具有上游喷射流的跨声速涡轮叶片端壁传热与冷却性能

Zhigang Li, B. Bai, Jun Li, Shuo Mao, W. Ng, Hongzhou Xu, M. Fox
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引用次数: 1

摘要

由于高度三维通道涡和端壁二次流的存在,涡轮叶片端壁附近的流场非常复杂。这使得采用传统的端壁冷却方法(如冲击冷却与叶片通道内局部膜冷却相结合)有效冷却端壁变得具有挑战性。一种有效的端壁冷却方案是:冷却剂通过端壁叶片前缘上游的离散孔喷射,这已经被许多燃气轮机公司考虑过。本文主要研究了通过离散孔上游注入冷却剂的端壁膜冷却效果评价。本文对上游离散孔注入冷却剂的端壁传热和冷却性能进行了详细的实验和数值研究。采用瞬态红外热成像技术对轴对称异形端壁进行了高分辨率传热系数(HTC)和绝热膜冷却效能值的测量。测试端壁为工业跨声速涡轮叶片的放大内端壁,双排离散圆柱膜冷却孔位于叶片前缘上游0.39Cx处。试验在跨声速线性叶栅吹落风洞设施中进行。以陆基发电涡轮为代表,根据出口条件和轴向弦长,出口马赫数为0.85,出口雷诺数为1.5 × 106。利用进气道湍流网格模拟了真实涡轮的典型湍流条件,产生了16%的高湍流水平,积分长度尺度为3.6%P。低温空气通过控制上游冷却剂喷射流量的两个参数:质量流量决定冷却剂与主流的吹气比(BR = 2.5, 3.5),气体温度决定密度比(DR = 1.2),模拟典型的冷却剂与主流的状态。为了突出上游冷却剂流动和通道二次流之间的相互作用以及对端壁传热和冷却性能的影响,使用商用CFD求解器ANSYS Fluent v.15求解稳态雷诺平均纳维-斯托克斯(RANS),将CFD预测结果与实验结果进行比较。对四种不同的雷诺数平均湍流模型进行了详细的数值方法验证。验证了Realizable κ- λ模型适用于获得可靠的数值解。数值研究了大范围冷却液-主流吹气比(BR = 1.0、1.5、1.9、2.5、3.0、3.5)的影响。提出并讨论了冷却剂注入与叶片通道内二次流之间复杂的相互作用。结果表明,当BR值较低时,上游双排离散孔的端壁冷却剂覆盖受到通道二次流的强烈控制,冷却效果很差。随着BR的增大,注入冷却剂可以抑制叶片通道内的强二次流,当BR增大到临界值(BR = 2.5 ~ 3.0)时,叶片通道内的强二次流开始基本消除。超过临界BR后,大部分注入的冷却剂开始从端壁上升,并明显渗透到主流流中,导致端壁冷却效果不佳。
本文章由计算机程序翻译,如有差异,请以英文原文为准。
Endwall Heat Transfer and Cooling Performance of a Transonic Turbine Vane With Upstream Injection Flow
Flow fields near the turbine vane endwall region are very complicated due to the presence of highly three-dimensional passage vortices and endwall secondary flows. This makes it challenging for the endwall to be effectively cooled by employing traditional endwall cooling methods, such as impingement cooling combined with local film cooling inside the vane passage. One effective endwall cooling scheme: coolant injection flow through discrete holes upstream of the vane leading edge on the endwall, has been considered by many gas turbine companies. The present paper focuses on endwall film cooling effectiveness evaluation with upstream coolant injection through discrete holes. Detailed experimental and numerical studies on endwall heat transfer and cooling performance with coolant injection flow through upstream discrete holes is presented in this paper. High resolution heat transfer coefficient (HTC) and adiabatic film cooling effectiveness values were measured using a transient infrared thermography technique on an axisymmetric contoured endwall. The endwall tested was a scaled up inner endwall of an industrial transonic turbine vane with double-row discrete cylindrical film cooling holes located 0.39Cx upstream of the vane leading edge. The tests were performed in a transonic linear cascade blow-down wind tunnel facility. Conditions were representative of a land-based power generation turbine with exit Mach number of 0.85 corresponding to exit Reynolds number of 1.5 × 106, based on exit condition and axial chord length. A high turbulence level of 16% with an integral length scale of 3.6%P was generated using inlet turbulence grid to reproduce the typical turbulence conditions in real turbine. Low temperature air was used to simulate the typical coolant-to-mainstream condition by controlling two parameters of the upstream coolant injection flow: mass flow rate to determine the coolant-to-mainstream blowing ratio (BR = 2.5, 3.5), and gas temperature to determine the density ratio (DR = 1.2). To highlight the interactions between the upstream coolant flow and the passage secondary flow combined with the influence on the endwall heat transfer and cooling performance, a comparison of CFD predictions to experimental results was performed by solving steady-state Reynolds-Averaged Navier-Stokes (RANS) using the commercial CFD solver ANSYS Fluent v.15. A detailed numerical method validation was performed for four different Reynolds-averaged turbulence models. The Realizable κ-ϵ model was validated to be suitable to obtain reliable numerical solution. The influences of a wide range of coolant-to-mainstream blowing ratios (BR = 1.0, 1.5, 1.9, 2.5, 3.0, 3.5) were numerically studied. Complex interactions between coolant injections and secondary flows in vane passage were presented and discussed. Results indicate that for lower values of BR, the endwall coolant coverage from the upstream double-row discrete holes is strongly controlled by the passage secondary flow, thus the cooling effectiveness is very poor. As the BR increases, the strong secondary flow in vane passage can be suppressed by the coolant injections and begin to be almost eliminated when BR increases to a critical value (BR = 2.5 – 3.0). Beyond the critical BR, most of the injected coolant begins to lift off from the endwall and penetrate significantly into the mainstream flow, yielding inefficient endwall cooling performance.
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