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Numerical studies of the flow structure and aerodynamic forces on two tandem square cylinders with different chamfered-corner ratios

机译:不同倒角基角比的两个串联方圆柱上流动结构和空气动力的数值研究

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摘要

Three-dimensional large eddy simulations were carried out to investigate the flow over two tandem square cylinders for a fixed spacing ratio of L/D = 4 and a Reynolds number of 5.3 x 10(3), where L is the cylinder center-to-center distance between the cylinders and D is the cylinder width. The corners of each cylinder were chamfered with a ratio of xi = B/D = 0%, 5%, 10%, and 15%, where B is the chamfered corner dimension. The focus is given on how xi influences the flow structure, wake recirculation bubble, flow separation bubble, Strouhal number (St), aerodynamic force, and phase lag (phi) between vortex sheddings from the cylinders. With increasing xi, the recirculation bubble length and minimum velocity in the wake of the upstream cylinder remain more or less constant and are close to those of a single cylinder, while the minimum velocity in the wake of the downstream cylinder dramatically drops between xi = 0% and 5%. While the flow over the downstream remains attached on the side surfaces, that over the upstream cylinder forms primary and secondary side-surface bubbles on the side surface, and both shrink with increasing xi. In addition, the leading chamfered corners are accompanied by corner bubbles that play an important role in the flow structure modification. Therefore, the time-mean drag and fluctuating lift of the upstream cylinder remarkably decrease for 0% <= xi <= 5% and remain almost unchanged for 5% < xi <= 15%, whereas those on the downstream cylinder diminish in the whole range of 0% <= xi <= 15%. The Strouhal number (St) being identical for the two cylinders grows from 0.104 to 0.132 when xi is increased from 0% to 15%. Overall, the influence of xi on the wake structure and aerodynamics is remarkable for 0% <= xi <= 5% because of the corner bubbles and is less for 5% < xi <= 15%.
机译:进行三维大涡流模拟,以研究两个串联方圆柱的流量,用于固定间隔比,L / D = 4和雷诺数为5.3×10(3),其中L是气缸中心 - 到 - 气缸和D之间的中心距离是气缸宽度。每个气缸的拐角的倒角,Xi = B / D = 0%,5%,10%和15%的比率,其中B是倒角拐角尺寸。关于Xi如何影响流动结构,唤醒再循环泡沫,流量分离气泡,斯特鲁姆数(ST),空气动力和相滞(PHI)从气缸之间影响旋转的焦点。随着Xi的增加,上游圆筒尾部的再循环气泡长度和最小速度仍然是或多或少恒定并且靠近单个圆筒的速度,而下游圆筒尾之迹的最小速度在Xi = 0之间逐渐下降。 %和5%。虽然在下游的流量保持在侧表面上,但在上游圆筒上形成侧表面上的初级和次级侧表面气泡,并且随着Xi的增加而缩小。此外,领先的倒角拐角伴随着在流动结构修改中发挥着重要作用的角气泡。因此,上游圆筒的时间平均阻力和波动升降量显着降低0%<= x = 5%,并且仍然几乎保持不变,5%

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  • 来源
    《Physics of fluids》 |2019年第7期|共15页
  • 作者单位

    Southwest Jiaotong Univ Res Ctr Wind Engn Chengdu 610031 Sichuan Peoples R China;

    Southwest Jiaotong Univ Res Ctr Wind Engn Chengdu 610031 Sichuan Peoples R China;

    Harbin Inst Technol Shenzhen Inst Turbulence Noise Vibrat Interact &

    Control Shenzhen 518055 Peoples R China;

    Southwest Jiaotong Univ Res Ctr Wind Engn Chengdu 610031 Sichuan Peoples R China;

    Tongji Univ State Key Lab Disaster Reduct Civil Engn Shanghai 200092 Peoples R China;

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  • 原文格式 PDF
  • 正文语种 eng
  • 中图分类 流体力学;
  • 关键词

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