首页> 外文期刊>International Journal of Heat and Fluid Flow >Flow evolution of a turbulent submerged two-dimensional rectangular free jet of air. Average Particle Image Velocimetry (PIV) visualizations and measurements
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Flow evolution of a turbulent submerged two-dimensional rectangular free jet of air. Average Particle Image Velocimetry (PIV) visualizations and measurements

机译:湍流淹没的二维矩形自由空气流动的演变。平均粒子图像测速(PIV)可视化和测量

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The paper presents average flow visualizations and measurements, obtained with the Particle Image Velocimetry (PIV) technique, of a submerged rectangular free jet of air in the range of Reynolds numbers from Re = 35,300 to Re = 2200, where the Reynolds number is defined according to the hydraulic diameter of a rectangular slot of height H. According to the literature, just after the exit of the jet there is a zone of flow, called zone of flow establishment, containing the region of mixing fluid, at the border with the stagnant fluid, and the potential core, where velocity on the centerline maintains a value almost equal to the exit one. After this zone is present the zone of established flow or fully developed region. The goal of the paper is to show, with average PIV visualizations and measurements, that, before the zone of flow establishment is present a region of flow, never mentioned by the literature and called undisturbed region of flow, with a length, L_u, which decreases with the increase of the Reynolds number. The main characteristics of the undisturbed region is the fact that the velocity profile maintains almost equal to the exit one, and can also be identified by a constant height of the average PIV visualizations, with length, L_(CH), or by a constant turbulence on the centerline, with length L_(CT) The average PIV velocity and turbulence measurements are compared to those performed with the Hot Film Anemometry (HFA) technique. The average PIV visualizations show that the region of constant height has a length L_(CH) which increases from L_(CH) = H at Re = 35,300 to L_(CH) = 4-5H at Re = 2200. The PIV measurements on the centerline of the jet show that turbulence remains constant at the level of the exit for a length, L_(CH), which increases from Lcr = H at Re = 35,300 to L_(CH) = 4-5H at Re = 2200. The PIV measurements show that velocity remains constant at the exit level for a length, L_U, which increases from L_U = H at Re = 35,300 to L_U = 6H at Re = 2200 and is called undisturbed region of flow. In turbulent flow the length L_U is almost equal to the lengths of the regions of constant height, L_(CH), and constant turbulence, L_(CH)- In laminar flow, Re = 2200, the length of the undisturbed region of flow, L_U, is greater than the lengths of the regions of constant height and turbulence, L_(CH)=L_(CH) = 4-5H. The average PIV and HFA velocity measurements confirm that the length of potential core, L_p, increases from L_p = 4-5H at Re - 35,300 to L_p = 7-8H at Re = 2200, and are compared to the previous experimental and theoretical results of the literature in the zone of mixing fluid and in the fully developed region with a good agreement.
机译:本文介绍了通过颗粒图像测速(PIV)技术获得的平均水下流动可视化和测量结果,这些测量是在雷诺数从Re = 35,300到Re = 2200的范围内的水下矩形自由射流中进行的,其中雷诺数是根据高度为H的矩形槽的水力直径。根据文献,在射流出口之后,有一个流动区域,称为流动建立区域,在与停滞点的边界处包含混合流体区域。流体和潜在的核心,中心线上的速度保持几乎等于出口的速度。在该区域之后是已建立流量或完全发育区域。本文的目标是通过平均的PIV可视化和测量结果表明,在流动建立区域出现之前,存在一个流动区域,该流动区域未被文献所提及,被称为不受干扰的流动区域,其长度为L_u,该长度为L_u。随着雷诺数的增加而减小。不受干扰区域的主要特征是速度分布几乎与出口保持一致,也可以通过平均PIV可视化的恒定高度,长度L_(CH)或恒定的湍流来识别。在中心线上,长度为L_(CT),将平均PIV速度和湍流测量结果与热膜风速仪(HFA)技术进行的测量结果进行比较。 PIV的平均可视化结果显示,恒定高度的区域的长度L_(CH)从Re = 35,300时的L_(CH)= H增加到Re = 2200时的L_(CH)= 4-5H。射流的中心线表明,在出口L处,湍流保持恒定L_(CH),从Re = 35,300时的Lcr = H增加到Re = 2200时的L_(CH)= 4-5H。PIV测量表明,在出口L处,速度在长度L_U上保持恒定,该长度从Re = 35,300时的L_U = H增大到Re = 2200时的L_U = 6H,被称为流动的不受干扰区域。在湍流中,长度L_U几乎等于恒定高度L_(CH)和恒定湍流L_(CH)的区域的长度-在层流中,Re = 2200,即不受干扰的流动区域的长度, L_U大于恒定高度和湍流区域的长度,L_(CH)= L_(CH)= 4-5H。 PIV和HFA的平均速度测量结果证实,潜在磁芯的长度L_p从Re-35,300处的L_p = 4-5H增加到Re = 2200处的L_p = 7-8H,并与之前的实验和理论结果进行了比较在混合流体区域和充分发达的地区,文献具有很好的一致性。

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