Critical effects of a spanwise surface wire on flow past a circular cylinder and the significance of the wire size and Reynolds number

被引:9
|
作者
Aydin, T. B. [1 ]
Joshi, A. [1 ]
Ekmekci, A. [1 ]
机构
[1] Univ Toronto, Inst Aerosp Studies, Toronto, ON, Canada
基金
加拿大自然科学与工程研究理事会; 加拿大创新基金会;
关键词
Flow control; Tripwire; Vortex shedding; Spanwise protrusion; Cylinder; Protrusion devices; TRIPPING WIRES; WAKE; CLASSIFICATION;
D O I
10.1016/j.jfluidstructs.2014.08.006
中图分类号
TH [机械、仪表工业];
学科分类号
0802 ;
摘要
An experimental study is conducted on flow past a circular cylinder fitted with a single spanwise wire on its surface. The work investigates the dependency of the critical wire locations on the wire size and Reynolds number, and examines the near wake and vortex shedding characteristics in an effort to advance the understanding of the critical wire effects beyond the existing literature. The Reynolds number is varied from 5000 to 30 000, and the wire diameter is varied from 2.9% to 5.9% of the cylinder diameter. All wires are larger than the boundary-layer thickness forming around a comparable smooth cylinder. Constant Temperature Anemometry and hydrogen bubble visualization are used as the flow diagnostic tools. The frequency and strength of the Karman instability are shown to vary with the wire location at any given Reynolds number nearly in an inverse fashion. For all the Reynolds numbers and wire sizes considered, two types of critical locations are shown to exist on the cylinder surface for the application of a wire. These locations are associated with the attenuation and amplification of the Karman instability, and in accord with the existing literature, are denoted as theta(c1) and theta(c2), respectively. The present work reveals that theta(c2) consists of a wide range of locations which remains unaffected from the wire size and Reynolds number, while theta(c1) is a relatively distinct location on the cylinder surface and depends on both the Reynolds number and wire size. For a given Reynolds number, increasing the wire size decreases theta(c1). For a given wire size, increasing the Reynolds number from 5000 to 15 000 increases theta(c1), and past 15 000, theta(c1) remains unaffected from the Reynolds number. When a wire is at theta(c1), even though, for the majority of the time the regular formation of Karman vortices ceases, the present data also reveals intermittent, short time periods where the regular shedding resumes. (C) 2014 Elsevier Ltd. All rights reserved.
引用
收藏
页码:132 / 147
页数:16
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