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We perform a comprehensive characterization of the propulsive performance of a thrust generating pitching foil over a wide range of Reynolds ( 10 Re 2000 ) and Strouhal ( $St$ ) numbers using a high-resolution viscous vortex particle method. For a given $Re$ , we show that the mean thrust coefficient CT increases monotonically with $St$ , exhibiting a sharp rise as the location of the inception of the wake asymmetry shifts towards the trailing edge. As a result, the propulsive efficiency too rises steeply before attaining a maximum and eventually declining at an asymptotic rate that is consistent with the inertial scalings of St² for CT and St³ for the mean power coefficient, with the latter scaling holding, quite remarkably, over the entire range of $Re$ . We find the existence of a sharp increase in the peak propulsive efficiency ηₘₐₓ (at a given $Re$ ) in the $Re$ range of 50 to approximately 1000, with ηₘₐₓ increasing rapidly from about 1.7 % to the saturated asymptotic value of approximately $16\,%$ . The $St$ at which ηₘₐₓ is attained decreases progressively with $Re$ towards an asymptotic limit of $0.45$ and always exceeds the one for transition from a reverse von Kármán to a deflected wake. Moreover, the drag-to-thrust transition occurs at a Strouhal number Stₜᵣ that exceeds the one for von Kármán to reverse von Kármán transition. The Stₜᵣ and the corresponding power coefficient Cp,ₜᵣ are found to be remarkably consistent with the simple scaling relationships Stₜᵣ~ Re-0.37 and Cp,ₜᵣ~ Re-1.12 that are derived from a balance of the thrust generated from the pitching motion and the drag force arising out of viscous resistance to the foil motion. The fact that the peak propulsive efficiency degrades appreciably only below Re≈ 10³ establishes a sharp lower threshold for energetically efficient thrust generation from a pitching foil. Our findings should be generalizable to other thrust-producing flapping foil configurations and should aid in establishing the link between wake patterns and energetic cost of thrust production in similar systems.
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Das et al. (2016) studied this question.
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