Influence of plane boundary proximity on the Honji instability. (3rd August 2018)

• Record Type: Journal Article
• Authors: Xiong, Chengwang; Cheng, Liang; Tong, Feifei; An, Hongwei
• Is Part Of: Journal of fluid mechanics. Volume 852(2018)
• Page Start: 226
• Page End: 256
• Publication Date: 2018-08-03
• Subjects: absolute/convective instability, -- boundary layer structure; Fluid mechanics -- Periodicals; 532.005
• DOI: 10.1017/jfm.2018.538
• Languages: English
• ISSNs: 0022-1120

Abstract

Abstract : This paper presents a numerical investigation of oscillatory flow around a circular cylinder that is placed in proximity to a plane boundary that is parallel to the cylinder axis. The onset and development of the Honji instability are studied over a range of Stokes numbers ( $\unicode[STIX]{x1D6FD}$ ) and gap-to-diameter ratios ( $e/D$ ) at a fixed Keulegan–Carpenter number ( $KC=2$ ). Four flow regimes are identified in the ( $e/D, \unicode[STIX]{x1D6FD}$ )-plane: (I) featureless two-dimensional flow, (II) stable Honji vortex, (III) unstable Honji vortex and (IV) chaotic flow. As $e/D$ increases from $-0.5$ (embedment) to $1$, the critical Stokes number $\unicode[STIX]{x1D6FD}_{cr}$ for the onset of the Honji instability follows two side-by-side convex functions, peaking at the connection point of $e/D=0.125$ and reaching troughs at $e/D=0$ and 0.375. The Honji instability is always initiated on the gap side of the cylinder surface for $0.375\leqslant e/D\leqslant 2$ and occurs only on the top side for $-0.5\leqslant e/D<0.125$ . The location for the initiation of the Honji instability switches from the gap side to the top side of the cylinder surface for $0.125<e/D<0.375$ . No Honji instability is observed at $e/D=0.125$, where the flow three-dimensionality is developed through a different flow mechanism. Consistently, the three-dimensional kinetic energy of the flow, which represents a measure of the strength of flow three-dimensionality, varies with $e/D$ in a trend opposite to that of $\unicode[STIX]{x1D6FD}_{cr}$ . Three physical mechanisms are identified as being responsible for the observed variation trend of $\unicode[STIX]{x1D6FD}_{cr}$ with $e/D$ and for various flow phenomena, which are the blockage effect induced by the geometry setting, the existence of the Stokes layer on the plane boundary and the favourable pressure gradient in the flow direction over the gap between the cylinder and the plane surface.