2006
DOI: 10.2514/1.10512
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Shock Wave/Transitional Boundary-Layer Interactions in Hypersonic Flow

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Cited by 92 publications
(83 citation statements)
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“…We shall return to this result after we have reviewed results from DNS. From a comparison of figure 6(a,b) it is possible to identify four different zones of the interaction (as may also be inferred from previous studies such as Benay et al (2006)): (i) the undisturbed flow upstream of the SWBLI where the Stanton number distribution is unaffected by the shock impingement; (ii) a zone with significantly reduced heat transfer, dipping below the laminar boundary-layer solution; (iii) a rapid rise in heat transfer up to a maximum downstream of the shock impingement point; and (iv) a slow recovery of heat-transfer rate towards that of an equilibrium turbulent boundary layer.…”
Section: Flow Visualisation and Mean Stanton Number Distributionsmentioning
confidence: 70%
See 1 more Smart Citation
“…We shall return to this result after we have reviewed results from DNS. From a comparison of figure 6(a,b) it is possible to identify four different zones of the interaction (as may also be inferred from previous studies such as Benay et al (2006)): (i) the undisturbed flow upstream of the SWBLI where the Stanton number distribution is unaffected by the shock impingement; (ii) a zone with significantly reduced heat transfer, dipping below the laminar boundary-layer solution; (iii) a rapid rise in heat transfer up to a maximum downstream of the shock impingement point; and (iv) a slow recovery of heat-transfer rate towards that of an equilibrium turbulent boundary layer.…”
Section: Flow Visualisation and Mean Stanton Number Distributionsmentioning
confidence: 70%
“…The environment is often of high background noise level, mainly due to sound radiation from turbulent boundary layers on nozzle walls, although some facilities have been designed to be quiet by the use of boundary-layer bleeds (see Schneider 2008 for a review). A study of transition with SWBLI was presented by Benay et al (2006) for a hollow cylinder flare model in the ONERA R2Ch wind tunnel at Mach 5. The stagnation pressure was varied to provide cases that were fully laminar, transitional and fully turbulent.…”
mentioning
confidence: 99%
“…They can cause locally increased pressure and thermal loads, cause separations and have a great influence onto the transition process. Most of the existing publications in this field deal with interactions of shock waves with turbulent boundary layers (Dupont et al 2006; Schülein 2006;Humble et al 2009; Helmer 2011;Grilli et al 2012), some handle the case of interactions of shock waves with laminar boundary layers (Boin et al 2006;Lüdeke and Sandham 2009;Brown and Boyce 2009) but investigations of the interaction between shock waves and transitional boundary layers are rare (Dolling 2001;Arnal and Delery 2004;Benay et al 2006;Vanstone et al 2013). In order to study these phenomena in detail within the framework of the ESA-TRP "laminar to turbulent transition in hypersonic flows," experiments in three different facilities using several measuring techniques have been carried out (Sandham et al 2014).…”
mentioning
confidence: 98%
“…This result is in agreement with the well-known tendencies relative to the transitional thermal loads, which are larger than the laminar ones and even larger than the turbulent ones. These have been proven by experiments performed at Onera [4] for an identical Reynolds number in natural transition or with triggered transition.…”
Section: Resultsmentioning
confidence: 81%
“…But precisely such interactions give rise to larger heat- §uxes at reattachment, even higher than those obtained in fully turbulent regime. Therefore, this transitional well-documented test case [4] achieved at Onera ¦lls a void in this domain. The third test case completes the range in cold hypersonic since it is relative to a natural fully turbulent shock wave / boundary layer interaction with transition occurring upstream of the separation.…”
Section: Discussionmentioning
confidence: 91%