Fig. 16.

(a) Growth rate σ of the inflectional instability as a function of the streamwise wavenumber kx for kz = 0, N = 1, Pr = 1, , f = 0 (i.e., Ω = 1 and θ = 90°) for Re = ∞ (black), Re = 50 (blue), and Re = 10 (red). The gray dash-dot line denotes the inviscid growth rate of the inflectional instability under the traditional approximation (i.e.,
). (b,c) Growth rate σ of the inertial instability as a function of the vertical wavenumber kz for kx = 0, N = 1,
, and f = 0.5 (i.e., Ω = 2.02 and θ = 82.9°) for (b) Pr = 1 and Re = ∞ (black), Re = 1000 (blue), and Re = 500 (red), and (c) Pr = 10−6 and Re = 104 (black), Re = 5000 (blue), and Re = 1000 (red). Solid lines are numerical results, and dashed lines in (b) and (c) are asymptotic predictions from Eqs. (86) and (89), respectively.
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