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Flow-induced vibration of an elastically mounted oblate spheroid with variable mass ratio 变质量比弹性椭球体的流激振动
IF 2.6 3区 工程技术 Q2 ENGINEERING, MECHANICAL Pub Date : 2025-11-24 DOI: 10.1016/j.ijheatfluidflow.2025.110129
Adrian Cordero Obando , Kerry Hourigan , Mark C. Thompson , Jisheng Zhao
<div><div>This study experimentally investigates the cross-flow flow-induced vibration (FIV) of an elastically mounted oblate spheroid with an aspect ratio of 2. The aspect ratio is 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, namely <span><math><mrow><mi>ϵ</mi><mo>=</mo><mi>b</mi><mo>/</mo><mi>a</mi></mrow></math></span>. The FIV response was characterised 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>5000</mn><mo>⩽</mo><mi>R</mi><mi>e</mi><mo>=</mo><mi>U</mi><mi>b</mi><mo>/</mo><mi>ν</mi><mo>⩽</mo><mn>20</mn><mspace></mspace><mn>000</mn></mrow></math></span>, with <span><math><mi>ν</mi></math></span> denoting the kinematic viscosity of the fluid. The mass ratio of the hydro-elastic system, defined as the ratio of the total oscillating mass (<span><math><mi>m</mi></math></span>) to the displaced fluid mass (<span><math><msub><mrow><mi>m</mi></mrow><mrow><mi>d</mi></mrow></msub></math></span>), namely <span><math><mrow><msup><mrow><mi>m</mi></mrow><mrow><mo>∗</mo></mrow></msup><mo>=</mo><mi>m</mi><mo>/</mo><msub><mrow><mi>m</mi></mrow><mrow><mi>d</mi></mrow></msub></mrow></math></span>, was varied from 32 to 250, while the mass-damping parameter <span><math><mrow><mrow><mo>(</mo><msup><mrow><mi>m</mi></mrow><mrow><mo>∗</mo></mrow></msup><mo>+</mo><msub><mrow><mi>C</mi></mrow><mrow><mi>A</mi></mrow></msub><mo>)</mo></mrow><mi>ζ</mi></mrow></math></span> was kept almost constant at 0.20 for all the <span><math><msup><mrow><mi>m</mi></mrow><mrow><mo>∗</mo></mrow></msup></math></span> values tested, with <span><math><msub><mrow><mi>C</mi></mrow><mrow><mi>A</mi></mrow></msub></math></span> being the potential added-mass coefficient. The results reveal that the dynamic response exhibits two distinct FIV phenomena: vortex-induced vibration (VIV) and galloping-like vibration. The VIV region is characterised by a roughly bell-shaped and bounded amplitude of vibration response as a function of reduced velocity. The peak normalised vibration amplitude was observed to be <span><math><mrow><msubsup><mrow><mi>A</mi></mrow><mrow><mn>10</mn></mrow><mrow><mo>∗</mo></mrow></msubsup><mo>=</mo><mn>0</mn><mo>.</mo><mn>70</mn></mrow></math></span>. On the other hand, the galloping region is characterised by a
实验研究了长径比为2的弹性椭球体的横流流激振动。纵横比定义为横流方向的大直径(b)与顺流方向的小直径(a)之比,即λ =b/a。FIV响应的特征是在一个降低的速度范围内,3.0≤U∗=U/(fnwb)≤12.0,其中U为自由流速度,fnw为静水中系统的固有频率。对应的雷诺数在5000≤Re=Ub/ν≤20000范围内变化,ν表示流体的运动粘度。水弹性系统的质量比,定义为总振荡质量(m)与位移流体质量(md)之比,即m∗=m/md,从32变化到250,而质量阻尼参数(m∗+CA)ζ在所有测试的m∗值中几乎保持恒定在0.20,CA是潜在的附加质量系数。结果表明,动态响应表现出两种不同的FIV现象:涡激振动和驰动振动。VIV区域的特征是振动响应的大致钟形和有界振幅作为降低速度的函数。峰归一化振动幅值为A10 * =0.70。另一方面,驰骋区域的特征是振幅响应随U∗的增加而线性增加,超过临界值U∗=7.0,在测试的最高减速速度U∗=12时达到最大值A10∗≈2。有趣的是,保持(m∗+CA)ζ的恒定值而改变m∗会导致在m∗的大范围内几乎相同的最大振幅响应,类似于圆柱体的VIV。此外,发现m∗=32显示出硬策动样(即由有限幅度干扰触发的振动的开始)响应,而对于m∗大于或等于50的响应的特征是软策动样(即来自静止的小幅度激励)响应。
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The FIV response was characterised over a range of reduced velocity, &lt;span&gt;&lt;math&gt;&lt;mrow&gt;&lt;mn&gt;3&lt;/mn&gt;&lt;mo&gt;.&lt;/mo&gt;&lt;mn&gt;0&lt;/mn&gt;&lt;mo&gt;⩽&lt;/mo&gt;&lt;msup&gt;&lt;mrow&gt;&lt;mi&gt;U&lt;/mi&gt;&lt;/mrow&gt;&lt;mrow&gt;&lt;mo&gt;∗&lt;/mo&gt;&lt;/mrow&gt;&lt;/msup&gt;&lt;mo&gt;=&lt;/mo&gt;&lt;mi&gt;U&lt;/mi&gt;&lt;mo&gt;/&lt;/mo&gt;&lt;mrow&gt;&lt;mo&gt;(&lt;/mo&gt;&lt;msub&gt;&lt;mrow&gt;&lt;mi&gt;f&lt;/mi&gt;&lt;/mrow&gt;&lt;mrow&gt;&lt;mi&gt;n&lt;/mi&gt;&lt;mi&gt;w&lt;/mi&gt;&lt;/mrow&gt;&lt;/msub&gt;&lt;mi&gt;b&lt;/mi&gt;&lt;mo&gt;)&lt;/mo&gt;&lt;/mrow&gt;&lt;mo&gt;⩽&lt;/mo&gt;&lt;mn&gt;12&lt;/mn&gt;&lt;mo&gt;.&lt;/mo&gt;&lt;mn&gt;0&lt;/mn&gt;&lt;/mrow&gt;&lt;/math&gt;&lt;/span&gt;, where &lt;span&gt;&lt;math&gt;&lt;mi&gt;U&lt;/mi&gt;&lt;/math&gt;&lt;/span&gt; is the free-stream velocity and &lt;span&gt;&lt;math&gt;&lt;msub&gt;&lt;mrow&gt;&lt;mi&gt;f&lt;/mi&gt;&lt;/mrow&gt;&lt;mrow&gt;&lt;mi&gt;n&lt;/mi&gt;&lt;mi&gt;w&lt;/mi&gt;&lt;/mrow&gt;&lt;/msub&gt;&lt;/math&gt;&lt;/span&gt; is the natural frequency of the system in quiescent water. The corresponding Reynolds number varied over the range &lt;span&gt;&lt;math&gt;&lt;mrow&gt;&lt;mn&gt;5000&lt;/mn&gt;&lt;mo&gt;⩽&lt;/mo&gt;&lt;mi&gt;R&lt;/mi&gt;&lt;mi&gt;e&lt;/mi&gt;&lt;mo&gt;=&lt;/mo&gt;&lt;mi&gt;U&lt;/mi&gt;&lt;mi&gt;b&lt;/mi&gt;&lt;mo&gt;/&lt;/mo&gt;&lt;mi&gt;ν&lt;/mi&gt;&lt;mo&gt;⩽&lt;/mo&gt;&lt;mn&gt;20&lt;/mn&gt;&lt;mspace&gt;&lt;/mspace&gt;&lt;mn&gt;000&lt;/mn&gt;&lt;/mrow&gt;&lt;/math&gt;&lt;/span&gt;, with &lt;span&gt;&lt;math&gt;&lt;mi&gt;ν&lt;/mi&gt;&lt;/math&gt;&lt;/span&gt; denoting the kinematic viscosity of the fluid. The mass ratio of the hydro-elastic system, defined as the ratio of the total oscillating mass (&lt;span&gt;&lt;math&gt;&lt;mi&gt;m&lt;/mi&gt;&lt;/math&gt;&lt;/span&gt;) to the displaced fluid mass (&lt;span&gt;&lt;math&gt;&lt;msub&gt;&lt;mrow&gt;&lt;mi&gt;m&lt;/mi&gt;&lt;/mrow&gt;&lt;mrow&gt;&lt;mi&gt;d&lt;/mi&gt;&lt;/mrow&gt;&lt;/msub&gt;&lt;/math&gt;&lt;/span&gt;), namely &lt;span&gt;&lt;math&gt;&lt;mrow&gt;&lt;msup&gt;&lt;mrow&gt;&lt;mi&gt;m&lt;/mi&gt;&lt;/mrow&gt;&lt;mrow&gt;&lt;mo&gt;∗&lt;/mo&gt;&lt;/mrow&gt;&lt;/msup&gt;&lt;mo&gt;=&lt;/mo&gt;&lt;mi&gt;m&lt;/mi&gt;&lt;mo&gt;/&lt;/mo&gt;&lt;msub&gt;&lt;mrow&gt;&lt;mi&gt;m&lt;/mi&gt;&lt;/mrow&gt;&lt;mrow&gt;&lt;mi&gt;d&lt;/mi&gt;&lt;/mrow&gt;&lt;/msub&gt;&lt;/mrow&gt;&lt;/math&gt;&lt;/span&gt;, was varied from 32 to 250, while the mass-damping parameter &lt;span&gt;&lt;math&gt;&lt;mrow&gt;&lt;mrow&gt;&lt;mo&gt;(&lt;/mo&gt;&lt;msup&gt;&lt;mrow&gt;&lt;mi&gt;m&lt;/mi&gt;&lt;/mrow&gt;&lt;mrow&gt;&lt;mo&gt;∗&lt;/mo&gt;&lt;/mrow&gt;&lt;/msup&gt;&lt;mo&gt;+&lt;/mo&gt;&lt;msub&gt;&lt;mrow&gt;&lt;mi&gt;C&lt;/mi&gt;&lt;/mrow&gt;&lt;mrow&gt;&lt;mi&gt;A&lt;/mi&gt;&lt;/mrow&gt;&lt;/msub&gt;&lt;mo&gt;)&lt;/mo&gt;&lt;/mrow&gt;&lt;mi&gt;ζ&lt;/mi&gt;&lt;/mrow&gt;&lt;/math&gt;&lt;/span&gt; was kept almost constant at 0.20 for all the &lt;span&gt;&lt;math&gt;&lt;msup&gt;&lt;mrow&gt;&lt;mi&gt;m&lt;/mi&gt;&lt;/mrow&gt;&lt;mrow&gt;&lt;mo&gt;∗&lt;/mo&gt;&lt;/mrow&gt;&lt;/msup&gt;&lt;/math&gt;&lt;/span&gt; values tested, with &lt;span&gt;&lt;math&gt;&lt;msub&gt;&lt;mrow&gt;&lt;mi&gt;C&lt;/mi&gt;&lt;/mrow&gt;&lt;mrow&gt;&lt;mi&gt;A&lt;/mi&gt;&lt;/mrow&gt;&lt;/msub&gt;&lt;/math&gt;&lt;/span&gt; being the potential added-mass coefficient. The results reveal that the dynamic response exhibits two distinct FIV phenomena: vortex-induced vibration (VIV) and galloping-like vibration. The VIV region is characterised by a roughly bell-shaped and bounded amplitude of vibration response as a function of reduced velocity. The peak normalised vibration amplitude was observed to be &lt;span&gt;&lt;math&gt;&lt;mrow&gt;&lt;msubsup&gt;&lt;mrow&gt;&lt;mi&gt;A&lt;/mi&gt;&lt;/mrow&gt;&lt;mrow&gt;&lt;mn&gt;10&lt;/mn&gt;&lt;/mrow&gt;&lt;mrow&gt;&lt;mo&gt;∗&lt;/mo&gt;&lt;/mrow&gt;&lt;/msubsup&gt;&lt;mo&gt;=&lt;/mo&gt;&lt;mn&gt;0&lt;/mn&gt;&lt;mo&gt;.&lt;/mo&gt;&lt;mn&gt;70&lt;/mn&gt;&lt;/mrow&gt;&lt;/math&gt;&lt;/span&gt;. On the other hand, the galloping region is characterised by a","PeriodicalId":335,"journal":{"name":"International Journal of Heat and Fluid Flow","volume":"117 ","pages":"Article 110129"},"PeriodicalIF":2.6,"publicationDate":"2025-11-24","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"145620164","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":3,"RegionCategory":"工程技术","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":"","EPubDate":null,"PubModel":null,"JCR":null,"JCRName":null,"Score":null,"Total":0}
引用次数: 0
Optimization of nanofluid impinging jet systems for advanced electronic cooling: A critical review 用于先进电子冷却的纳米流体冲击射流系统的优化:综述
IF 2.6 3区 工程技术 Q2 ENGINEERING, MECHANICAL Pub Date : 2025-11-24 DOI: 10.1016/j.ijheatfluidflow.2025.110149
P. Balakrishnan
This review critically examines the integration of nanofluid properties and impinging jet configurations for enhanced electronic cooling applications, addressing thermal management challenges in an electronics market projected to reach USD 1,406.47 billion by 2034, where more than 55 % of failures are heat-related. The synergistic potential of Al2O3, CuO, TiO2, SiC, and hybrid nanofluids is analysed, revealing heat transfer enhancements of 15–72 %, although performance strongly depends on operational parameters. Single jet systems deliver concentrated cooling with optimal efficiency at H/D ratios of 5–8, achieving peak Nusselt numbers near 7–8, whereas multiple jets ensure more uniform heat dissipation at lower H/D ratios (≈2) and intermediate S/D ratios (≈3), achieving a balanced trade-off between turbulence intensity, jet interaction, and surface cooling uniformity. However, multiple jets face challenges related to flow distribution and pressure drop. Hybrid nanofluids, particularly Al2O3–Cu combinations, exhibit Nusselt number increases of 63.5 % at Re = 24,000, demonstrating favourable performance–stability trade-offs. Nanoparticle characteristics significantly influence system behaviour, with optimal concentrations between 0.5–2 % required to balance enhanced thermal conductivity and fluid stability. The findings highlight the potential of optimized nanofluid impinging jets to overcome critical electronic thermal bottlenecks. However, practical implementation faces challenges related to increased viscosity and pumping power, along with long-term stability issues, high synthesis costs, and environmental concerns in large-scale deployment. Addressing these challenges requires focused research on standardized nanofluid preparation protocols, improved stability and scalability, and comprehensive life-cycle assessments of hybrid nanofluids and advanced jet configurations.
这篇综述批判性地研究了纳米流体特性和冲击射流配置的集成,以增强电子冷却应用,解决电子市场的热管理挑战,预计到2034年将达到1,4064.7亿美元,其中55%以上的故障与热相关。分析了Al2O3、CuO、TiO2、SiC和混合纳米流体的协同潜力,揭示了15 - 72%的传热增强,尽管性能在很大程度上取决于操作参数。单射流系统在H/D比为5-8时提供最佳效率的集中冷却,峰值努塞尔数接近7-8,而多射流在较低的H/D比(≈2)和中间的S/D比(≈3)下确保更均匀的散热,实现湍流强度、射流相互作用和表面冷却均匀性之间的平衡。然而,多喷嘴面临着与流动分布和压降相关的挑战。杂化纳米流体,特别是Al2O3-Cu组合,在Re = 24000时,努塞尔数增加了63.5%,表现出良好的性能稳定性权衡。纳米颗粒的特性显著影响系统行为,最佳浓度在0.5 - 2%之间,以平衡增强的导热性和流体稳定性。这些发现突出了优化的纳米流体撞击射流在克服关键的电子热瓶颈方面的潜力。然而,在实际应用中面临着粘度和泵送功率增加、长期稳定性问题、高合成成本以及大规模部署时的环境问题等挑战。解决这些挑战需要集中研究标准化的纳米流体制备方案,提高稳定性和可扩展性,以及混合纳米流体和先进射流配置的全面生命周期评估。
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引用次数: 0
Effects of air-injection pressure and nozzle diameter on flow and cavitation characteristics of aerated submerged waterjet 喷气压力和喷嘴直径对加气水下水射流流动和空化特性的影响
IF 2.6 3区 工程技术 Q2 ENGINEERING, MECHANICAL Pub Date : 2025-11-23 DOI: 10.1016/j.ijheatfluidflow.2025.110154
Shifeng Yan , Can Kang , Haixia Liu , Guangxin Ding , Hyoung-Bum Kim
The present study aims to elucidate flow and cavitation characteristics of the aerated submerged waterjet. A numerical study is conducted using the method incorporating the large eddy simulation (LES) and Schnerr-Sauer cavitation models. The numerical scheme is validated through an experimental work of visualizing cavitation clouds in submerged waterjet. With two nozzles of 2.0 and 4.0 mm in diameter, evolution of cavitation clouds is illustrated and compared under non-aeration and different air-injection pressures. The results show that cavitation intensity and air-injection pressure are not monotonically related. For the nozzle of 4.0 mm in diameter, the cavitation volume fraction reaches its maximum at an air-injection pressure of 0.3 MPa and declines drastically with further increasing the air-injection pressure. The shedding frequency of cavitation clouds varies inversely with the air-injection pressure. When increasing air-injection pressure, vortex structures remain similar for the nozzle of 2.0 mm in diameter, while for the larger nozzle, long and straight vortex structures prevail. Integrity of vorticity rings attenuates continuously with increasing air-injection pressure. The conclusions are expected to shed light on the mechanisms underlying cavitation evolution and inter-phase interactions in the aerated submerged waterjet.
本研究的目的是研究加气水下水射流的流动和空化特性。采用大涡模拟(LES)和Schnerr-Sauer空化模型相结合的方法进行了数值研究。通过水下水射流中空化云的可视化实验验证了该方法的有效性。以直径为2.0 mm和4.0 mm的两种喷嘴为例,对比了在不充气和不同喷气压力下空化云的演变过程。结果表明,空化强度与空气注入压力不是单调相关的。对于直径为4.0 mm的喷嘴,空化体积分数在喷气压力为0.3 MPa时达到最大值,随着喷气压力的进一步增大,空化体积分数急剧下降。空化云的脱落频率与空气注入压力成反比。增大喷气压力时,直径为2.0 mm的喷嘴涡结构基本保持不变,而较大的喷嘴涡结构以长而直的涡结构为主。涡度环的完整性随着喷气压力的增加而不断衰减。这些结论有望揭示水下加气水射流中空化演化和相间相互作用的机制。
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引用次数: 0
Insights of quantitative imaging and instantaneous heat transfer coefficient measurement in spouted bed column 喷淋床柱定量成像及瞬时传热系数测量的研究进展
IF 2.6 3区 工程技术 Q2 ENGINEERING, MECHANICAL Pub Date : 2025-11-22 DOI: 10.1016/j.ijheatfluidflow.2025.110152
Hasan A. Abdulwahab , Abbas J. Sultan , Amer A. Abdulrahman , Haydar A.S. Aljaafari , Ali A. Yahya , Zahraa W. Hasan , Malik M. Mohammed , Laith S. Sabri , Bashar J. Kadhim , Jamal M. Ali , Muthanna H. Al-Dahhan
In this study, the heat transfer behavior of a conical spouted bed column was imaged for the first time across its entire cross-sectional area and at multiple axial heights. To achieve this, a custom-built quantitative imaging approach was developed. This method combined FluxTeq heat flux sensors with an Arduino-based data acquisition system. The experimental setup enabled instantaneous, spatially resolved measurements of surface temperature, heat flux, and local heat transfer coefficients (LHTC) under various operating conditions. Measurements at different radial locations, angles, and heights provided a comprehensive view of heat transfer behaviour throughout the column. The obtained cross-sectional images show that the magnitude of LHTC increases with both axial height and superficial gas velocity. Gains reached up to 25 % between the lowest and highest velocities tested. Time-resolved data reveal greater fluctuations in the central spout region, especially at higher axial positions (H/D = 2.1). These fluctuations promote vigorous convective exchange and reduce temperature non-uniformity. Persistent radial asymmetry was observed, linked to distinct hydrodynamic behaviors in the spout, annulus, and fountain zones. Increasing gas velocities further reduced the solids fraction in the reactor core, affecting heat flux and temperature distribution. This experiment effectively captures transient and spatial characteristics often missed by conventional methods. The resulting benchmark data support CFD model validation, guide reactor scale-up, and improve thermal management in industrial gas–solid systems.
在这项研究中,首次对锥形喷淋床柱在其整个横截面和多个轴向高度上的传热行为进行了成像。为了实现这一目标,开发了一种定制的定量成像方法。该方法将FluxTeq热流通量传感器与基于arduino的数据采集系统相结合。实验装置实现了在各种操作条件下的表面温度、热流密度和局部传热系数(LHTC)的瞬时、空间分辨测量。在不同的径向位置,角度和高度的测量提供了整个柱的传热行为的全面视图。得到的横截面图像表明,LHTC的大小随轴向高度和表面气速的增加而增加。在测试的最低和最高速度之间的增益达到25%。时间分辨数据显示,中央喷口区域波动较大,特别是在较高的轴向位置(H/D = 2.1)。这些波动促进了激烈的对流交换,减少了温度的不均匀性。观察到持续的径向不对称,这与喷口、环空和喷泉区不同的流体动力学行为有关。气速的增加进一步降低了堆芯中的固体分数,影响了热流密度和温度分布。该实验有效地捕获了传统方法常常遗漏的瞬态和空间特征。由此产生的基准数据支持CFD模型验证,指导反应器规模扩大,并改善工业气固系统的热管理。
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引用次数: 0
Patterned surface structures for passive control of surface-wave mode transitions 用于被动控制表面波模式转换的图案表面结构
IF 2.6 3区 工程技术 Q2 ENGINEERING, MECHANICAL Pub Date : 2025-11-22 DOI: 10.1016/j.ijheatfluidflow.2025.110143
Zihao Dong , Yan Xing , Qingfei Fu , Ruo-Yu Dong
Modulating the transition threshold of surface waves is of great significance in both scientific research and engineering applications. Traditional control methods—such as rigid structural constraints—often suffer from high energy consumption, slow response, and poor adaptability to complex boundary conditions. This study proposes and implements a patterned surface structure to regulate free-surface wave behavior. By introducing periodic adhesion contrast and curvature-induced disturbances, the pattern enables precise control over wall-bounded vorticity generation and dissipation pathways. During the subharmonic transition, shear disturbances induced at the wall enhance energy dissipation, thereby significantly increasing the critical threshold. Systematic experiments reveal the coupled effects of pattern parameters and fluid depth, demonstrating how structural tuning governs the spatial extent of wave response and the associated instability conditions. Furthermore, we find that once the fluid layer exceeds a critical thickness, the control effect of the pattern diminishes markedly. This work presents a lightweight, efficient strategy for surface wave suppression, offering a new paradigm for high-performance propulsion systems and liquid management in microgravity environments.
调制表面波的过渡阈值在科学研究和工程应用中都具有重要意义。传统的控制方法(如刚性结构约束)往往存在能耗高、响应慢、对复杂边界条件适应性差等问题。本研究提出并实现了一种模式表面结构来调节自由表面波的行为。通过引入周期性的粘附对比和曲率引起的扰动,该模式能够精确控制壁面涡量的产生和耗散路径。在亚谐波过渡期间,壁面处的剪切扰动增强了能量耗散,从而显著提高了临界阈值。系统实验揭示了模式参数和流体深度的耦合效应,展示了结构调谐如何控制波响应的空间范围和相关的不稳定条件。此外,我们发现,一旦流体层超过临界厚度,图案的控制效果显着减弱。这项工作提出了一种轻量、高效的表面波抑制策略,为微重力环境下的高性能推进系统和液体管理提供了新的范例。
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引用次数: 0
Flow and heat transfer of various internal cooling technologies for rotating blades: A review on recent twenty-years progress of experimental studies 各种旋转叶片内冷却技术的流动与传热:近二十年实验研究进展综述
IF 2.6 3区 工程技术 Q2 ENGINEERING, MECHANICAL Pub Date : 2025-11-20 DOI: 10.1016/j.ijheatfluidflow.2025.110145
Wenbin He , Jiang Lei , Gongnan Xie
Internal cooling technologies are essential for ensuring the reliable operation of gas turbine blades under extreme high-temperature environments. For rotating blades, Coriolis and rotational buoyancy effects critically alter the flow and heat transfer characteristics within internal cooling channels, which cannot be neglected. In this paper, a comparative analysis is first conducted on the advantages and limitations of measurement techniques including thermocouple-copper plate method, naphthalene sublimation methods, steady-state/transient liquid crystal thermography (LCT/TLCT), infrared thermography (IRT), laser doppler velocimetry (LDV), particle image velocimetry (PIV), and hot-wire anemometry (HWA), with focused discussions on the technical specifications of representative rotating test facilities. Subsequently, experimental data from multi-pass serpentine channels, pin–fin arrays channels, and impingement cooling channels are synthesized to elucidate the influence mechanisms of Coriolis and buoyancy effects on flow and heat transfer within the channels. Finally, recommendations are proposed for future experimental research. This literature review serves as a valuable reference for the design of rotating test facilities and the optimization of internal cooling structures in turbine rotor blades. This paper systematically reviews advancements in experimental studies on rotating internal cooling from the past two decades, while also referencing earlier and seminal works to provide foundational insights.
内部冷却技术对于保证燃气轮机叶片在极端高温环境下的可靠运行至关重要。对于旋转叶片,科里奥利效应和旋转浮力效应对内部冷却通道内的流动和换热特性有着不可忽视的影响。本文首先对比分析了热电偶-铜板法、萘升华法、稳态/瞬态液晶热成像法(LCT/TLCT)、红外热成像法(IRT)、激光多普勒测速法(LDV)、粒子图像测速法(PIV)、热线测速法(HWA)等测量技术的优缺点,重点讨论了具有代表性的旋转测试设备的技术指标。随后,综合了多通道蛇形通道、鳍状阵列通道和撞击冷却通道的实验数据,阐明了科里奥利效应和浮力效应对通道内流动和换热的影响机制。最后,对今后的实验研究提出了建议。本文的文献综述可为涡轮转子叶片旋转试验装置的设计和内部冷却结构的优化提供有价值的参考。本文系统地回顾了过去二十年来旋转内部冷却实验研究的进展,同时也参考了早期和开创性的工作,以提供基本的见解。
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引用次数: 0
Experimental research on the heat transfer performance of ultra-thin vapor chambers with composite wicks for electronics cooling 电子冷却用复合芯超薄蒸汽室换热性能实验研究
IF 2.6 3区 工程技术 Q2 ENGINEERING, MECHANICAL Pub Date : 2025-11-19 DOI: 10.1016/j.ijheatfluidflow.2025.110148
Tengqing Liu , Yaokang Zhang , Shuangfeng Wang , Qianxi Zhang , Huifeng Kang
Ultra-thin vapor chambers (UTVCs) have been proposed to address the high heat flux problem of portable electronic devices. In this study, five types of spiral woven mesh (SWM)-based UTVCs with a thickness of 0.4 mm were designed, namely, nine-wires SWM (NSWM), nine-wires SWM-wettability-patterned (NSWM-WP), nine-wires SWM-screen mesh (NSWM-SM), eight-wires SWM-WP (ESWM-WP) and eight-wires SWM-SM (ESWM-SM) UTVCs. The WP microstructure was fabricated on the bottom sheet via laser etching, and the SM was bonded on the bottom sheet. The effects of wick structure and orientation on heat transfer performance, including temperature distribution, heat source temperature, and thermal resistance, were investigated. The results indicated that the effect of wick structures and orientations on the heat source temperature was negligible at the same input power, but they affected the thermal resistance by redistributing the condensate on the bottom sheet. In addition, the SWM-WP and SWM-SM composite wicks substantially reduced the thermal resistance of the SWM-based UTVC. The maximum heat flux of all the designed UTVCs was 3.58 W/cm2, and the lowest equivalent thermal resistances of the NSWM, ESWM-WP, and ESWM-SM UTVCs were 1.750, 0.832, and 0.097 (cm2·K)/W, respectively.
为了解决便携式电子设备的高热流密度问题,提出了超薄蒸汽室(UTVCs)。本研究设计了五种厚度为0.4 mm的螺旋编织网(SWM) utvc,即九丝编织网(NSWM)、九丝编织网润湿性图案(NSWM- wp)、九丝编织网筛网(NSWM- sm)、八丝编织网wp (ESWM-WP)和八丝编织网sm (ESWM-SM) utvc。采用激光刻蚀法在底板上制备了WP微结构,并将SM粘结在底板上。研究了灯芯结构和取向对温度分布、热源温度和热阻等传热性能的影响。结果表明,在相同的输入功率下,灯芯结构和灯芯取向对热源温度的影响可以忽略不计,但灯芯结构和灯芯取向对热源温度的影响是通过底层冷凝水的再分布来影响热阻的。此外,SWM-WP和SWM-SM复合灯芯大大降低了swm基UTVC的热阻。所有设计的utvc的最大热通量为3.58 W/cm2, NSWM、ESWM-WP和ESWM-SM的最小等效热阻分别为1.750、0.832和0.097 (cm2·K)/W。
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引用次数: 0
Direct numerical simulation of a cantilevered rod experiment 悬臂杆试验的直接数值模拟
IF 2.6 3区 工程技术 Q2 ENGINEERING, MECHANICAL Pub Date : 2025-11-19 DOI: 10.1016/j.ijheatfluidflow.2025.110112
Sean Bistany, Victor Coppo Leite, Carolina Bourdot Dutra, Sinan Okyay, Anshuman Chaube, Tri Nguyen, Elia Merzari
Flow-induced vibrations may lead to grid-to-rod fretting, a wear phenomenon that remains the primary cause of fuel failures in pressurized water reactors. This study presents a high-fidelity Direct Numerical Simulation of turbulent flow around a cantilevered rod in a confining pipe, replicating an experiment from the University of Manchester and producing benchmark data for validating turbulence models within the GO-VIKING consortium. The simulations were performed using NekRS on the Frontier supercomputer, resolving the full turbulence spectrum. Verification and validation were achieved through canonical pipe flow analysis and experimental comparisons. Flow structures were analyzed via Q-criterion, Barycentric anisotropy maps, and full turbulent kinetic energy budgets, revealing strong anisotropy and local partial laminarization due to axisymmetric contraction, along with elevated pressure diffusion. These results provide insight into the mechanisms driving flow-induced vibrations and highlight limitations of conventional turbulence models, supporting the development of improved predictive tools for nuclear fuel design.
流动引起的振动可能导致电网到棒的微动,这是一种磨损现象,仍然是压水堆燃料故障的主要原因。这项研究提出了一个高保真的直接数值模拟,模拟了围流管内悬臂杆周围的湍流,复制了曼彻斯特大学的实验,并为GO-VIKING联盟的湍流模型验证提供了基准数据。模拟使用前沿超级计算机上的NekRS进行,解决了整个湍流谱。通过典型管流分析和实验对比,对该方法进行了验证。通过q准则、重心各向异性图和全湍流动能预算分析了流动结构,揭示了由于轴对称收缩和高压扩散而产生的强各向异性和局部部分层压化。这些结果提供了对驱动流动诱发振动的机制的深入了解,并突出了传统湍流模型的局限性,支持开发改进的核燃料设计预测工具。
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引用次数: 0
Study on fogging and defogging during the aircraft diving process 飞机潜水过程中起雾与除雾的研究
IF 2.6 3区 工程技术 Q2 ENGINEERING, MECHANICAL Pub Date : 2025-11-19 DOI: 10.1016/j.ijheatfluidflow.2025.110151
Jing-Jing Xu, Yi-Rong Gu, Xue-Li Li
Fog on the windshield of an aircraft can seriously block the view of the pilots and affect the flight safety. The transient changes of the flow field parameters inside and outside the aircraft cabin during the dive process are usually ignored in the existing research, which reduces the accuracy of fogging predictions. This paper employs transient simulation techniques to investigate the fogging and defogging behaviors in an aircraft equipped with a hot air defogging system during the aircraft diving process. The influence of atmospheric temperature, pressure, humidity and anti-fog/defog airflow with various parameters on the fog formation is analyzed. The results show that during the aircraft’s dive, as the pressure and humidity inside the cabin increase, fog gradually begins to form on the inner surface of the windshield. Activating the anti-fog airflow effectively delays this fogging process. For windshields with high thermal conductivity and low heat capacity, due to the increased influence of external temperature, when the aircraft descends to an altitude of about 1,000 m, the atmospheric inversion layer accelerates the fogging on the inner surface. When the aircraft dives into a low-altitude environment of high pressure and high humidity, the use of the high temperature defogging airflow may cause fog to form in some areas of the inner surface. In contrast, the 10 ℃ cold air defogging airflow does not cause to fog by avoiding significant temperature differences between the windshield and the near-wall air layer, even at humidity up to 30 g/(kg·dra). And the defogging rate distribution on the inner surface is more uniform than that of the hot air defogging.
飞机挡风玻璃上的雾会严重遮挡飞行员的视线,影响飞行安全。现有的研究往往忽略了俯冲过程中机舱内外流场参数的瞬态变化,从而降低了起雾预测的准确性。本文采用瞬态仿真技术研究了装有热空气除雾系统的飞机在俯冲过程中的起雾和除雾行为。分析了大气温度、气压、湿度和不同参数的防雾/除雾气流对雾形成的影响。结果表明,在飞机俯冲过程中,随着机舱内压力和湿度的增加,在挡风玻璃的内表面逐渐开始形成雾气。激活防雾气流有效地延缓了这个雾化过程。对于导热系数高、热容量低的挡风玻璃,由于外界温度的影响增大,当飞机下降到1000 m左右高度时,大气逆温层加速了内表面的起雾。当飞机潜入高压高湿的低空环境时,使用高温除雾气流可能会导致内表面某些区域形成雾。相比之下,即使在湿度高达30 g/(kg·dra)的情况下,10℃的冷空气除雾气流也不会引起雾,因为它避免了挡风玻璃和近壁空气层之间的显著温差。内表面的除雾率分布比热风除雾更均匀。
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引用次数: 0
Research on the optimal design of anti-collision heat pipe radiator for nuclear powered spacecraft 核动力航天器防碰撞热管散热器优化设计研究
IF 2.6 3区 工程技术 Q2 ENGINEERING, MECHANICAL Pub Date : 2025-11-17 DOI: 10.1016/j.ijheatfluidflow.2025.110141
Zengen Li , Haochun Zhang , Dong Zhang , Xi Luo , Yan Xia
The exponential increase of space debris will have serious consequences for the flight safety of nuclear-powered spacecraft. This research establishes a 2D calculation program 2D-INCHPR for in-direct contact heat pipe radiators. Based on the whale optimization algorithm, a multi objective optimization analysis of the radiator with multi parameter coupling is carried out. A space debris impact resistant radiator is devised without reducing heat transfer efficiency, providing a theoretical basis for structural optimization of space nuclear power system. The method of calculating alkali metal heat pipes transient and steady-state multi-physics coupling characteristics of in space nuclear power systems based on gas dynamics theory is extended to a 2D model of entire heat pipe domain. A 2D program 2D-NCAMHP is established for multi- physics coupling calculation of space alkali metal heat pipes. The optimized structural parameters of the radiation heat sink with low probability of space debris impact after optimization design are Lf = 0.0537 m, Tinl = 852.2493 K, lhpc = 1.9298 m, qm = 7.4340 kg·s-1. The thermal and hydraulic characteristics of alkali metal heat pipes were obtained through simulation analysis, which provides a theoretical basis for the optimization design of radiator structures in nuclear powered spacecraft.
空间碎片呈指数级增长,将对核动力航天器的飞行安全造成严重后果。本文建立了非直接接触热管散热器的二维计算程序2D- inchpr。基于鲸鱼优化算法,对多参数耦合的散热器进行了多目标优化分析。设计了一种不降低换热效率的空间碎片抗冲击散热器,为空间核动力系统结构优化提供了理论依据。将基于气体动力学理论的空间核动力系统碱金属热管瞬态和稳态多物理场耦合特性计算方法推广到整个热管域的二维模型。建立了用于空间碱金属热管多物理场耦合计算的二维程序2D- ncamhp。优化设计后低空间碎片撞击概率辐射散热器的优化结构参数为:Lf = 0.0537 m, Tinl = 852.2493 K, lhpc = 1.9298 m, qm = 7.4340 kg·s-1。通过仿真分析,获得了碱金属热管的热工特性,为核动力航天器散热器结构的优化设计提供了理论依据。
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引用次数: 0
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International Journal of Heat and Fluid Flow
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