1981
DOI: 10.1017/s0022112081002176
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On the transition between regular and Mach reflection in truly non-stationary flows

Abstract: Shock reflections over a convex and a concave wedge were investigated by using a 5 × 7 cm ordinary pressure-driven shock tube. Dry air was used for both the driving and driven gases. The large difference between the transition from regular (RR) to Mach reflection (MR) and that from MR to RR was observed, confirming the results obtained by Ben-Dor, Takayama & Kawauchi (1980). These results contradict all of the previous theoretical transition criteria. A new theory on the transition between RR and MR was de… Show more

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Cited by 53 publications
(33 citation statements)
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References 8 publications
(10 reference statements)
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“…There is no analytical model available so far for the reflection over cylindrical convex surfaces. A simple numerical code by Itoh, Okazaki & Itaya (1981) was found to well agree with experimental results in the range 1 < M s < 1.25.…”
Section: R1-2supporting
confidence: 54%
“…There is no analytical model available so far for the reflection over cylindrical convex surfaces. A simple numerical code by Itoh, Okazaki & Itaya (1981) was found to well agree with experimental results in the range 1 < M s < 1.25.…”
Section: R1-2supporting
confidence: 54%
“…The transition process from regular to Mach reflection, RR → MR, and the reverse process, MR → RR, over circular surfaces have been the focus of many studies over the past four decades (Ben-Dor, Takayama & Kawauchi 1980;Ben-Dor & Takayama 1981;Itoh, Okazaki & Itaya 1981;Gvozdeva, Lagutov & Fokeev 1982;Takayama & Sasaki 1983;Ben-Dor & Takayama 1986Gruber & Skews 2013). This transient problem caught the interest of many researchers due to the fact that experimental findings show significant discrepancies in the pseudo-steady predictions of the RR → MR transition position (Geva, Ram & Sadot 2013;Kleine et al 2014).…”
Section: Transient Shock Reflectionmentioning
confidence: 99%
“…If convex surfaces are used then the flows are truly non-stationary and do decay. Experiments of this type have been done by Ben-Dor et al (1980) and Itoh et al (1981). The decay of the shocks is attributed to the following expansion waves and not viscosity effects, and apparently they are also responsible for the delay in transition.…”
Section: Transition Between Regular and Irregular Wave Interactionmentioning
confidence: 99%