2021
DOI: 10.1103/physrevfluids.6.084607
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Effects of porous walls on near-wall supersonic turbulence

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Cited by 3 publications
(2 citation statements)
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“…The gradient of the velocity becomes large near both of the walls because the viscous shear stress is dominant due to the suppression of turbulence. The mean temperature reaches its maximum value around in all cases, as in supersonic and hypersonic channel flows (Chen & Scalo 2021 a , b ), because both of the top and bottom wall temperatures are lower than the recovery temperature, which is proportional to the Mach number squared. The mean temperature variation is strong near the wall, while the variation toward the centre of the channel is mild over .…”
Section: Resultsmentioning
confidence: 97%
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“…The gradient of the velocity becomes large near both of the walls because the viscous shear stress is dominant due to the suppression of turbulence. The mean temperature reaches its maximum value around in all cases, as in supersonic and hypersonic channel flows (Chen & Scalo 2021 a , b ), because both of the top and bottom wall temperatures are lower than the recovery temperature, which is proportional to the Mach number squared. The mean temperature variation is strong near the wall, while the variation toward the centre of the channel is mild over .…”
Section: Resultsmentioning
confidence: 97%
“…The code CFDSU has been successfully applied to several wall-bounded hypersonic flows (Sousa et al. 2019; Chen & Scalo 2021 a , b ). The solver adopts a staggered finite-difference scheme.…”
Section: Methodsmentioning
confidence: 99%