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Direct Computation of Wall-Pressure ...
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Liu, Yi,
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Direct Computation of Wall-Pressure Fluctuations in Weakly Compressible Turbulent Wall-Bounded Flows /
Record Type:
Electronic resources : Monograph/item
Title/Author:
Direct Computation of Wall-Pressure Fluctuations in Weakly Compressible Turbulent Wall-Bounded Flows // Yi Liu.
Author:
Liu, Yi,
Description:
1 electronic resource (202 pages)
Notes:
Source: Dissertations Abstracts International, Volume: 85-12, Section: B.
Contained By:
Dissertations Abstracts International85-12B.
Subject:
Fluid mechanics. -
Online resource:
https://pqdd.sinica.edu.tw/twdaoapp/servlet/advanced?query=31235370
ISBN:
9798382723167
Direct Computation of Wall-Pressure Fluctuations in Weakly Compressible Turbulent Wall-Bounded Flows /
Liu, Yi,
Direct Computation of Wall-Pressure Fluctuations in Weakly Compressible Turbulent Wall-Bounded Flows /
Yi Liu. - 1 electronic resource (202 pages)
Source: Dissertations Abstracts International, Volume: 85-12, Section: B.
Knowledge of wall-pressure fluctuations in turbulent wall-bounded flows is important for predictions of structural vibration and noise. In this study, compressible direct numerical simulations with a sixth-order, non-dissipative finite difference scheme are employed to accurately capture the spatiotemporal characteristics of wall-pressure fluctuations in low-Mach-number turbulent wall-bounded flows. Turbulent channel flow simulations are conducted at bulk Mach numbers Mb = 0.4, 0.2 and 0.1, and friction Reynolds number Reτ = 180. In addition to the convective ridge that is virtually Mach number independent, acoustic ridges, whose magnitudes are orders of magnitude lower, are identified in the two-dimensional wavenumber-frequency spectrum. At lower frequencies, the acoustic ridges represent propagating longitudinal and oblique waves that match the theoretical predictions of two-dimensional duct modes with a uniform mean flow. They decay with decreasing Mach numbers but remain distinctly identifiable even at Mb = 0.1. At high frequencies, in contrast, no propagating waves are found, and the spectral level in the supersonic wavenumber range is broadly elevated and increases with decreasing Mach number.At Mb = 0.4, two additional simulations are carried out, one in a plane channel at Reτ = 500 to explore the Reynolds number effect, and the other in a channel with a surface hump at friction Reτ = 180 to examine the impact of surface inhomogeneity. A strong Reynolds number dependence is observed in the subconvective wavenumber region, where the spectral level shows a significant elevation with increasing Reynolds number, especially at higher frequencies. The presence of the small two-dimensional hump along the spanwise direction is shown to vastly increase the acoustic energy for both longitudinal and oblique modes as well as the broadband subconvective spectral level as a result of diffraction and turbulence generation induced by the hump.Moreover, the fluctuating wall pressure beneath a flat-plate turbulent boundary layer is investigated at M∞ = 0.4 and momentum-thickness Reynolds numbers Reθ up to 1918. The results reveal the presence of acoustic ridges associated with longitudinally propagating waves in the two-dimensional wavenumber-frequency spectra. These acoustic ridges are less prominent compared with their counterparts in the plane channel. With proper frequency scaling, the convective ridges in TBL and plane-channel flows are found to be nearly identical. A small two-dimensional surface hump is found to substantially increase the acoustic energy for the downstream propagating waves downstream of the hump, but has less impact on the upstream region.
English
ISBN: 9798382723167Subjects--Topical Terms:
528155
Fluid mechanics.
Subjects--Index Terms:
Aeroacoustics
Direct Computation of Wall-Pressure Fluctuations in Weakly Compressible Turbulent Wall-Bounded Flows /
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Knowledge of wall-pressure fluctuations in turbulent wall-bounded flows is important for predictions of structural vibration and noise. In this study, compressible direct numerical simulations with a sixth-order, non-dissipative finite difference scheme are employed to accurately capture the spatiotemporal characteristics of wall-pressure fluctuations in low-Mach-number turbulent wall-bounded flows. Turbulent channel flow simulations are conducted at bulk Mach numbers Mb = 0.4, 0.2 and 0.1, and friction Reynolds number Reτ = 180. In addition to the convective ridge that is virtually Mach number independent, acoustic ridges, whose magnitudes are orders of magnitude lower, are identified in the two-dimensional wavenumber-frequency spectrum. At lower frequencies, the acoustic ridges represent propagating longitudinal and oblique waves that match the theoretical predictions of two-dimensional duct modes with a uniform mean flow. They decay with decreasing Mach numbers but remain distinctly identifiable even at Mb = 0.1. At high frequencies, in contrast, no propagating waves are found, and the spectral level in the supersonic wavenumber range is broadly elevated and increases with decreasing Mach number.At Mb = 0.4, two additional simulations are carried out, one in a plane channel at Reτ = 500 to explore the Reynolds number effect, and the other in a channel with a surface hump at friction Reτ = 180 to examine the impact of surface inhomogeneity. A strong Reynolds number dependence is observed in the subconvective wavenumber region, where the spectral level shows a significant elevation with increasing Reynolds number, especially at higher frequencies. The presence of the small two-dimensional hump along the spanwise direction is shown to vastly increase the acoustic energy for both longitudinal and oblique modes as well as the broadband subconvective spectral level as a result of diffraction and turbulence generation induced by the hump.Moreover, the fluctuating wall pressure beneath a flat-plate turbulent boundary layer is investigated at M∞ = 0.4 and momentum-thickness Reynolds numbers Reθ up to 1918. The results reveal the presence of acoustic ridges associated with longitudinally propagating waves in the two-dimensional wavenumber-frequency spectra. These acoustic ridges are less prominent compared with their counterparts in the plane channel. With proper frequency scaling, the convective ridges in TBL and plane-channel flows are found to be nearly identical. A small two-dimensional surface hump is found to substantially increase the acoustic energy for the downstream propagating waves downstream of the hump, but has less impact on the upstream region.
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https://pqdd.sinica.edu.tw/twdaoapp/servlet/advanced?query=31235370
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