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Analysis of wall-pressure fluctuation sources from DNS of turbulent channel flow

Published 19 Nov 2019 in physics.flu-dyn | (1911.08534v2)

Abstract: The sources of wall-pressure fluctuations in turbulent channel flow are studied using a novel framework. The wall-pressure power spectral density (PSD) (ϕpp(ω))(\phi_{pp}(\omega)) is expressed as an integrated contribution from all wall-parallel plane pairs, ϕpp(ω)=∫−δ<sup>+δ∫−δ<sup>+δΓ(r,s,ω) dr ds\phi_{pp}(\omega)=\int_{-\delta}<sup>{+\delta}\int_{-\delta}<sup>{+\delta}\Gamma(r,s,\omega)\,\mathrm{dr}\,\mathrm{ds}, using the Green's function. Here, Γ(r,s,ω)\Gamma(r,s,\omega) is termed the net source cross spectral density (CSD) between two wall-parallel planes, y=ry=r and y=sy=s and δ\delta is the half channel height. Direct Numerical Simulation (DNS) data at friction Reynolds number of $180$ and $400$ are used to compute Γ(r,s,ω)\Gamma(r,s,\omega). Analysis of the net source CSD, Γ(r,s,ω)\Gamma(r,s,\omega) reveals that the location of dominant sources responsible for the premultiplied peak in the power spectra at ω<sup>+≈</sup>0.35\omega<sup>+\approx</sup> 0.35 and the wavenumber spectra at λ<sup>+≈</sup>200\lambda<sup>+\approx</sup> 200 is in the buffer layer at y<sup>+≈</sup>16.5y<sup>+\approx</sup> 16.5 and $18.4$ for Reτ=180Re_{\tau}=180 and $400$, respectively. The contribution from a wall-parallel plane (located at distance y<sup>+y<sup>+ from the wall) to wall-pressure PSD is log-normal in y<sup>+y<sup>+ for $\omega<sup>+&gt;0.35$. A dominant inner-overlap region interaction of the sources is observed at low frequencies. Further, the decorrelated features of the wall-pressure fluctuation sources are analyzed using spectral Proper Orthogonal Decomposition (POD). We require the modes to be orthogonal in an inner product with a symmetric positive definite kernel. Spectral POD supports the case that the net source is composed of two decorrelated components - active (dominant mode) and inactive (remaining modes). The structure represented by the dominant POD mode at the premultiplied wall-pressure PSD peak inclines in the downstream direction. At the low-frequency linear PSD peak, the dominant mode resembles a large scale vertical pattern.

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