2000
DOI: 10.1016/s0010-2180(00)00134-6
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Characteristics of unstable detonations near extinction limits

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Cited by 34 publications
(15 citation statements)
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“…These values are found to be approximately 0.9V CJ , 0.79V CJ and 0.78V CJ for CH 4 + 2O 2 , C 3 H 8 + 5O 2 and C 2 H 2 + 5N 2 O, respectively. These results agree with those reported in the literature (e.g., [2,3,28]) that there is still a velocity deficit in the average velocity of the galloping detonation. The present results appear to be slight higher than those found in [2,3,28] (i.e., $0.6V CJ ).…”
Section: Wavelength and Amplitude Of The Galloping Cyclesupporting
confidence: 93%
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“…These values are found to be approximately 0.9V CJ , 0.79V CJ and 0.78V CJ for CH 4 + 2O 2 , C 3 H 8 + 5O 2 and C 2 H 2 + 5N 2 O, respectively. These results agree with those reported in the literature (e.g., [2,3,28]) that there is still a velocity deficit in the average velocity of the galloping detonation. The present results appear to be slight higher than those found in [2,3,28] (i.e., $0.6V CJ ).…”
Section: Wavelength and Amplitude Of The Galloping Cyclesupporting
confidence: 93%
“…These results agree with those reported in the literature (e.g., [2,3,28]) that there is still a velocity deficit in the average velocity of the galloping detonation. The present results appear to be slight higher than those found in [2,3,28] (i.e., $0.6V CJ ). A possible reason for such discrepancy can be due to the velocity measurement used in the present study which has limited resolution and is not obtained continuously.…”
Section: Wavelength and Amplitude Of The Galloping Cyclesupporting
confidence: 93%
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“…The above mentioned characteristics are typical near-limit phenomena. Different detonable mixtures and tube geometries exhibit slightly different nearlimit behavior [7][8][9][10][11][12][13][14]. To understand the limit phenomena, an extensive study covering a spectrum of mixture properties and tube geometries is required.…”
Section: Introductionmentioning
confidence: 99%