detonation are emphasised, and they are different from those in previous studies on single-phase gaseous detonation. The gas–droplet reacting flow system is solved by means of a hybrid Eulerian–Lagrangian method. The two-way coupling for the interphase interactions is carefully considered using a particle-in-cell model. For discretisation of the governing equations of the gas phase, a WENO-CU6 scheme (Hu et al., J. Comput. Phys., vol. 229 (23), 2010, pp. 8952–8965) and a sixth-order compact scheme are employed for the convective terms and the diffusive terms, respectively. The inflow parameters are chosen properly from real flight conditions. The fuel vapour, droplets and their mixture are taken as the fuel in homogeneous streams with a stoichiometric ratio, respectively. The effects of evaporating droplets and initial droplet size on the initiation, transition from oblique shock to detonation and stabilisation are elucidated. The two-phase oblique detonation wave is stabilised from the oblique shock wave induced by the wedge. As the mass flow rate of droplets increases, a shift from a smooth transition with a curved shock to an abrupt one with a multi-wave point is found, and the initiation length of the oblique detonation increases, which is associated with the increase of the transition pressure. By increasing the initial droplet size, a smooth transition pattern is observed, even if the equivalence ratio remains constant, and the transition pressure decreases. The factor responsible is incomplete evaporation before the detonation fronts, which results in a complicated flame structure, including regimes of formation of oblique detonation, evaporative cooling of droplets and post-detonation reaction.


2013 ◽  
Vol 135 (3) ◽  
Author(s):  
Neal P. Bitter ◽  
Joseph E. Shepherd

Detonations and deflagration-to-detonation transition (DDT) are experimentally studied in horizontal pipes which are partially filled with water. The gas layer above the water is stoichiometric hydrogen–oxygen at 1 bar. The detonation wave produces oblique shock waves in the water, which focus at the bottom of the pipe due to the curvature of the walls. This results in peak pressures at the bottom of the pipe that are 4–6 times greater than the peak detonation pressure. Such pressure amplification is measured for water depths of 0.25, 0.5, 0.75, 0.87, and 0.92 pipe diameters. Focusing of the oblique shock waves is studied further by measuring the circumferential variation of pressure when the water depth is 0.5 pipe diameters, and reasonable agreement with theoretical modeling is found. Despite the local pressure amplification due to shock focusing, peak hoop strains decreased with increasing water depth. Failure of the detonation wave was not observed, even for water depths as high as 0.92 pipe diameters. Likewise, transition to detonation occurred for every water height.


2002 ◽  
Vol 24 (3) ◽  
pp. 149-157 ◽  
Author(s):  
C. A. R. Pimentel ◽  
J. L. F. Azevedo ◽  
L.F. Figueira da Silva ◽  
B. Deshaies

1987 ◽  
Author(s):  
M. OSTRANDER ◽  
J. HYDE ◽  
M. YOUNG ◽  
R. KISSINGER ◽  
D. PRATT

2021 ◽  
pp. 106964
Author(s):  
Hongbo Guo ◽  
Xiongbin Jia ◽  
Ningbo Zhao ◽  
Shuying Li ◽  
Hongtao Zheng ◽  
...  

1988 ◽  
pp. 1107-1112
Author(s):  
Shigetoshi KAWAGOE ◽  
Kazuyasu MATSUO ◽  
Soon Bum KWON ◽  
Toshiaki SETOGUCHI ◽  
Shigeru MATSUO

2021 ◽  
pp. 97-117
Author(s):  
Forrest E. Ames ◽  
Clement Tang
Keyword(s):  

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