Abstract

In nature, the locomotion and maneuvering force of fish with thunniform mode crucially originate from the flapping foil as a principal component to produce thrust. Aiming to investigate the thrust performance and hydromechanical efficiency of flapping hydrofoil, a very large eddy simulation (VLES) method is introduced into dynamic mesh technique to solve the unsteady flow past flapping hydrofoil. The method can broaden the simulation of complex separated flow along with excellent compromise of accuracy and computing resources. In addition, the feasibility and validation of the method are verified to be well fit for dynamic mesh technique. The optimal propulsion performance is explored through varying the Strouhal (St) number and maximum angle of attack (α0) in an incoming flow condition of Re = 40,000. The temporal evolution of the angle of attack has a significant impact on lateral force coefficient, moment coefficient and the structure of shedding corotating vortices in the wake for high St number. The α0 exerts evident effect on the leading-edge separation. With the increase of St, the low-pressure values of suction surface become greater and the low-pressure areas become wider, hence producing more vortex-augmented thrusts and longer active time. The highest efficiency is equipped with the higher growth rate of thrust coefficient and moderate wake vortex strength. Furthermore, the temporal evolution of angle of attack has little effect, as does the leading-edge separation. In reality, an insight about high efficiency combined with high thrust should be considered in order to arrive to well-behaved propulsion system.

Highlights

  • Through thousands of years of natural selection, fish have harvested outstanding swimming performance in underwater

  • A very large eddy simulation (VLES) method is introduced into dynamic mesh technique to solve the unsteady flow past flapping hydrofoil

  • The main conclusions are summarized as following: (1) The feasibility and validation of the VLES method are verified by the Fr distribution, average thrust coefficient and hydromechanical efficiency to be well fit for dynamic mesh technique

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Summary

Introduction

Through thousands of years of natural selection, fish have harvested outstanding swimming performance in underwater. The fish generates a backward “jet” through the undulation of the body and oscillation of caudal fin when employs BCF, Body and/or Caudal fin, swimming mode. The “jet” is the essential reason of forward thrust since it changes the momentum of the fluid in the flow field, fish body is subject to the “reaction force” of the fluid. The swimmers with crescent caudal fin produced more than 90% of the propulsive force, such as shark, tuna.. The swimmers with crescent caudal fin produced more than 90% of the propulsive force, such as shark, tuna.1 These swimmers adopted thunniform swimming mode, which is considered as the most efficient swimming mode for fast swimming.. The locomotion and maneuvering force in thunniform mode crucially resulted from the flapping hydrofoil. The motion mode is in agreement with the caudal fin oscillation model of thunniform swimmers

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