{"title":"旋转椭圆形气缸的在线流动诱导振动","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":"{\"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}","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}
In-line flow-induced vibration of rotating elliptical cylinders
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:
The Journal of Fluids and Structures serves as a focal point and a forum for the exchange of ideas, for the many kinds of specialists and practitioners concerned with fluid–structure interactions and the dynamics of systems related thereto, in any field. One of its aims is to foster the cross–fertilization of ideas, methods and techniques in the various disciplines involved.
The journal publishes papers that present original and significant contributions on all aspects of the mechanical interactions between fluids and solids, regardless of scale.