燃气涡轮发动机叶片前缘周围气流中冷却膜形成的数字微粒图像可视化

IF 0.9 Q4 ENERGY & FUELS Thermal Engineering Pub Date : 2024-07-27 DOI:10.1134/S0040601524700137
S. V. Veretennikov, O. A. Evdokimov, A. A. Kolesova, K. A. Vinogradov, A. I. Gur’yanov
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引用次数: 0

摘要

摘要 介绍了利用粒子图像可视化技术在涡轮喷嘴叶片穿孔前缘附近测量的速度场。非接触式测量是在一个由三个喷嘴叶片组成的平面区段内进行的,该平面区段具有一个光学透明的入口区段,高速相机和激光片可以直观地进入中央叶片的前缘区域。实验研究是在 33 米/秒的固定进气流速下进行的,通过冷却孔的相对空气流速从 1.6% 到 6.4% 不等。对三种不同型号的叶片前缘附近的冷却膜流进行了观察,这些叶片在孔的供气方式、孔的直径和数量上各不相同。从一个空腔向冷却孔供应冷却剂会导致前缘上的冷却膜分布高度不均匀,这是因为通过靠近吸气侧的孔喷射的冷却剂具有较高的吹气比。实验结果表明,向压力侧、前缘和吸入尺寸上的孔分别供应冷却空气,可最大限度地降低形成的薄膜厚度对冷却剂相对流速的敏感性,并在 0.5 至 2.5 的较大喷射比范围内,使冷却剂在叶片表面的分布更加均匀。可视化显示了沿叶片翼面的薄膜流的广泛不稳定性。在这种情况下,通过中心孔送入的冷却射流会发生摆动,从而导致在压力侧或吸入侧周期性地形成薄膜。
本文章由计算机程序翻译,如有差异,请以英文原文为准。

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Digital Particle Image Visualization of the Cooling Film Formation in a Flow Around the Leading Edge of a Vane in a Gas Turbine Engine

Velocity fields measured in the vicinity of the perforated leading edge of a turbine nozzle vane using the particle image visualization technique are presented. Noncontact measurements were performed in a plane segment consisting of three nozzle vanes and having an optically transparent inlet section offering visual access to the region of the leading edge of the central vane for a high-speed camera and to the laser sheet. The experimental investigations were performed at a fixed incoming flow velocity of 33 m/s, and the relative air flowrate through the cooling holes varied from 1.6 to 6.4%. The cooling film flow near the leading edge was visualized for three models of vanes differing in the air supply method to the holes, hole diameter, and number. Supply of the coolant to the cooling holes from one cavity resulted in a high degree of nonuniformity in the distribution of the film over the leading edge, which was caused by a high blowing ratio for the jets injected through holes located closer to the suction side. The experimental results have revealed that separate supply of cooling air to the holes on the pressure side, leading edge, and suction size minimizes sensitivity of the formed film thickness to the relative flow rate of the coolant and provides a more uniform distribution of the coolant over the vane surface in a wide range of the blowing ratio for the jets that varies from 0.5 to 2.5. Visualization has demonstrated extensive unsteadiness of the film flow along the vane airfoil. In this case, the cooling jet fed through the central hole oscillates, thereby leading to periodic formation of a film on either the pressure side or the suction side.

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来源期刊
CiteScore
1.30
自引率
20.00%
发文量
94
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