首页 | 本学科首页   官方微博 | 高级检索  
     检索      


A circular cylinder undergoing large-amplitude transverse oscillations in a slow uniform cross flow
Institution:1. Department of Aerodynamics, Nanjing University of Aeronautics and Astronautics, Yudao Street 29, Nanjing, Jiangsu 210016, China;2. National Key Laboratory of Science and Technology on Hydrodynamics, China Ship Scientific Research Center, Wuxi, Jiangsu 214082, China;1. Department of Mathematical and Statistical Sciences, University of Alberta, Edmonton, Alberta T6G2G1, Canada;2. Department of Mechanical Engineering, University of Alberta, Edmonton, Alberta T6G2G8, Canada;1. Laboratoire de Mathématiques (UMR 6620), Campus des Cézeaux, Université Blaise Pascal, B.P. 80026, 63171 Aubière cedex, France;2. Institut de Mathématiques de Toulouse, Unité Mixte C.N.R.S. 5219, Université Paul Sabatier Toulouse III, 118 route de Narbonne, 31062 Toulouse Cedex 9, France;1. Department of Ocean Engineering, University of Rhode Island, Narragansett, RI 02882-1197, USA;2. China International Marine Containers (Group) LTD., Shenzhen 518067, China;3. CIMC Offshore Engineering Institute Company Limited, Yantai 264670, China;4. Shandong Provincial Key Lab of Ocean Engineering, Ocean University of China, Qingdao 266100, China
Abstract:This study explores the vortex patterns formed by a circular cylinder undergoing lateral cylinder oscillations with large amplitudes and in the presence of a slow uniform cross flow. It is an extension of our previous study (Lam et al., 2010b) in which formation of the 2S, 2P and P+S vortex modes were discussed from the viewpoint of interaction of a uniform cross-flow with the vortex street patterns of a cylinder oscillating in an otherwise quiescent fluid at Keulegan–Carpenter numbers up to KC=8.9. The present paper reports three additional experimental sets in which the amplitudes of cylinder oscillations have even larger values, at A/D>2.5, and lie beyond the vortex mode map usually quoted from Williamson and Roshko (1988). It is found that the slow uniform cross-flow at λ/D≈3 and Reynolds number based on cross-flow velocity at 232 acts to convect the corresponding vortex patterns in the absence of cross-flow downstream across the line of cylinder oscillation. Vortex–vortex interaction and vortex–cylinder interaction are observed to affect the subsequent development of vortices. The P+S vortex mode is found to occur up to KC=16. At KC between 16 and 24, a new vortex mode is observed in which only one vortex pair can be convected downstream every cylinder oscillation cycle. Another new vortex mode with two vortex pairs and two stationary vortices are found at KC>24.
Keywords:
本文献已被 ScienceDirect 等数据库收录!
设为首页 | 免责声明 | 关于勤云 | 加入收藏

Copyright©北京勤云科技发展有限公司  京ICP备09084417号