Vortex dynamics and turbulence transport in flow around a near-wall rectangular cylinder

被引:0
|
作者
Li, Jiang-Hua [1 ,2 ,3 ,4 ]
Wang, Bo-Fu [3 ]
Qiu, Xiang [3 ,4 ]
Zhou, Quan [3 ]
Fu, Shi-Xiao [1 ,2 ]
Liu, Yu-Lu [3 ,4 ]
机构
[1] Shanghai Jiao Tong Univ, Sch Ocean & Civil Engn, Shanghai 200240, Peoples R China
[2] Shanghai Jiao Tong Univ, State Key Lab Ocean Engn, Shanghai 200040, Peoples R China
[3] Shanghai Univ, Shanghai Inst Appl Math & Mech, Sch Mech & Engn Sci, Shanghai Key Lab Mech Energy Engn, Shanghai 200072, Peoples R China
[4] Shanghai Inst Technol, Sch Sci, Shanghai 201418, Peoples R China
基金
中国国家自然科学基金; 中国博士后科学基金;
关键词
CIRCULAR-CYLINDER; COHERENT STRUCTURES; BOUNDARY; LAYER; SIMULATIONS; SINGLE; PRISMS;
D O I
10.1063/5.0255293
中图分类号
O3 [力学];
学科分类号
08 ; 0801 ;
摘要
This study investigates the vortex dynamics and turbulent characteristics of flow around a near-wall rectangular cylinder for varying gap ratios ( G/D=0.1, 0.3, and 0.9) and aspect ratios ( L/D=5, 10, and 15). Kelvin-Helmholtz vortices form from the upper leading edge (ULE) shear layer, with secondary instabilities leading to three-dimensional vortex structures. For small gap ratios ( G/D=0.1 and 0.3), strong near-wall effects suppress the formation of lower leading edge (LLE) shear layers, whereas at G/D=0.9, both LLE and lower trailing edge shear layers form, increasing vortex complexity. The downstream wall recirculation also decreases with increasing G/D. For smaller aspect ratios ( L/D=5), the ULE recirculation spans the upper side of the cylinder, while for larger L/D values ( L/D=10, 15), hairpin vortices form on the upper side. The growth of the ULE shear layer, quantified by vorticity thickness (delta(omega)), is influenced by the near-wall effect and exhibits three growth regions. Turbulent fluctuations, reflected in total turbulent kinetic energy (TKE) and Reynolds stresses, are influenced by both G/D and L/D. Fluctuations decrease as G/D increases from 0.1 to 0.3 due to weakened vortex-wall interactions, while alternating vortex shedding at G/D=0.9 intensifies fluctuations. The integration of TKE and Reynolds stresses reveals single and double peaks for L/D=5 and L/D=10,15, respectively. TKE production analysis shows that P-11 dominates the total TKE for smaller gap ratios, while P-22 for wall-normal TKE becomes more significant at G/D=0.9. These findings provide insight into the complex vortex dynamics and turbulence mechanisms in near-wall bluff body flows.
引用
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页数:16
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