To elucidate the complex rheological behavior of non-Newtonian fluids in fluidic control components, this study systematically investigates the coupled control mechanism of rheological parameters—specifically, the flow behavior index n (representing shear-thinning capability) and the consistency index K (representing global viscous resistance) —along with the oscillation chamber expansion angle (\: \: ) on the oscillation onset characteristics of a feedback fluidic oscillator. Based on unsteady numerical simulations, the topological bifurcation laws governing the evolution from “self-excited oscillation” to “steady straight jet” are revealed. The results indicate that: The strong coupling effect between the consistency index K and the flow behavior index n is the decisive factor for oscillation onset. The precise critical threshold is identified at \: n\: 0. 61 (K\: \: 0. 163) ; exceeding this threshold causes the Coanda effect to fail due to excessive viscous barriers. Two distinct states of oscillation cessation are identified: “marginal locking” and “deep locking”. For the marginal condition (n = 0. 61), increasing inlet velocity can break the viscous constraint to achieve dynamic unlocking, whereas the high-consistency condition (n = 0. 71) exhibits an irreversible deadlock state. Furthermore, the expansion angle \: \: significantly suppresses oscillation stability. Even under strong shear-thinning conditions (n = 0. 3) favorable for oscillation, an angle exceeding \: 20^\: accelerates flow degradation by weakening the wall-attachment pressure gradient. This study establishes a rheology-geometry-dynamics coupled criterion for oscillation onset, providing theoretical support for the optimization of fluidic components operating with complex working fluids.
Wang et al. (2026) studied this question.