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Fluid-structure interactions of an oscillating cylinder in cross flow in the presence of a neighbouring cylinder.

机译:在存在相邻圆柱体的情况下,振荡圆柱体在错流中的流体-结构相互作用。

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摘要

The fluid-structure interactions of a single streamwise oscillating circular cylinder and two tandem (including a streamwise oscillating circular cylinder) and side-by-side circular cylinders have been experimentally investigated using methods of LIF (Laser-induced fluorescence) visualization, PIV, laser vibrometer and hot wires.;In the case of a single streamwise oscillating cylinder, the wake mode has been studied at relatively large oscillation amplitudes A/d = 0.5 and 0.67 over a range of frequencies fe/fs = 0∼3.1. Five typical flow structures, referred to as S-I, S-II, A-I, A-III and A-IV modes, respectively, are identified. Their occurrence is dependent on a combination of A/d and fe/f s. The occurrence of the S-II mode has been predicted. The threshold frequency ratio (fe/fs) c for the occurrence of the S-II mode is inversely proportional to A/d and dependent on the Reynolds number Re. The Re effect is negligible for Re > 250. The results are in good agreement with available experimental data.;Interference between a streamwise oscillating cylinder (A/d = 0.5 and 0.67, fe/fs = 0∼2) wake and that of a downstream stationary cylinder with an identical diameter has been experimentally studied. The center-to-center spacing L/d of two cylinders varies from 2.5 to 4.5. Three distinct flow regimes have been identified. For 0.45∼0.5 < fe/fs < 0.8∼1.0 (depends on A/d), a single antisymmetrical vortex street (A-mode) emerges behind the downstream cylinder. For 0.8∼1.0 < fe/fs < (fe/f s)c which depends on A/d and Re, the flow behind the downstream cylinder is characterized by an antisymmetric-antisymmetric complex street (AA-mode) that consists of two outer rows of binary vortices originating from the upstream cylinder, and two inner rows of single vortices shed by the downstream cylinder. For fe/fs > (fe/f s)c, the symmetric-antisymmetric complex street (SA-mode) occurs behind the downstream cylinders, respectively.;Interference between a stationary cylinder wake and that of a downstream streamwise oscillating cylinder (L/d = 2.5∼4.5; A/d = 0.5 and 0.67; fe/fs = 0∼2) has also been studied. Two flow regimes have been identified, i.e., the ‘single-cylinder shedding regime’ at L/d ≤ 3.5 and the ‘two-cylinder shedding regime’ at L/d > 3.5. For the ‘single-cylinder shedding regime’, the upstream cylinder does not appear to shed vortices; vortices are symmetrically formed behind the downstream cylinder as a result of interactions between the shear layers separated from the upstream cylinder and the oscillation of the downstream cylinder. (Abstract shortened by UMI.).
机译:使用LIF(激光诱导荧光)可视化,PIV,激光的方法,通过实验研究了一个单向流振荡圆柱和两个串联(包括一个流向振荡圆柱)和并排圆柱的流体-结构相互作用。在单个流式振荡缸的情况下,已经在频率fe / fs = 0至3.1的较大振幅A / d = 0.5和0.67的情况下研究了唤醒模式。确定了五个典型的流动结构,分别称为S-I,S-II,A-I,A-III和A-IV模式。它们的出现取决于A / d和fe / f s的组合。已经预测到S-II模式的出现。发生S-II模式的阈值频率比(fe / fs)c与A / d成反比,并取决于雷诺数Re。当Re> 250时,Re的影响可忽略不计。结果与可用的实验数据很好地吻合。流向振荡的圆柱体(A / d = 0.5和0.67,fe / fs = 0〜2)与水流的振荡之间的干扰已经对具有相同直径的下游固定缸进行了实验研究。两个圆柱体的中心距L / d从2.5到4.5不等。已经确定了三种不同的流动方式。当0.45〜0.5 (fe / fs)c时,对称-非对称复数街(SA-mode)分别出现在下游圆柱体的后面;固定圆柱体尾流与下游流向振荡圆柱体(L / d)之间的干扰(2.5 / 4.5; A / d = 0.5和0.67; fe / fs = 0-2)。已经确定了两种流动状态,即L / d≤3.5时的“单缸脱落状态”和当L / d> 3.5时的“两缸脱落状态”。对于“单缸脱落系统”,上游缸似乎没有脱落涡流;由于与上游圆柱体分离的剪切层与下游圆柱体的振动之间的相互作用,在下游圆柱体的后面对称地形成了涡流。 (摘要由UMI缩短。)。

著录项

  • 作者

    Xu, Shengjin.;

  • 作者单位

    Hong Kong Polytechnic University (Hong Kong).;

  • 授予单位 Hong Kong Polytechnic University (Hong Kong).;
  • 学科 Engineering Mechanical.
  • 学位 Ph.D.
  • 年度 2003
  • 页码 178 p.
  • 总页数 178
  • 原文格式 PDF
  • 正文语种 eng
  • 中图分类
  • 关键词

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