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Abstract
Vortexinduced vibration (VIV) of a sphere represents one of the most generic fundamental fluid–structure interaction problems. Since vortexinduced vibration can lead to structural failure, numerous studies have focused on understanding the underlying principles of VIV and its suppression. This paper reports on an experimental investigation of the effect of imposed axial rotation on the dynamics of vortexinduced vibration of a sphere that is free to oscillate in the crossflow direction, by employing simultaneous displacement and force measurements. The VIV response was investigated over a wide range of reduced velocities (i.e. velocity normalised by the natural frequency of the system): (Formula presented.), corresponding to a Reynolds number range of (Formula presented.), while the rotation ratio, defined as the ratio between the sphere surface and inflow speeds, (Formula presented.), was varied in increments over the range of (Formula presented.). It is found that the vibration amplitude exhibits a typical inverted bellshaped variation with reduced velocity, similar to the classic VIV response for a nonrotating sphere but without the higher reduced velocity response tail. The vibration amplitude decreases monotonically and gradually as the imposed transverse rotation rate is increased up to (Formula presented.), beyond which the body vibration is significantly reduced. The synchronisation regime, defined as the reduced velocity range where large vibrations close to the natural frequency are observed, also becomes narrower as (Formula presented.) is increased, with the peak saturation amplitude observed at progressively lower reduced velocities. In addition, for small rotation rates, the peak amplitude decreases almost linearly with (Formula presented.). The imposed rotation not only reduces vibration amplitudes, but also makes the body vibrations less periodic. The frequency spectra revealed the occurrence of a broadband spectrum with an increase in the imposed rotation rate. Recurrence analysis of the structural vibration response demonstrated a transition from periodic to chaotic in a modified recurrence map complementing the appearance of broadband spectra at the onset of bifurcation. Despite considerable changes in flow structure, the vortex phase ((Formula presented.)), defined as the phase between the vortex force and the body displacement, follows the same pattern as for the nonrotating case, with the (Formula presented.) increasing gradually from low values in Mode I of the sphere vibration to almost (Formula presented.) as the system undergoes a continuous transition to Mode II of the sphere vibration at higher reduced velocity. The total phase ((Formula presented.)), defined as the phase between the transverse lift force and the body displacement, only increases from low values after the peak amplitude response in Mode II has been reached. It reaches its maximum value ((Formula presented.)) close to the transition from the Mode II upper plateau to the lower plateau, reminiscent of the behaviour seen for the upper to lower branch transition for cylinder VIV. Hydrogenbubble visualisations and particle image velocimetry (PIV) performed in the equatorial plane provided further insights into the flow dynamics near the sphere surface. The mean wake is found to be deflected towards the advancing side of the sphere, associated with an increase in the Magnus force. For higher rotation ratios, the nearwake rear recirculation zone is absent and the flow is highly vectored from the retreating side to the advancing side, giving rise to largescale shedding. For a very high rotation ratio of (Formula presented.), for which vibrations are found to be suppressed, a onesided largescale shedding pattern is observed, similar to the shearlayer instability onesided shedding observed previously for a rigidly mounted rotating sphere.
Original language  English 

Pages (fromto)  258292 
Number of pages  35 
Journal  Journal of Fluid Mechanics 
Volume  837 
DOIs  
Publication status  Published  25 Feb 2018 
Keywords
 flowstructure interactions
 vortex streets
 wakes
Projects
 1 Finished

Wake Transitions and FluidStructure Interactions of Rotating Bluff Bodies
Hourigan, K., Lo Jacono, D., Sheridan, J., Thompson, M. & Leweke, T.
Australian Research Council (ARC), Monash University, CNRS  Centre National de la Recherche Scientifique (French National Centre for Scientific Research), Université PaulSabatier (Paul Sabatier University)
1/01/15 → 6/11/18
Project: Research