1985
DOI: 10.2514/3.9113
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Theoretical and experimental study of nonadiabatic transonic shock/boundary-layer interaction

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Cited by 5 publications
(4 citation statements)
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“…The sand grain surface roughness heights of the bump surface are discretely increased from 0 (smooth) to 50 m, 580 m, and 1470 m covering the aerodynamically smooth (50 m) to fully rough (580 m and 1470 m) regimes. These particular roughness heights are also used by Inger and Gendt (1997) in their experimental study of transonic flow over a bump in a channel. The roughness is specified on the bump surface only.…”
Section: Resultsmentioning
confidence: 99%
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“…The sand grain surface roughness heights of the bump surface are discretely increased from 0 (smooth) to 50 m, 580 m, and 1470 m covering the aerodynamically smooth (50 m) to fully rough (580 m and 1470 m) regimes. These particular roughness heights are also used by Inger and Gendt (1997) in their experimental study of transonic flow over a bump in a channel. The roughness is specified on the bump surface only.…”
Section: Resultsmentioning
confidence: 99%
“…(Fluent, 2006) as well as in (Wilcox, 2002), and hence are not repeated here for brevity. In the earlier studies by Sharif (2005, 2009) (Wilcox, 2002), and the Reynolds stress transport model (RSM) (Launder, Reece and Rodi, 1975), in the computation of turbulent transonic flow over a smooth bump in a channel was evaluated against the experimental data of Liu and Squire (1988) and Inger and Gendt (1997). Some representative comparison of the predictions by different turbulence models against the experimental data of Liu and Squire (1988) is presented in Fig.…”
Section: Numerical Proceduresmentioning
confidence: 99%
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“…Holden [34] correlated results from swept interaction heat transfer experiments with the peak surface-pressure ratio, and showed that increased localized heat transfer occurs near the fin and surface intersection. Inger et al [35] investigated the effects of heat transfer on shock/boundary layer interactions for a supercritical airfoil with minimal flow separations and a freestream Mach number of 1.3. It was found that increases in surface temperature of the airfoil led to significant increases in drag and decreases in lift, compared to subcritical airfoil performance with no shock waves present.…”
Section: Interactions Which Included Thermal Transport and Convectivementioning
confidence: 99%