TY - JOUR
T1 - Impact of mixture mass flux on hydrodynamic blockage ratio and Mach number of rotating detonation combustor
AU - Noda, Tomoyuki
AU - Matsuoka, Ken
AU - Goto, Keisuke
AU - Kawasaki, Akira
AU - Watanabe, Hiroaki
AU - Itouyama, Noboru
AU - Kasahara, Jiro
AU - Matsuo, Akiko
N1 - Funding Information:
This work was supported by a JSPS KAKENHI Grant Number JP20H02349 (Grant-in-Aid for Scientific Research (B), JP20K21046 (Grant-in-Aid for Exploratory Research) and JP18KK0404 (Fostering Joint International Research).
Publisher Copyright:
© 2023 IAA
PY - 2023/6
Y1 - 2023/6
N2 - To analyze non-ideal phenomena, such as burned gas backflow and non-detonation combustion, which affect the rotating detonation wave Mach number, simultaneous self-luminous visualization, time-averaged static pressure, fluctuating pressure, and thrust measurements with gaseous ethylene and oxygen were performed. Consequently, by doubling the number density of the fuel injectors, the hydrodynamic blockage ratio at the oxidizer inlet increased approximately 1.7-fold under the same oxidizer inlet area conditions. This may be attributed to the increase in the detonation propagation Mach number owing to the enhanced mixing of fuel and oxidizer. The relationship between the parasitic combustion fraction in front of the rotating detonation wave and the Mach number was also investigated by using a distributed heat release model. Consequently, it was suggested that experimental Mach number decreased from approximately 4.1 to 2.8 with increase in a mixture mass flux, and the theoretical detonation wave propagation Mach number was 7.3.
AB - To analyze non-ideal phenomena, such as burned gas backflow and non-detonation combustion, which affect the rotating detonation wave Mach number, simultaneous self-luminous visualization, time-averaged static pressure, fluctuating pressure, and thrust measurements with gaseous ethylene and oxygen were performed. Consequently, by doubling the number density of the fuel injectors, the hydrodynamic blockage ratio at the oxidizer inlet increased approximately 1.7-fold under the same oxidizer inlet area conditions. This may be attributed to the increase in the detonation propagation Mach number owing to the enhanced mixing of fuel and oxidizer. The relationship between the parasitic combustion fraction in front of the rotating detonation wave and the Mach number was also investigated by using a distributed heat release model. Consequently, it was suggested that experimental Mach number decreased from approximately 4.1 to 2.8 with increase in a mixture mass flux, and the theoretical detonation wave propagation Mach number was 7.3.
KW - Burned gas backflow
KW - Detonation mach number
KW - Non-detonation combustion
KW - Pressure gain combustion
KW - Rotating detonation combustor
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U2 - 10.1016/j.actaastro.2023.03.013
DO - 10.1016/j.actaastro.2023.03.013
M3 - Article
AN - SCOPUS:85150372237
SN - 0094-5765
VL - 207
SP - 219
EP - 226
JO - Acta Astronautica
JF - Acta Astronautica
ER -