2018
DOI: 10.1016/j.actaastro.2018.06.025
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Experimental investigations on ethylene-air Continuous Rotating Detonation wave in the hollow chamber with Laval nozzle

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Cited by 68 publications
(6 citation statements)
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“…Among the past studies on detonation in HCCs, similarities between RDWs and the tangential combustion instability of an LRE have been mentioned [21]. Recent progress on this topic has been to investigate the feasibility of detonation in an HCC with a Laval nozzle [17] and analyze the relationship of RDWs and tangential combustion instability of an LRE based on their frequency [20,28]. From the perspective of combustion instability, 1T and 2T intrinsic acoustic frequencies (i.e., 6.24 and 10.34 kHz) of the HCC can be calculated from intrinsic acoustic frequency formula f m00 c∕2α m0 ∕R out [20], respectively, where c is computed from the initial state parameters of the H 2 -air mixture (P 0 90 kPa, T 0 288 K); the value of α m0 is the mth root of the zero-order Bessel function, 0.5861 and 0.9722 for the first-order and secondorder tangential acoustic frequencies, respectively.…”
Section: Resultsmentioning
confidence: 99%
See 1 more Smart Citation
“…Among the past studies on detonation in HCCs, similarities between RDWs and the tangential combustion instability of an LRE have been mentioned [21]. Recent progress on this topic has been to investigate the feasibility of detonation in an HCC with a Laval nozzle [17] and analyze the relationship of RDWs and tangential combustion instability of an LRE based on their frequency [20,28]. From the perspective of combustion instability, 1T and 2T intrinsic acoustic frequencies (i.e., 6.24 and 10.34 kHz) of the HCC can be calculated from intrinsic acoustic frequency formula f m00 c∕2α m0 ∕R out [20], respectively, where c is computed from the initial state parameters of the H 2 -air mixture (P 0 90 kPa, T 0 288 K); the value of α m0 is the mth root of the zero-order Bessel function, 0.5861 and 0.9722 for the first-order and secondorder tangential acoustic frequencies, respectively.…”
Section: Resultsmentioning
confidence: 99%
“…On the contrary, experimental observation demonstrated a shift from the dual-wave mode to the single-wave mode in H 2 -air propellant [14], which are two distinct mechanisms relating to the formation of RDWs in an HCC under atmospheric ambient pressure with different injection conditions [15,16]. Moreover, the Laval nozzle with optional contraction ratios [17], hydrocarbon fuel [14,17], and contrasting injection area ratio [4,13] make the stability of RDW more diverse and complicated. As for the thrust performance, simulation results reported that the absence of the inner wall does not hinder the thrust performance of RDEs [18].…”
mentioning
confidence: 99%
“…In addition, the collision of waves also contributes to the great velocity deficit. and μ = S/f , where S is standard deviation, N is the number of propagation cycles, and μ is relative standard deviation [29]. The propagation stability is negatively correlated with the combustor width in different CRD propagation modes.…”
Section: Effects Of Combustor Widthmentioning
confidence: 99%
“…The CRD wave propagated in single wave mode with relatively high velocity at 1647.92 m/s. Furthermore, Peng et al [29] achieved ethylene-air CRD with large operating range and low velocity deficit in the hollow combustor with a Laval nozzle. The highest propagation velocity reached 1915.4 m/s in single wave mode.…”
Section: Introductionmentioning
confidence: 99%
“…Currently, gaseous fuels were generally used in the studies of the hollow RDC. Wang et al (2018), Peng et al (2018), andPeng et al (2019) obtained the single-and double-rotating detonation wave in the experiments based on hydrocarbon fuels such as methane and ethylene. Analyzing the rotating detonation propagation modes, the range of stable operating conditions is significantly smaller due to the worse detonation of methane.…”
Section: Introductionmentioning
confidence: 99%