Fig. C.1

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Frequency power spectrum of the vertical velocity component υ extracted in the middle of the stable layer at (x, y, z) = (−0.2, 2.5, −0.2) over the time series t ∈ (10τconv, 32τconv) in the problem of turbulent convection and wave excitation described in Sec. 3.2. These results are obtained on a grid with 1283 cells, using the LHLLC Riemann solver and the CTO-WENO scheme of Kolb (2014) for different values of the parameter ε WENO occurring in the smoothness indicators of the scheme (see Sect. C), ranging from 10−12 to 102. As a reference, power spectra obtained with the numerical options LHLLC + PPM84 and LHLLC + LIN + VL are also shown. The convective turnover frequency (ωconv = 2π/τconv), the Brunt-Väisälä frequency at the location of the point probe (NBV), and the frequency of the fundamental oscillation mode of the cavity (ω0 = 1.1) are represented by the black dashed-dotted, dashed, and dotted lines, respectively.
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