Flow past a near-wall retrograde rotating cylinder at varying rotation and gap ratios
Autor: | Soon Keat Tan, Yalin Li, Xikun Wang, Shouqi Yuan |
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Přispěvatelé: | School of Civil and Environmental Engineering, Maritime Research Centre |
Rok vydání: | 2018 |
Předmět: |
Physics
Environmental Engineering Turbulence Ocean Engineering Engineering::Civil engineering [DRNTU] 02 engineering and technology Mechanics Vortex shedding Rotation 01 natural sciences 010305 fluids & plasmas Physics::Fluid Dynamics Boundary layer 020303 mechanical engineering & transports 0203 mechanical engineering Particle image velocimetry 0103 physical sciences Cylinder Potential flow Rotating Cylinder Retrograde direction Wall Proximity |
Zdroj: | Ocean Engineering. 156:240-251 |
ISSN: | 0029-8018 |
DOI: | 10.1016/j.oceaneng.2018.03.015 |
Popis: | The flow past a circular cylinder that is rotating retrograde near a turbulent wall boundary layer at Re = 10 000 has been investigated experimentally using particle image velocimetry (PIV). The cylinder rotates in retrograde direction with different rotation ratios from α = 0 to 2, where α is defined as the ratio of the peripheral speed on the cylinder surface divided by the free-stream velocity. The gap ratio, G * = G/D, is varied between 0 and 1.6, where G is the gap between the cylinder and the plane wall, and D is the cylinder diameter. The flow structure is greatly modified due to the influence of wall proximity and cylinder rotation, notably the onset/suppression, frequency and strength of vortex shedding. Similar to a near-wall stationary cylinder, there exists a critical gap ratio (about 0.4) below which periodic vortex shedding from the cylinder is suppressed. On the other hand, the cylinder rotation causes vortex shedding to cease at α ≥ 1.6, which is slightly lower than the reported value of α ≈ 2 in the literature on rotating cylinder in uniform flow. However, reducing G * and increasing α do not always favor the suppression of vortex shedding. In fact, cylinder rotation promotes vortex shedding over a certain range (α < 1). As α increases, the length of recirculation region behind the cylinder, which is indicated by the movement of the mean saddle point, decreases almost linearly. The effects of wall proximity and cylinder rotation are also evident on the ensemble-averaged flow field, such as the turbulent kinetic energy and Reynolds shear stress. Accepted version |
Databáze: | OpenAIRE |
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