“…This is not in line with our conventional physics understanding of hypersonic boundary-layer stabilization. Actually, our findings can be evidently explained by examining the pressure distributions of the Mack second mode using a high-order accurate direct numerical simulation (DNS) [8,12]. As shown in the upper subplot of Fig.…”
Section: Therotical Analysismentioning
confidence: 70%
“…For hypersonic boundary-layer flow problems [9][10][11][12]31], the boundary condition at the wall surface is generally modeled as v w = p w /Z, where v w and p w are the vertical flow velocity and acoustic pressure at the wall, respectively. Z is the surface acoustic impedance, which depends on the properties of the wall material, mean flow characteristics at the wall surface, and flow-perturbation parameters such as wave frequency [31].…”
Section: Therotical Analysismentioning
confidence: 99%
“…Z is the surface acoustic impedance, which depends on the properties of the wall material, mean flow characteristics at the wall surface, and flow-perturbation parameters such as wave frequency [31]. Z becomes infinite for a rigid wall and is often designed to match the specific acoustic impedance of the background medium to maximize the absorption effect [11,12]. Note that, as a trapped mode within a waveguide, the sound ray of the Mack second mode is almost normal to the wall surface [32], which means the absorption reaches a maximum for the matched impedance.…”
Section: Therotical Analysismentioning
confidence: 99%
“…The half-width and depth of the cavities are b and H, respectively, with the unit-cell period being s. The porosity and aspect ratio are φ = 2b/s and A r = 2b/H, respectively. Assuming that the periodicity s is much smaller than the acoustic wavelength λ acs , the plane wave expansion method [12,29,30] can be used to derive the normalized effective surface acoustic impedance of the proposed metasurface as…”
Section: Practical Realization With Acoustic Metasurfacementioning
confidence: 99%
“…As the Mack second mode exhibits acoustic-wavelike behavior, one straightforward way to suppress its development while minimally disturbing the mean flow is to dissipate the acoustic wave energy by implementing an absorptive boundary [5,6]. Following this idea, a so-called ultrasonic absorptive coating (UAC) was proposed and optimized to obtain the required dissipation effect through the thermal and viscous boundary layers inside the narrow cavities [9][10][11][12]. Contrary to this intuitive thinking, here we show that an effective boundary with hardly any absorptive capability can still suppress the Mack second mode provided that its surface acoustic impedance approaches zero.…”
Hypersonic boundary-layer transition induced by the Mack second mode is a fundamental issue in fluid mechanics and hypersonic vehicle design, whose physics are not yet fully understood. Nevertheless, given the acoustic nature of the Mack second mode, ultrasonic absorptive coatings have been proposed to dissipate the wave energy and thus stabilize the hypersonic boundary-layer flow. We, however, show that even with little damping, the Mack second mode can be greatly suppressed by introducing an artificial boundary of near-zero surface acoustic impedance. This phenomenon can be attributed to the minimized acoustic pressure perturbation at the antinode of the Mack second mode, which prevents the surface-wavelike mode from being effectively excited. As a practical realization, we present a grooved acoustic metasurface and numerically verify its feasibility. Results reveal that the out-of-phase behavior between the incident and reflected waves at the resonant frequency minimizes the near-surface acoustic pressure, largely inhibiting the growth of the Mack second mode. Our study sheds light on the physical mechanism of the Mack second mode and opens up alternative possibilities toward full control of hypersonic boundary-layer transition with acoustic metasurfaces.
“…This is not in line with our conventional physics understanding of hypersonic boundary-layer stabilization. Actually, our findings can be evidently explained by examining the pressure distributions of the Mack second mode using a high-order accurate direct numerical simulation (DNS) [8,12]. As shown in the upper subplot of Fig.…”
Section: Therotical Analysismentioning
confidence: 70%
“…For hypersonic boundary-layer flow problems [9][10][11][12]31], the boundary condition at the wall surface is generally modeled as v w = p w /Z, where v w and p w are the vertical flow velocity and acoustic pressure at the wall, respectively. Z is the surface acoustic impedance, which depends on the properties of the wall material, mean flow characteristics at the wall surface, and flow-perturbation parameters such as wave frequency [31].…”
Section: Therotical Analysismentioning
confidence: 99%
“…Z is the surface acoustic impedance, which depends on the properties of the wall material, mean flow characteristics at the wall surface, and flow-perturbation parameters such as wave frequency [31]. Z becomes infinite for a rigid wall and is often designed to match the specific acoustic impedance of the background medium to maximize the absorption effect [11,12]. Note that, as a trapped mode within a waveguide, the sound ray of the Mack second mode is almost normal to the wall surface [32], which means the absorption reaches a maximum for the matched impedance.…”
Section: Therotical Analysismentioning
confidence: 99%
“…The half-width and depth of the cavities are b and H, respectively, with the unit-cell period being s. The porosity and aspect ratio are φ = 2b/s and A r = 2b/H, respectively. Assuming that the periodicity s is much smaller than the acoustic wavelength λ acs , the plane wave expansion method [12,29,30] can be used to derive the normalized effective surface acoustic impedance of the proposed metasurface as…”
Section: Practical Realization With Acoustic Metasurfacementioning
confidence: 99%
“…As the Mack second mode exhibits acoustic-wavelike behavior, one straightforward way to suppress its development while minimally disturbing the mean flow is to dissipate the acoustic wave energy by implementing an absorptive boundary [5,6]. Following this idea, a so-called ultrasonic absorptive coating (UAC) was proposed and optimized to obtain the required dissipation effect through the thermal and viscous boundary layers inside the narrow cavities [9][10][11][12]. Contrary to this intuitive thinking, here we show that an effective boundary with hardly any absorptive capability can still suppress the Mack second mode provided that its surface acoustic impedance approaches zero.…”
Hypersonic boundary-layer transition induced by the Mack second mode is a fundamental issue in fluid mechanics and hypersonic vehicle design, whose physics are not yet fully understood. Nevertheless, given the acoustic nature of the Mack second mode, ultrasonic absorptive coatings have been proposed to dissipate the wave energy and thus stabilize the hypersonic boundary-layer flow. We, however, show that even with little damping, the Mack second mode can be greatly suppressed by introducing an artificial boundary of near-zero surface acoustic impedance. This phenomenon can be attributed to the minimized acoustic pressure perturbation at the antinode of the Mack second mode, which prevents the surface-wavelike mode from being effectively excited. As a practical realization, we present a grooved acoustic metasurface and numerically verify its feasibility. Results reveal that the out-of-phase behavior between the incident and reflected waves at the resonant frequency minimizes the near-surface acoustic pressure, largely inhibiting the growth of the Mack second mode. Our study sheds light on the physical mechanism of the Mack second mode and opens up alternative possibilities toward full control of hypersonic boundary-layer transition with acoustic metasurfaces.
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