Jinlong Liu , Qingxian Liu , Peng Dong , Weijian Ding , Quan Wang
{"title":"方形棱镜的直线和旋转流激振动的统一框架","authors":"Jinlong Liu , Qingxian Liu , Peng Dong , Weijian Ding , Quan Wang","doi":"10.1016/j.ijmecsci.2025.110876","DOIUrl":null,"url":null,"abstract":"<div><div>A unified framework is developed in this study to investigate the flow-induced vibrations of a square prism along a circular trajectory, bridging the gap between rectilinear and rotational flow-induced vibrations (FIVs) and aiming to offer an interconnected perspective for understanding the underlying physical mechanisms of fluid-structure interactions. Comprehensive analyses of the vibration responses, phase portrait evolutions, vortex shedding patterns, work-energy characteristics, and surface pressure distributions of the square prism undergoing vortex-induced vibration and galloping are conducted using this framework and validated against experimental data. The above analyses over a wide range of trajectory radii spanning from 0.1 <em>D</em> to 100 <em>D</em> (where <em>D</em> denotes the side length of the square prism) and a broad variety of airflow velocities ranging from 0.1 m/s to 3.0 m/s, are performed for concave and convex configurations corresponding to equilibrium circular trajectory angles of 0<sup>°</sup> and 180<sup>°</sup>, respectively. Three principal observations are obtained. The introduction of a finite trajectory radius <em>R</em> results in configuration-dependent dynamical evolution pathways from rectilinear (<em>R</em>→∞) to rotational (<em>R</em> = 0) FIVs. For the concave configuration, the flow-body system sequentially undergoes galloping for <em>R</em>/<em>D</em> > 2, forced vibrations for 0.2 ≤ <em>R</em>/<em>D</em> ≤ 2, and classical vortex-induced vibrations (VIVs) at <em>R</em> = 0. In contrast, the convex configuration demonstrates three distinct dynamic regimes: galloping for <em>R</em>/<em>D</em> ≥ 2, subharmonic VIV for 0.4 ≤ <em>R</em>/<em>D</em> ≤ 1, and classical VIV for <em>R</em>/<em>D</em> ≤ 0.2. Moreover, the subharmonic VIV regime is characterized by the emergence of an upper branch triggered by a 2P (two-pair) wake mode and a higher branch triggered by either a 4(2S) or 6(2S) wake mode, corresponding to four or six successive two-single vortex shedding patterns within each oscillation cycle. Additionally, the excitation mechanism underlying FIVs is dictated by the sign of aerodynamic work: positive work gives rise to large-amplitude synchronization branches, whereas negative work leads to small-amplitude desynchronization branches.</div></div>","PeriodicalId":56287,"journal":{"name":"International Journal of Mechanical Sciences","volume":"306 ","pages":"Article 110876"},"PeriodicalIF":9.4000,"publicationDate":"2025-09-22","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":"0","resultStr":"{\"title\":\"A unified framework for rectilinear and rotational flow-induced vibrations of a square prism\",\"authors\":\"Jinlong Liu , Qingxian Liu , Peng Dong , Weijian Ding , Quan Wang\",\"doi\":\"10.1016/j.ijmecsci.2025.110876\",\"DOIUrl\":null,\"url\":null,\"abstract\":\"<div><div>A unified framework is developed in this study to investigate the flow-induced vibrations of a square prism along a circular trajectory, bridging the gap between rectilinear and rotational flow-induced vibrations (FIVs) and aiming to offer an interconnected perspective for understanding the underlying physical mechanisms of fluid-structure interactions. Comprehensive analyses of the vibration responses, phase portrait evolutions, vortex shedding patterns, work-energy characteristics, and surface pressure distributions of the square prism undergoing vortex-induced vibration and galloping are conducted using this framework and validated against experimental data. The above analyses over a wide range of trajectory radii spanning from 0.1 <em>D</em> to 100 <em>D</em> (where <em>D</em> denotes the side length of the square prism) and a broad variety of airflow velocities ranging from 0.1 m/s to 3.0 m/s, are performed for concave and convex configurations corresponding to equilibrium circular trajectory angles of 0<sup>°</sup> and 180<sup>°</sup>, respectively. Three principal observations are obtained. The introduction of a finite trajectory radius <em>R</em> results in configuration-dependent dynamical evolution pathways from rectilinear (<em>R</em>→∞) to rotational (<em>R</em> = 0) FIVs. For the concave configuration, the flow-body system sequentially undergoes galloping for <em>R</em>/<em>D</em> > 2, forced vibrations for 0.2 ≤ <em>R</em>/<em>D</em> ≤ 2, and classical vortex-induced vibrations (VIVs) at <em>R</em> = 0. In contrast, the convex configuration demonstrates three distinct dynamic regimes: galloping for <em>R</em>/<em>D</em> ≥ 2, subharmonic VIV for 0.4 ≤ <em>R</em>/<em>D</em> ≤ 1, and classical VIV for <em>R</em>/<em>D</em> ≤ 0.2. Moreover, the subharmonic VIV regime is characterized by the emergence of an upper branch triggered by a 2P (two-pair) wake mode and a higher branch triggered by either a 4(2S) or 6(2S) wake mode, corresponding to four or six successive two-single vortex shedding patterns within each oscillation cycle. Additionally, the excitation mechanism underlying FIVs is dictated by the sign of aerodynamic work: positive work gives rise to large-amplitude synchronization branches, whereas negative work leads to small-amplitude desynchronization branches.</div></div>\",\"PeriodicalId\":56287,\"journal\":{\"name\":\"International Journal of Mechanical Sciences\",\"volume\":\"306 \",\"pages\":\"Article 110876\"},\"PeriodicalIF\":9.4000,\"publicationDate\":\"2025-09-22\",\"publicationTypes\":\"Journal Article\",\"fieldsOfStudy\":null,\"isOpenAccess\":false,\"openAccessPdf\":\"\",\"citationCount\":\"0\",\"resultStr\":null,\"platform\":\"Semanticscholar\",\"paperid\":null,\"PeriodicalName\":\"International Journal of Mechanical Sciences\",\"FirstCategoryId\":\"5\",\"ListUrlMain\":\"https://www.sciencedirect.com/science/article/pii/S0020740325009580\",\"RegionNum\":1,\"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":"International Journal of Mechanical Sciences","FirstCategoryId":"5","ListUrlMain":"https://www.sciencedirect.com/science/article/pii/S0020740325009580","RegionNum":1,"RegionCategory":"工程技术","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":null,"EPubDate":"","PubModel":"","JCR":"Q1","JCRName":"ENGINEERING, MECHANICAL","Score":null,"Total":0}
A unified framework for rectilinear and rotational flow-induced vibrations of a square prism
A unified framework is developed in this study to investigate the flow-induced vibrations of a square prism along a circular trajectory, bridging the gap between rectilinear and rotational flow-induced vibrations (FIVs) and aiming to offer an interconnected perspective for understanding the underlying physical mechanisms of fluid-structure interactions. Comprehensive analyses of the vibration responses, phase portrait evolutions, vortex shedding patterns, work-energy characteristics, and surface pressure distributions of the square prism undergoing vortex-induced vibration and galloping are conducted using this framework and validated against experimental data. The above analyses over a wide range of trajectory radii spanning from 0.1 D to 100 D (where D denotes the side length of the square prism) and a broad variety of airflow velocities ranging from 0.1 m/s to 3.0 m/s, are performed for concave and convex configurations corresponding to equilibrium circular trajectory angles of 0° and 180°, respectively. Three principal observations are obtained. The introduction of a finite trajectory radius R results in configuration-dependent dynamical evolution pathways from rectilinear (R→∞) to rotational (R = 0) FIVs. For the concave configuration, the flow-body system sequentially undergoes galloping for R/D > 2, forced vibrations for 0.2 ≤ R/D ≤ 2, and classical vortex-induced vibrations (VIVs) at R = 0. In contrast, the convex configuration demonstrates three distinct dynamic regimes: galloping for R/D ≥ 2, subharmonic VIV for 0.4 ≤ R/D ≤ 1, and classical VIV for R/D ≤ 0.2. Moreover, the subharmonic VIV regime is characterized by the emergence of an upper branch triggered by a 2P (two-pair) wake mode and a higher branch triggered by either a 4(2S) or 6(2S) wake mode, corresponding to four or six successive two-single vortex shedding patterns within each oscillation cycle. Additionally, the excitation mechanism underlying FIVs is dictated by the sign of aerodynamic work: positive work gives rise to large-amplitude synchronization branches, whereas negative work leads to small-amplitude desynchronization branches.
期刊介绍:
The International Journal of Mechanical Sciences (IJMS) serves as a global platform for the publication and dissemination of original research that contributes to a deeper scientific understanding of the fundamental disciplines within mechanical, civil, and material engineering.
The primary focus of IJMS is to showcase innovative and ground-breaking work that utilizes analytical and computational modeling techniques, such as Finite Element Method (FEM), Boundary Element Method (BEM), and mesh-free methods, among others. These modeling methods are applied to diverse fields including rigid-body mechanics (e.g., dynamics, vibration, stability), structural mechanics, metal forming, advanced materials (e.g., metals, composites, cellular, smart) behavior and applications, impact mechanics, strain localization, and other nonlinear effects (e.g., large deflections, plasticity, fracture).
Additionally, IJMS covers the realms of fluid mechanics (both external and internal flows), tribology, thermodynamics, and materials processing. These subjects collectively form the core of the journal's content.
In summary, IJMS provides a prestigious platform for researchers to present their original contributions, shedding light on analytical and computational modeling methods in various areas of mechanical engineering, as well as exploring the behavior and application of advanced materials, fluid mechanics, thermodynamics, and materials processing.