Reducing flow separation of an inclined plate via travelling waves

Abstract

Many aquatic animals propel themselves by generating backward traveling waves over their body, which is thought to reattach the flow when the wave speed ($C=\unicode[STIX]{x1D706}f$, where $\unicode[STIX]{x1D706}$ is wavelength and $f$ is frequency) is larger than the swimming speed ($U$). This has inspired the use of travelling waves, which have recently been generated at low amplitudes using smart materials, to reduce flow separation on an inclined plate. To see if low-amplitude travelling waves (amplitude approximately 0.01 of chord length $L$) can reduce the separation on an inclined plate, large-eddy simulations are performed. The simulations are carried out for Reynolds number ($Re$) 20 000 and an angle of attack of $10^{\circ }$ with different wavelengths and frequencies. The travelling waves at a low reduced frequency ($f^{\ast }=fL/U=6$ and $\unicode[STIX]{x1D706}^{\ast }=\unicode[STIX]{x1D706}/L=0.2$, where $U$ is free-stream velocity) do not affect the flow separation and aerodynamic performance compared to the flat inclined plate. Nevertheless, increasing the wave speed by increasing the reduced frequency to 20 and 30 reduces flow separation. However, increasing the wave speed by increasing the wavelength, in contrast to the common belief, does not monotonically reduce the flow separation. In fact, increasing the wave speed by increasing the wavelength from 0.15 to 0.5 at constant frequency $f^{\ast }=20$ increases the separation, but increasing from 0.5 to 1.0 and 2.0, interestingly, reduces flow separation. These observations indicate that the wave speed is not the only parameter for flow reattachment, but both wavelength and frequency individually impact flow separation by affecting two competing but interconnected mechanisms: the axial momentum, imparted onto the fluid by the undulations, tends to reattach the flow but the lateral velocity tends to detach it. In fact, increasing $f^{\ast }$ and $\unicode[STIX]{x1D706}^{\ast }$ increases both the axial momentum and the lateral velocity, which are competing to attach and detach the flow, respectively.

The Ground Effect in Anguilliform Swimming

“…At a high Re of 40,000, the wake of the swimmer becomes turbulent, whereas its boundary layer remains laminar. Therefore, the turbulent flow around the fish is modeled using a dynamic Smagorinsky LES modeling [30] which has been used and validated for simulating moving boundaries within turbulent flows [31,32]. The no-slip boundary condition on the moving boundaries of the swimmer's body is handled using the sharp-interface immersed boundary method [24,27].…”

Sugarcane Bagasse Gasification in a Downdraft Fixed-Bed Gasifier: Optimization of Operation Conditions

“…By considering two-dimensional modeling, the effects of the reactor geometry and gasification properties can be investigated along vertical and horizontal directions. Fluid flow was assumed to be steady [40][41][42] and turbulent [42][43][44][45] similar to previous studies. Feedstock entered the reactor from the upper part of the geometry, and air inlet nozzles were located on both sides of the reactor.…”

Numerical Simulations of Flow around Copepods: Challenges and Future Directions

“…The method is fully parallelized using Message Passing Interface (MPI) and Portable, Extensible Toolkit for Scientific Computation (PETSc) [48]. It has been fully validated [46,[49][50][51] and applied to a wide range of applications: vortex induced vibrations [52,53], aquatic locomotion [54][55][56][57][58][59][60][61][62][63], cardiovascular flows [64][65][66][67][68][69][70], sediment transport [71], large-eddy simulations and flow control [72][73][74][75], rheology [76,77], and copepods [4]. In the next section, some of the copepod simulations using this method are presented and discussed.…”