{"title":"In-line flow-induced vibration of rotating elliptical cylinders","authors":"","doi":"10.1016/j.jfluidstructs.2024.104186","DOIUrl":null,"url":null,"abstract":"<div><p>This study numerically investigates the in-line flow-induced vibration (FIV) of elastically mounted elliptical cylinders undergoing forced rotations in a free-stream flow. The two-dimensional numerical simulations were conducted at a Reynolds number of 100. The cross-sectional aspect ratio (or elliptical ratio) of the cylinders varied from 1 to 0.25. The aspect/elliptical ratio is defined by <span><math><mrow><mi>ϵ</mi><mo>=</mo><mn>2</mn><mi>b</mi><mo>/</mo><mn>2</mn><mi>a</mi></mrow></math></span>, where <span><math><mrow><mn>2</mn><mi>a</mi></mrow></math></span> and <span><math><mrow><mn>2</mn><mi>b</mi></mrow></math></span> are the streamwise and cross-flow dimensions, respectively, of the cross-section of a cylinder placed at zero incidence angle. The Reynolds number is defined by <span><math><mrow><mi>R</mi><mi>e</mi><mo>=</mo><mi>U</mi><mi>D</mi><mo>/</mo><mi>ν</mi></mrow></math></span>, where <span><math><mi>U</mi></math></span> is the free-stream velocity, <span><math><mi>ν</mi></math></span> is the kinematic viscosity of the fluid, and <span><math><mi>D</mi></math></span> is the major axis length (i.e. <span><math><mrow><mi>D</mi><mo>=</mo><mn>2</mn><mi>a</mi></mrow></math></span>). The dimensionless rotation rate, defined by <span><math><mrow><mi>α</mi><mo>=</mo><mrow><mo>|</mo><mi>Ω</mi><mo>|</mo></mrow><mi>D</mi><mo>/</mo><mrow><mo>(</mo><mn>2</mn><mi>U</mi><mo>)</mo></mrow></mrow></math></span>, is varied at values of 0.2, 0.5, 1 and 2, where <span><math><mi>Ω</mi></math></span> represents the angular velocity of the body rotation. The FIV response is examined as a function of reduced velocity, defined by <span><math><mrow><msup><mrow><mi>U</mi></mrow><mrow><mo>∗</mo></mrow></msup><mo>=</mo><mi>U</mi><mo>/</mo><mrow><mo>(</mo><msub><mrow><mi>f</mi></mrow><mrow><mi>n</mi></mrow></msub><mi>D</mi><mo>)</mo></mrow></mrow></math></span>, with <span><math><msub><mrow><mi>f</mi></mrow><mrow><mi>n</mi></mrow></msub></math></span> being the natural frequency of the system. Interestingly, two synchronisation modes were identified: a “rotation-dominated” (RD) mode and a “wake-dominated” (WD) mode. For <span><math><mrow><mi>α</mi><mo>∈</mo><mrow><mo>{</mo><mn>0</mn><mo>.</mo><mn>2</mn><mo>,</mo><mn>0</mn><mo>.</mo><mn>5</mn><mo>,</mo><mn>1</mn><mo>}</mo></mrow></mrow></math></span>, the RD mode was found to be associated with significantly high-amplitude vibration, while the WD mode was associated with low-amplitude vibration. However, as <span><math><mi>α</mi></math></span> increased to 2, the WD region exhibited a higher amplitude peak compared to the RD region. The maximum vibration amplitude in the present study was observed to be approximately <span><math><mrow><mn>0</mn><mo>.</mo><mn>5</mn><mi>D</mi></mrow></math></span>, occurring for <span><math><mrow><mi>α</mi><mo>=</mo><mn>0</mn><mo>.</mo><mn>2</mn></mrow></math></span>. A further analysis of the wake structure revealed that vortex feeding or merging behaviour occurred at <span><math><mrow><mi>α</mi><mo>=</mo><mn>0</mn><mo>.</mo><mn>5</mn></mrow></math></span>, 1 and 2 for <span><math><mrow><mi>ϵ</mi><mo>=</mo><mn>0</mn><mo>.</mo><mn>25</mn></mrow></math></span> and <span><math><mrow><mi>ϵ</mi><mo>⩽</mo><mn>0</mn><mo>.</mo><mn>75</mn></mrow></math></span> for <span><math><mrow><mi>α</mi><mo>=</mo><mn>0</mn><mo>.</mo><mn>5</mn></mrow></math></span>. Increasing the rotation rate or the aspect ratio could weaken the impact of rotation on vibration, resulting in a reduction in the peak vibration amplitude of RD region. Notably, harmonic frequency components exceeding the rotation frequency were observed for <span><math><mrow><mi>α</mi><mo>=</mo><mn>0</mn><mo>.</mo><mn>2</mn></mrow></math></span>. Further investigation with the fixed body revealed that the wake pattern of the rotating elliptical cylinder undergoes a transition when <span><math><mrow><mi>α</mi><mo><</mo><mn>0</mn><mo>.</mo><mn>3</mn></mrow></math></span>, exhibiting significant instability characterised by the superposition of high-order harmonic components.</p></div>","PeriodicalId":54834,"journal":{"name":"Journal of Fluids and Structures","volume":null,"pages":null},"PeriodicalIF":3.4000,"publicationDate":"2024-09-21","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":"0","resultStr":null,"platform":"Semanticscholar","paperid":null,"PeriodicalName":"Journal of Fluids and Structures","FirstCategoryId":"5","ListUrlMain":"https://www.sciencedirect.com/science/article/pii/S088997462400121X","RegionNum":2,"RegionCategory":"工程技术","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":null,"EPubDate":"","PubModel":"","JCR":"Q1","JCRName":"ENGINEERING, MECHANICAL","Score":null,"Total":0}
引用次数: 0
Abstract
This study numerically investigates the in-line flow-induced vibration (FIV) of elastically mounted elliptical cylinders undergoing forced rotations in a free-stream flow. The two-dimensional numerical simulations were conducted at a Reynolds number of 100. The cross-sectional aspect ratio (or elliptical ratio) of the cylinders varied from 1 to 0.25. The aspect/elliptical ratio is defined by , where and are the streamwise and cross-flow dimensions, respectively, of the cross-section of a cylinder placed at zero incidence angle. The Reynolds number is defined by , where is the free-stream velocity, is the kinematic viscosity of the fluid, and is the major axis length (i.e. ). The dimensionless rotation rate, defined by , is varied at values of 0.2, 0.5, 1 and 2, where represents the angular velocity of the body rotation. The FIV response is examined as a function of reduced velocity, defined by , with being the natural frequency of the system. Interestingly, two synchronisation modes were identified: a “rotation-dominated” (RD) mode and a “wake-dominated” (WD) mode. For , the RD mode was found to be associated with significantly high-amplitude vibration, while the WD mode was associated with low-amplitude vibration. However, as increased to 2, the WD region exhibited a higher amplitude peak compared to the RD region. The maximum vibration amplitude in the present study was observed to be approximately , occurring for . A further analysis of the wake structure revealed that vortex feeding or merging behaviour occurred at , 1 and 2 for and for . Increasing the rotation rate or the aspect ratio could weaken the impact of rotation on vibration, resulting in a reduction in the peak vibration amplitude of RD region. Notably, harmonic frequency components exceeding the rotation frequency were observed for . Further investigation with the fixed body revealed that the wake pattern of the rotating elliptical cylinder undergoes a transition when , exhibiting significant instability characterised by the superposition of high-order harmonic components.
期刊介绍:
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