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在康达效应滞后现象背景下平板上的压力分布。

Pressure distribution on a flat plate in the context of the phenomenon of the Coanda effect hysteresis.

作者信息

Skotnicka-Siepsiak Aldona

机构信息

Faculty of Geoengineering, University of Warmia and Mazury in Olsztyn, Heweliusza 4, 10-724, Olsztyn, Poland.

出版信息

Sci Rep. 2022 Jul 25;12(1):12687. doi: 10.1038/s41598-022-17031-3.

DOI:10.1038/s41598-022-17031-3
PMID:35879342
原文链接:https://pmc.ncbi.nlm.nih.gov/articles/PMC9314395/
Abstract

As a result of the Coanda effect, a symmetrical free jet will flow as an asymmetrical wall jet. At the same time, at the obstacle along which the flow is observed, the wall jet generates pressure distribution. In this study, the obstacle located at the diffuser outlet is a flat plate with a variable inclination angle. The article presents results of the study on pressure distributions on a flat plate with a variable angle of inclination. In the experiment, the Reynolds number ranged from 16,192 to 42,240. A fixed geometry diffuser (Witoszyński nozzle) with a height of 0.60 m, width of 0.02 m and outlet velocity of 11.33-29.57 m/s was used. A plate with a length of 1.00 m and a variable inclination angle was installed at the diffuser outlet. What is new, however, is that the presented results of the experimental research include the influence of the Coanda effect hysteresis on the pressure distribution on the plate. The article shows how pressure distributions change on the plate depending on whether the initial angle of inclination was 0° and was increased gradually in the course of the experiment until a detachment of the jet flowing from the plate was observed, or the initial angle of inclination was close to 90° in the primal state and as the angle of the plate inclination was decreased, the jet flowing towards the plate reached the state of attachment to the plate surface. The study demonstrated that for a turbulent jet, pressure distribution on a flat plate is determined not only by the plate's inclination angle, but also by the direction of its rotation.

摘要

由于康达效应,对称自由射流会以不对称壁面射流的形式流动。与此同时,在观察到流动的障碍物处,壁面射流会产生压力分布。在本研究中,位于扩散器出口处的障碍物是一块倾斜角度可变的平板。本文呈现了关于倾斜角度可变的平板上压力分布的研究结果。实验中,雷诺数范围为16192至42240。使用了一个固定几何形状的扩散器(维托申斯基喷嘴),其高度为0.60米,宽度为0.02米,出口速度为11.33 - 29.57米/秒。在扩散器出口处安装了一块长度为1.00米且倾斜角度可变的平板。然而,新的是,所呈现的实验研究结果包括康达效应滞后对平板上压力分布的影响。本文展示了平板上的压力分布如何根据初始倾斜角度是0°并在实验过程中逐渐增大直至观察到从平板流出的射流分离,还是初始倾斜角度在初始状态下接近90°且随着平板倾斜角度减小,流向平板的射流达到附着在平板表面的状态而发生变化。研究表明,对于湍流射流,平板上的压力分布不仅取决于平板的倾斜角度,还取决于其旋转方向。