Abstract

Self-propelled flapping foils with distinct locomotion-enabling kinematic restraints exhibit a remarkably similar Strouhal number ( $St$ )-Reynolds number ( $Re$ ) dependence. This similarity has been hypothesized to pervade diverse forms of oscillatory self-propulsion and undulatory biolocomotion; however, its genesis and implications on the energetic cost of locomotion remain elusive. Here, using high-resolution simulations of translationally free and restrained foils that self-propel as they are pitched, we demonstrate that a generality in the $St$ - $Re$ relationship can emerge despite significant disparities in thrust generation mechanics and locomotory performance. Specifically, owing to a recoil reaction induced passive heave, the fluid's inertial response to the prescribed rotational pitch, the principal source of thrust in unidirectionally free and towed configurations, ceases to produce thrust in a bidirectionally free configuration. Rather, the thrust generated from the leading edge suction mechanics self-propels a bidirectionally free pitching foil. Owing to the foregoing distinction in the thrust generation mechanics, the $St$ - $Re$ relationships for the bidirectionally and unidirectionally free/towed foils are dissimilar and pitching amplitude dependent, but specifically for large reduced frequencies, converge to a previously reported unified power law. Importantly, to propel at a given mean forward speed, the bidirectionally free foil must counteract the out-of-phase passive heave through a more intense rotational pitch, resulting in an appreciably higher power consumption over the range $10 \leq Re \leq 10^3$ . We highlight the critical role of thrust in introducing an offset in the $St$ - $Re$ relation, and through its amplification, being ultimately responsible for the considerable disparity in the locomotory performance of differentially constrained foils.

Highlights

  • Rigid foils that undergo a periodic rotational pitch and/or transverse heave exhibit an exceptional tendency to self-propel unidirectionally (Alben & Shelley 2005; Spagnolie et al 2010; Zhang, Liu & Lu 2010; Alben et al 2012; Zhu, He & Zhang 2014; Deng & Caulfield 2016; Verma et al 2017; Das, Shukla & Govardhan 2019; Lin, Wu & Zhang 2021)

  • Given the morphological and dynamical similarity between swimming fish and typical foils (Webb 1975; Triantafyllou et al 2005; Lucas, Lauder & Tytell 2020), we anticipate that the distinction in thrust generation mechanics and the extreme sensitivity of energetics to the locomotion-enabling kinematics will be observed over a wide spectrum of rigid and flexible flapping foil self-propulsion and undulatory biolocomotion

  • Through detailed simulations, we demonstrated that bidirectionally and unidirectionally free self-propelled pitching foils exhibit a stark distinction in the thrust generation mechanics and locomotory performance, and yet are governed by a remarkably similar Strouhal number (St)-Reynolds number (Re) scaling

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Summary

Introduction

Rigid foils that undergo a periodic rotational pitch and/or transverse heave exhibit an exceptional tendency to self-propel unidirectionally (Alben & Shelley 2005; Spagnolie et al 2010; Zhang, Liu & Lu 2010; Alben et al 2012; Zhu, He & Zhang 2014; Deng & Caulfield 2016; Verma et al 2017; Das, Shukla & Govardhan 2019; Lin, Wu & Zhang 2021). Our analysis supports a significant departure from this popular view in that a convergence to a unified St-Re power law occurs only in the large reduced frequency limit It is only in this large reduced frequency limit that the thrusts generated from distinct leading edge suction and added mass related mechanisms assume a considerably simpler and familiar, forcing frequency and amplitude squared dependent form. Given the morphological and dynamical similarity between swimming fish and typical foils (Webb 1975; Triantafyllou et al 2005; Lucas, Lauder & Tytell 2020), we anticipate that the distinction in thrust generation mechanics and the extreme sensitivity of energetics to the locomotion-enabling kinematics will be observed over a wide spectrum of rigid and flexible flapping foil self-propulsion and undulatory biolocomotion

Free and restrained self-propelled foil configurations
The St-Re relationship and the drag–thrust balance
C D that
Energetic cost of self-propulsion
Conclusions
Model for prediction of imposed pitch induced passive heave of a BF foil
Thrust generation mechanics of UF and BF self-propelled foils
Thrust coefficients in a UF configuration
Thrust coefficients in a BF configuration
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