TY - JOUR
T1 - Experimental and numerical studies on detonation failure and re-initiation behind a half-cylinder
AU - Yang, Tianwei
AU - He, Qinghua
AU - Ning, Jianguo
AU - Li, Jian
N1 - Publisher Copyright:
© 2022 Hydrogen Energy Publications LLC
PY - 2022/3/22
Y1 - 2022/3/22
N2 - Mach reflection causes the re-initiation of decoupled detonation owing to changes in the boundary. A complementary series of experiments and numerical simulations, illustrating detonation failure and subsequent reinitiation processes, have been presented. Immediately across the half-cylinder, the decoupled detonation owing to the diffraction effect wave is reflected on the bottom wall to form a regular reflection, and then changes into the Mach reflection, which further determines the detonation reinitiation. Two different reinitiation modes after detonation wave diffraction were observed for the stable mixtures: the direct Mach reflection re-initiation mode and Mach reflection combined with the transverse detonation. However, for unstable detonations, a different reinitiation mode was obtained, whereby the development of intrinsic instabilities resonates with the reflection on the bottom wall, rendering the Mach reflection randomly occurring or even absent. The critical limit of detonation failure is characterized by the radius of the half-cylinder and the cell size. In addition, the transition length from regular to Mach reflection was measured to reveal the length-scale effect on the process.
AB - Mach reflection causes the re-initiation of decoupled detonation owing to changes in the boundary. A complementary series of experiments and numerical simulations, illustrating detonation failure and subsequent reinitiation processes, have been presented. Immediately across the half-cylinder, the decoupled detonation owing to the diffraction effect wave is reflected on the bottom wall to form a regular reflection, and then changes into the Mach reflection, which further determines the detonation reinitiation. Two different reinitiation modes after detonation wave diffraction were observed for the stable mixtures: the direct Mach reflection re-initiation mode and Mach reflection combined with the transverse detonation. However, for unstable detonations, a different reinitiation mode was obtained, whereby the development of intrinsic instabilities resonates with the reflection on the bottom wall, rendering the Mach reflection randomly occurring or even absent. The critical limit of detonation failure is characterized by the radius of the half-cylinder and the cell size. In addition, the transition length from regular to Mach reflection was measured to reveal the length-scale effect on the process.
KW - Cellular detonation
KW - Length scale effect
KW - Re-initiation
KW - Transverse detonation
UR - http://www.scopus.com/inward/record.url?scp=85125454008&partnerID=8YFLogxK
U2 - 10.1016/j.ijhydene.2022.01.230
DO - 10.1016/j.ijhydene.2022.01.230
M3 - Article
AN - SCOPUS:85125454008
SN - 0360-3199
VL - 47
SP - 12711
EP - 12725
JO - International Journal of Hydrogen Energy
JF - International Journal of Hydrogen Energy
IS - 25
ER -