Flow over a cylinder with a hinged-splitter plate

• Published in: Journal of fluids and structures 2009-05, Vol.25 (4), p.713-720
• Main Authors: Shukla, S., Govardhan, R.N., Arakeri, J.H.
• Format: Article
• Language: English
• Subjects: Cylinder wake; Exact sciences and technology; Fluid dynamics; Fundamental areas of phenomenology (including applications); Physics; Rotational flow and vorticity; Solid mechanics; Splitter plate; Structural and continuum mechanics; Turbulent flows, convection, and heat transfer; Vibration, mechanical wave, dynamic stability (aeroelasticity, vibration control...); Vortex-induced vibrations; Wakes
• ISSN: 0889-9746; 1095-8622
• DOI: 10.1016/j.jfluidstructs.2008.11.004

Previous work on rigid splitter plates in the wake of a bluff body has shown that the primary vortex shedding can be suppressed for sufficiently long splitter plates. In the present work, we study the problem of a hinged-splitter plate in the wake of a circular cylinder. The splitter plate can rotate about the hinge at the base of the cylinder due to the unsteady fluid forces acting on it, and hence the communication between the two sides of the wake is not totally disrupted as in the rigid splitter plate case. In our study, we investigate this problem in the limit where the stiffness and internal damping associated with the hinge are negligible, and the mass ratio of the splitter plate is small. The experiments show that the splitter plate oscillations increase with Reynolds numbers at low values of Re, and are found to reach a saturation amplitude level at higher Re, Re > 4000 . This type of saturation amplitude level that appears to continue indefinitely with Re, appears to be related to the fact that there is no structural restoring force, and has been observed previously for transversely oscillating cylinders with no restoring force. In the present case, the saturation tip amplitude level can be up to 0.45 D , where D is the cylinder diameter. For this hinged-rigid splitter plate case, it is found that the splitter plate length to cylinder diameter ratio ( L / D ) is crucial in determining the character and magnitude of the oscillations. For small splitter plate lengths ( L / D ⩽ 3.0 ), the oscillations appear to be nearly periodic with tip amplitudes of about 0.45 D nearly independent of L / D . The nondimensional oscillation frequencies ( fD / U ) on the other hand are found to continuously vary with L / D from fD / U ≈ 0.2 at L / D = 1 to fD / U ≈ 0.1 at L / D = 3 . As the splitter plate length is further increased beyond L / D ⩾ 4.0 , the character of the splitter plate oscillations suddenly changes. The oscillations become aperiodic with much smaller amplitudes. In this long splitter plate regime, the spectra of the oscillations become broadband, and are reminiscent of the change in character of the wake oscillations seen in the earlier fixed-rigid splitter plate case for L / D ⩾ 5.0 . In the present case of the hinged-splitter plate, the sudden transition seen as the splitter plate length ( L / D ) is increased from 3 to 4 may be attributed to the fact that the wake vortices are no longer able to synchronize with the plate motions for larger spl