双壁燃烧室衬垫稀释孔附近射流冷却模式的影响:第2部分——流场测量

Adam C. Shrager, K. Thole, Dominic Mongillo
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引用次数: 1

摘要

燃气轮机燃烧室内部复杂的流场给冷却燃烧室壁带来了困难的挑战。许多现代燃烧室都采用双壁设计,既包括壁面背面的撞击冷却,也包括壁面外侧的射流冷却。使问题更加复杂的是,这些双壁还包含大的稀释孔,由此,来自渗出孔的冷却膜被高动量稀释射流打断。考虑到冷却整个面板的重要性,包括稀释孔周围的金属,本文的重点是了解稀释孔附近区域的流动情况。在稀释孔附近对三种不同的射流冷却孔模式进行了近壁流场测量。在稀释孔附近的区域,积液冷却孔的模式不同,包括:无积液孔;渗出孔从稀释孔向外呈放射状;渗出孔呈放射状向内指向稀释孔。采用粒子图像测速(PIV)技术捕获了自由流湍流强度分别为0.5%和13%时的时间平均流场。结果表明,三种渗液孔型的稀释孔前缘均有向下运动。对比三种几何形状,向外的射流孔向稀释射流前缘的速度明显高于其他两种几何形状。虽然稀释射流产生的流场在下游流动中占主导地位,但每个冷却孔型与流场的相互作用是独特的。接近自由流的湍流对流场没有显著影响。
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Effects of Effusion Cooling Pattern Near the Dilution Hole for a Double-Walled Combustor Liner: Part 2 — Flowfield Measurements
The complex flowfield inside a gas turbine combustor creates a difficult challenge in cooling the combustor walls. Many modern combustors are designed with a double-wall that contain both impingement cooling on the backside of the wall and effusion cooling on the external side of the wall. Complicating matters is the fact that these double-walls also contain large dilution holes whereby the cooling film from the effusion holes is interrupted by the high-momentum dilution jets. Given the importance of cooling the entire panel, including the metal surrounding the dilution holes, the focus of this paper is understanding the flow in the region near the dilution holes. Near-wall flowfield measurements are presented for three different effusion cooling hole patterns near the dilution hole. The effusion cooling hole patterns were varied in the region near the dilution hole and include: no effusion holes; effusion holes pointed radially outward from the dilution hole; and effusion holes pointed radially inward toward the dilution hole. Particle image velocimetry (PIV) was used to capture the time-averaged flowfield at approaching freestream turbulence intensities of 0.5% and 13%. Results showed evidence of downward motion at the leading edge of the dilution hole for all three effusion hole patterns. In comparing the three geometries, the outward effusion holes showed significantly higher velocities toward the leading edge of the dilution jet relative to the other two geometries. Although the flowfield generated by the dilution jet dominated the flow downstream, each cooling hole pattern interacted with the flowfield uniquely. Approaching freestream turbulence did not have a significant effect on the flowfield.
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