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Jaywant Arakeri

Publications and source records attributed to Jaywant Arakeri.

2 recordsLinked to original sources

Existence of three distinct scaling regimes in self-propelled rigid pitching airfoil

We investigate the effect of imposed kinematics on the self-propulsion of the NACA0015 symmetric airfoil section subject to sinusoidal pitching. We employ a rotary apparatus capable of achieving self-propulsion. A power-spring-based crank-rocker mechanism actuates the airfoil. Three distinct scaling relations emerge, which relate the self-propulsion Reynolds number $Re_s$ to the frequency Reynolds number $Re_f$, the amplitude of pitching $θ_0$, and the location of the pitching point, $p$. When pitched near the center, a \textit{linear} scaling emerges with $Re_s \sim Re_f θ_0$. When pitched near the leading edge, a \textit{power} scaling emerges with $Re_s \sim (1-2p)(Re_f θ_0)^{3/2}$ for low amplitude pitching and a \textit{separable} scaling emerges with $Re_s \sim (1-2p)^{1/2}Re_fθ_0^{1/2}$ for moderate to high amplitude pitching. These relations are consistent with the scaling relations derived from balancing inviscid thrust with viscous drag, pressure drag, and enhanced pressure drag for the \textit{power}, \textit{separable}, and \textit{linear} regimes, respectively. We find that different vortical patterns in the wake are directly correlated to the airfoil's self-propulsion speed which essentially determines the spatial separation between the shed vortices. Our findings provide a comprehensive framework for understanding the self-propulsion of rigid pitching airfoils across a wide range of parameters validated experimentally.

physics.flu-dyn↗

A self propelling clapping body

We report an experimental study of the motion of a clapping body consisting of two flat plates pivoted at the leading edge by a torsion spring. Clapping motion and forward propulsion of the body are initiated by the sudden release of the plates, initially held apart at an angle $2θ_0$. Results are presented for the clapping and forward motions, and for the wake flow field for 24 cases, where depth to length ratio ($d^* =$ 1.5, 1 and 0.5), spring stiffness per unit depth ($Kt$), body mass ($m_b$), and initial separation angle ($2θ_0 $= 45 and 60 deg) are varied. The body motion consists of a rapid forward acceleration to a maximum velocity followed by a slow retardation to nearly zero velocity. Whereas the acceleration phase involves a complex interaction between plate and fluid motions, the retardation phase is simply fluid dynamic drag slowing the body. The wake consists of either a single axis-switching elliptical vortex loop (for $d^*$ = 1 and 1.5) or multiple vortex loops (for $d^*$ = 0.5). The body motion is nearly independent of $d^*$ and most affected by variations in $θ_0$ and $Kt$. Using conservation of linear momentum and conversion of spring strain energy into kinetic energy in the fluid and body, we obtain a relation for the translation velocity of the body in terms of the various parameters. Approximately 80% of the initial stored energy is transferred to the fluid, only 20% to the body. The experimentally obtained $COT$ lies between 2 and 8.

physics.flu-dyn↗