Effect of aspect ratio on flow-induced vibration of oblate spheroids and implications for energy generation

IF 3.4 2区 工程技术 Q1 ENGINEERING, MECHANICAL Journal of Fluids and Structures Pub Date : 2024-06-19 DOI:10.1016/j.jfluidstructs.2024.104137
Adrian Cordero Obando , Mark C. Thompson , Kerry Hourigan , Jisheng Zhao
{"title":"Effect of aspect ratio on flow-induced vibration of oblate spheroids and implications for energy generation","authors":"Adrian Cordero Obando ,&nbsp;Mark C. Thompson ,&nbsp;Kerry Hourigan ,&nbsp;Jisheng Zhao","doi":"10.1016/j.jfluidstructs.2024.104137","DOIUrl":null,"url":null,"abstract":"<div><p>This study experimentally investigates the influence of aspect ratio on cross-flow flow-induced vibration (FIV) of elastically mounted oblate spheroids. The aspect ratio (<span><math><mrow><mi>ϵ</mi><mo>=</mo><mi>b</mi><mo>/</mo><mi>a</mi></mrow></math></span>) of an oblate spheroid, defined as the ratio of the major diameter (<span><math><mi>b</mi></math></span>) in the cross-flow direction to the minor diameter (<span><math><mi>a</mi></math></span>) in the streamwise direction, was varied between 1.00 and 3.20. The FIV response was characterized over a range of reduced velocity, <span><math><mrow><mn>3</mn><mo>.</mo><mn>0</mn><mo>⩽</mo><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><mi>w</mi></mrow></msub><mi>b</mi><mo>)</mo></mrow><mo>⩽</mo><mn>12</mn><mo>.</mo><mn>0</mn></mrow></math></span>, where <span><math><mi>U</mi></math></span> is the free-stream velocity and <span><math><msub><mrow><mi>f</mi></mrow><mrow><mi>n</mi><mi>w</mi></mrow></msub></math></span> is the natural frequency of the system in quiescent water. The corresponding Reynolds number varied over the range <span><math><mrow><mn>4730</mn><mo>⩽</mo><mi>R</mi><mi>e</mi><mo>⩽</mo><mn>20</mn><mspace></mspace><mn>120</mn></mrow></math></span>. It was found that in addition to the vortex-induced vibration (VIV) Mode I and Mode II responses observed for a sphere, on increasing the aspect ratio to <span><math><mrow><mi>ϵ</mi><mo>=</mo><mn>1</mn><mo>.</mo><mn>53</mn></mrow></math></span> and 2.0, a galloping-dominated response, denoted by G-I, was encountered at high reduced velocities. With a further increase in aspect ratio to <span><math><mrow><mi>ϵ</mi><mo>=</mo><mn>2</mn><mo>.</mo><mn>50</mn></mrow></math></span>, the body vibration exhibited an additional VIV-like response (V-I) following the sequential appearance of Mode I, Mode II and G-I, with smooth transitions between these modes. In the case of the largest aspect ratio considered in the present study, <span><math><mrow><mi>ϵ</mi><mo>=</mo><mn>3</mn><mo>.</mo><mn>20</mn></mrow></math></span>, the spheroid intriguingly exhibited only a pure VIV Mode I before transitioning to a VIV-dominated mode, namely V-II. The largest vibration amplitude observed was <span><math><mrow><mn>2</mn><mo>.</mo><mn>17</mn><mi>b</mi></mrow></math></span>, occurring at the highest tested reduced velocity of <span><math><mrow><msup><mrow><mi>U</mi></mrow><mrow><mo>∗</mo></mrow></msup><mo>=</mo><mn>12</mn><mo>.</mo><mn>0</mn></mrow></math></span> for <span><math><mrow><mi>ϵ</mi><mo>=</mo><mn>2</mn><mo>.</mo><mn>5</mn></mrow></math></span>. Furthermore, the maximum time-averaged power coefficient was observed to be 0.165 for the thinnest oblate spheroid tested, <span><math><mrow><mi>ϵ</mi><mo>=</mo><mn>3</mn><mo>.</mo><mn>20</mn></mrow></math></span>, approximately 660% higher than that observed for VIV of a sphere. This shows the relevance of geometry for FIV energy harvesting from oblate spheroids. The findings highlight the distinctive nature of FIV responses of 3D oblate spheroids compared to 2D bluff bodies such as elliptical, D-section, and square cylinders.</p></div>","PeriodicalId":54834,"journal":{"name":"Journal of Fluids and Structures","volume":null,"pages":null},"PeriodicalIF":3.4000,"publicationDate":"2024-06-19","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"https://www.sciencedirect.com/science/article/pii/S0889974624000720/pdfft?md5=a5fb645d3e64e202999601338797ddb6&pid=1-s2.0-S0889974624000720-main.pdf","citationCount":"0","resultStr":null,"platform":"Semanticscholar","paperid":null,"PeriodicalName":"Journal of Fluids and Structures","FirstCategoryId":"5","ListUrlMain":"https://www.sciencedirect.com/science/article/pii/S0889974624000720","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 experimentally investigates the influence of aspect ratio on cross-flow flow-induced vibration (FIV) of elastically mounted oblate spheroids. The aspect ratio (ϵ=b/a) of an oblate spheroid, defined as the ratio of the major diameter (b) in the cross-flow direction to the minor diameter (a) in the streamwise direction, was varied between 1.00 and 3.20. The FIV response was characterized over a range of reduced velocity, 3.0U=U/(fnwb)12.0, where U is the free-stream velocity and fnw is the natural frequency of the system in quiescent water. The corresponding Reynolds number varied over the range 4730Re20120. It was found that in addition to the vortex-induced vibration (VIV) Mode I and Mode II responses observed for a sphere, on increasing the aspect ratio to ϵ=1.53 and 2.0, a galloping-dominated response, denoted by G-I, was encountered at high reduced velocities. With a further increase in aspect ratio to ϵ=2.50, the body vibration exhibited an additional VIV-like response (V-I) following the sequential appearance of Mode I, Mode II and G-I, with smooth transitions between these modes. In the case of the largest aspect ratio considered in the present study, ϵ=3.20, the spheroid intriguingly exhibited only a pure VIV Mode I before transitioning to a VIV-dominated mode, namely V-II. The largest vibration amplitude observed was 2.17b, occurring at the highest tested reduced velocity of U=12.0 for ϵ=2.5. Furthermore, the maximum time-averaged power coefficient was observed to be 0.165 for the thinnest oblate spheroid tested, ϵ=3.20, approximately 660% higher than that observed for VIV of a sphere. This shows the relevance of geometry for FIV energy harvesting from oblate spheroids. The findings highlight the distinctive nature of FIV responses of 3D oblate spheroids compared to 2D bluff bodies such as elliptical, D-section, and square cylinders.

查看原文
分享 分享
微信好友 朋友圈 QQ好友 复制链接
本刊更多论文
长宽比对扁球体流动诱导振动的影响及对能源生产的启示
本研究通过实验研究了长宽比对弹性安装的扁球体的横流流动诱导振动(FIV)的影响。扁球体的长宽比(ϵ=b/a)定义为横流方向的大直径(b)与流向方向的小直径(a)之比,在 1.00 和 3.20 之间变化。FIV 响应的特征是在速度减小的范围内,3.0⩽U∗=U/(fnwb)⩽12.0,其中 U 是自由流速度,fnw 是静水中系统的固有频率。相应的雷诺数变化范围为 4730⩽Re⩽2020。研究发现,除了在球体上观察到的涡旋诱导振动(VIV)模式 I 和模式 II 响应外,当纵横比增加到 ϵ=1.53 和 2.0 时,在高速降低时还会出现以 G-I 表示的奔腾为主的响应。当长宽比进一步增大到 ϵ=2.50 时,车身振动在依次出现模式 I、模式 II 和 G-I 之后,又表现出一种类似 VIV 的响应(V-I),这些模式之间过渡平滑。在本研究中考虑的最大长宽比ϵ=3.20 的情况下,球体在过渡到以 VIV 为主导的模式(即 V-II)之前仅表现出纯粹的 VIV 模式 I,令人费解。观测到的最大振幅为 2.17b,发生在ϵ=2.5 条件下测试的最高减速度 U∗=12.0 时。此外,在测试的最薄扁球体 ϵ=3.20 时,观测到的最大时间平均功率系数为 0.165,比球体的 VIV 高出约 660%。这表明几何形状与扁球体的 FIV 能量收集有关。研究结果突出了三维扁球体的 FIV 响应与二维钝体(如椭圆、D 型截面和方形圆柱体)相比的独特性。
本文章由计算机程序翻译,如有差异,请以英文原文为准。
求助全文
约1分钟内获得全文 去求助
来源期刊
Journal of Fluids and Structures
Journal of Fluids and Structures 工程技术-工程:机械
CiteScore
6.90
自引率
8.30%
发文量
173
审稿时长
65 days
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.
期刊最新文献
A new approach for spatio-temporal interface treatment in fluid–solid interaction using artificial neural networks employing coupled partitioned fluid–solid solvers Condensation solution method for fluid-structure interaction dynamic models of structural system Turbulence-induced vibration in annular flow of a rigid cylinder mounted on a cantilever beam Recurrent graph convolutional multi-mesh autoencoder for unsteady transonic aerodynamics On the characteristics of fluid flow field and oscillatory response of tuned liquid multi-column dampers
×
引用
GB/T 7714-2015
复制
MLA
复制
APA
复制
导出至
BibTeX EndNote RefMan NoteFirst NoteExpress
×
×
提示
您的信息不完整,为了账户安全,请先补充。
现在去补充
×
提示
您因"违规操作"
具体请查看互助需知
我知道了
×
提示
现在去查看 取消
×
提示
确定
0
微信
客服QQ
Book学术公众号 扫码关注我们
反馈
×
意见反馈
请填写您的意见或建议
请填写您的手机或邮箱
已复制链接
已复制链接
快去分享给好友吧!
我知道了
×
扫码分享
扫码分享
Book学术官方微信
Book学术文献互助
Book学术文献互助群
群 号:481959085
Book学术
文献互助 智能选刊 最新文献 互助须知 联系我们:info@booksci.cn
Book学术提供免费学术资源搜索服务,方便国内外学者检索中英文文献。致力于提供最便捷和优质的服务体验。
Copyright © 2023 Book学术 All rights reserved.
ghs 京公网安备 11010802042870号 京ICP备2023020795号-1