| More Details: |
We study the stability of a steady Eckart streaming jet that is acoustically forced at one end of a closed cylindrical cavity and impinges the wall at the other end, where a recirculation forms. This configuration generically represents industrial processes where acoustic forcing offers a contactless means of stirring or controlling confined flows. Successfully doing so, however, requires sufficient insight into the topology of the acoustically forced flow. This raises the question of whether the base acoustic streaming jet is stable and, when not, of which alternative states emerge. Using Linear Stability Analysis (LSA) and three-dimensional nonlinear simulations, we identify the instability mechanisms and determine the nature of the bifurcations that ensue. We show that the ratio $C_R$ between the cavity and the maximum beam radii determines the dominant unstable mode. For $4 \leq C_R \leq 6$, a non-oscillatory perturbation rooted in the jet impingement triggers a supercritical bifurcation. For $C_R = 3$, the flow destabilises through a subcritical non-oscillatory bifurcation. Further reducing $C_R$ increases the shear within the flow, and gradually relocates the instability in the shear layer between impingement-induced vortices: for $C_R = 2$, an unstable travelling wave grows out of a subcritical bifurcation, which becomes supercritical for $C_R=1$. For each geometry, the nonlinear 3D simulations validate the LSA, identify the saturated nonlinear state and its stability. This study offers fundamental insight into the stability of acoustically-driven flows in general, but also opens possible pathways to either induce turbulence acoustically, or to avoid it in realistic configurations.
Comment: 34 pages, 21 figures |
