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Drag reduction in fish-like locomotion
498
Citations
18
References
1999
Year
EngineeringDrag ReductionExperimental ForceMechanical EngineeringMotor ControlMarine EngineeringPower MeasurementsKinesiologySoft RoboticsBiomechanicsBio-inspired RoboticsLegged RobotKinematicsHealth SciencesWing DesignMarine HydrodynamicsOcean Wave MechanicsHydromechanicsPropulsionShip HydrodynamicsApplied AerodynamicsUnderwater RobotBipedal LocomotionMechanical SystemsAeroelasticityAerodynamicsFar-field HydrodynamicsUnderwater Sensing
The fish‑like body moves with a traveling‑wave lateral motion whose amplitude increases from head to tail. The study shows that actively swimming fish‑like bodies require less power than towing a rigid body at the same speed. Experimental measurements were taken on a 1.2‑m fish‑like robot with flexible skin and a tail fin at Reynolds numbers up to 10^6, and the flow was modeled using a boundary‑integral method with a desingularized dipole sheet wake. Drag reduction depends on Strouhal number, oscillation amplitude, wavelength, fin angle and phase, with the necessary condition that the wave phase speed exceeds forward speed, and inviscid numerical power estimates agree with experiments.
We present experimental force and power measurements demonstrating that the power required to propel an actively swimming, streamlined, fish-like body is significantly smaller than the power needed to tow the body straight and rigid at the same speed U . The data have been obtained through accurate force and motion measurements on a laboratory fish-like robotic mechanism, 1.2 m long, covered with a flexible skin and equipped with a tail fin, at Reynolds numbers up to 10 6 , with turbulence stimulation. The lateral motion of the body is in the form of a travelling wave with wavelength λ and varying amplitude along the length, smoothly increasing from the front to the tail end. A parametric investigation shows sensitivity of drag reduction to the non-dimensional frequency (Strouhal number), amplitude of body oscillation and wavelength λ, and angle of attack and phase angle of the tail fin. A necessary condition for drag reduction is that the phase speed of the body wave be greater than the forward speed U . Power estimates using an inviscid numerical scheme compare favourably with the experimental data. The method employs a boundary-integral method for arbitrary flexible body geometry and motions, while the wake shed from the fish-like form is modelled by an evolving desingularized dipole sheet.
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