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Large eddy simulation of base drag reduction using jet boat tail passive flow control

机译:基于喷射船尾部被动流量控制的基础减阻的大型涡流模拟

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摘要

This study conducts an implicit large eddy simulation (ILES) of jet boat tail (JBT) flows to investigate its drag reduction mechanism. The concept of JBT passive flow control is to create a circumferential jet around a bluff body toward the center of the base area. It forms a jet cone to have the similar effect of a solid boat tail. The LES is performed for a baseline bluff body and a JBT model modified from the baseline. The LES predicts that the JBT reduces the averaged drag coefficient by 19.3%, a reasonable agreement with the experimental drag reduction of 22.5%. The reduced averaged wake area is also observed for the JBT model, resulting in a decreased drag. In addition, the unsteady flow structures of the baseline and JBT flow are analyzed to study the flow mixing and entrainment mechanism. For the baseline configuration, the coherent vortex structures occur far downstream of the base surface. It hence does not have strong entrainment and energy transfer from freestream to the base area. For the JBT flow, a pulsative jet is induced by the vortex shedding of the shear layer and interacts immediately with the shear layer near the base surface. It generates the small structures that are substantially larger than those of the baseline configuration. The larger vortex structures of JBT enhance the flow entrainment and transfer more energy from the freestream to the base area. It results in higher static pressure in the base area that substantially reduces the pressure drag. Proper orthogonal decomposition of flow field reveals the periodic jet pulsation pattern in the azimuthal direction. (C) 2019 Elsevier Ltd. All rights reserved.
机译:本研究开展了喷射船尾(JBT)流的隐式大涡模拟(ILE),以研究其阻力减压机制。 JBT被动流量控制的概念是在朝向基部区域的中心围绕凹槽体产生圆周射流。它形成射流,具有固体船尾的类似效果。对基线诈唬主体进行的LES和从基线修改的JBT模型。 LES预测,JBT将平均拖累系数降低了19.3%,合理协议与实验阻力减少22.5%。对于JBT模型,也观察到降低的平均唤醒区域,导致阻力下降。此外,分析了基线和JBT流的不稳定流动结构,以研究流动混合和夹带机构。对于基线配置,相干涡流结构远离基面下游。因此,它没有从FreeStream到基地区域的强烈夹带和能量转移。对于JBT流,通过剪切层的涡流缩放诱导脉动射流,并立即与基部附近的剪切层相互作用。它产生基本上大于基线配置的小结构。 JBT的较大涡旋结构增强了流动夹带,并将更多能量从FreeStream转移到基地区域。它导致基本区域的静态压力较高,基本上减小了压力阻力。流场的适当正交分解揭示了方位角方向上的周期性喷射脉动图案。 (c)2019年elestvier有限公司保留所有权利。

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  • 来源
    《Computers & Fluids》 |2020年第2020期|共13页
  • 作者单位

    Univ Miami Dept Mech &

    Aerosp Engn Coral Gables FL 33124 USA;

    Univ Miami Dept Mech &

    Aerosp Engn Coral Gables FL 33124 USA;

    Univ Miami Dept Mech &

    Aerosp Engn Coral Gables FL 33124 USA;

    Univ Miami Dept Mech &

    Aerosp Engn Coral Gables FL 33124 USA;

    Univ Miami Dept Mech &

    Aerosp Engn Coral Gables FL 33124 USA;

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  • 正文语种 eng
  • 中图分类 计算机的应用;
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