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LEADING-EDGE FILM-COOLING PHYSICS: PART Ⅱ- HEAT TRANSFER COEFFICIENT

机译:领先的薄膜冷却物理:第二部分-传热系数

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A comprehensive study of film cooling on a turbine airfoil leading edge was performed with a documented, well-tested computational methodology. In this paper, numerically predicted heat transfer coefficients on the film-cooled leading edge are compared with experimental data from the open literature. The results are presented as the ratio of heat transfer coefficient with film cooling to that without film cooling, and the physics behind the surface results are discussed. The leading edge model was a half-cylinder in shape with a bluff afterbody to match the validation experiment, and other geometric parameters matched those of Part I of this study. Coolant at a density equal to that of the mainstream flow was injected through three rows of cylindrical film-cooling holes. One row of holes was centered on the stagnation line of the cylinder, and the other two rows were located + -3.5 hole diameters off stagnation. The downstream rows were staggered such that they were centered laterally between holes in the stagnation row. The holes were inclined at 20° with the surface, and made a 90° angle with the streamwise direction (radial injection). Four average blowing ratios were simulated in the range of 0.75 to 1.9, corresponding to the same momentum flux ratios as in Part I of this work. The multi-block, unstructured numerical grid was characterized by high quality and density, especially in the near wall region, in order to minimize error in predictions of the heat transfer. A fully-implicit scheme was used to solve the steady Reynolds-averaged Navier-Stokes equations, and a realizable k-ε model provided turbulence closure. A two-layer near-wall treatment allowed the resolution of the viscous sublayer for maximum accuracy in the prediction of the wall heat transfer coefficient. The numerical predictions exhibited generally good agreement with experimental data. The heat transfer coefficient was observed to increase sharply aft of the holes in the downstream rows. When coupled with the adiabatic effectiveness results of the first paper in this series, it is evident that a systematic computational methodology may be effectively applied to investigate and understand the complicated leading edge film-cooling problem.
机译:涡轮机翼前缘上的薄膜冷却的综合研究是通过有证的,经过良好测试的计算方法来进行的。在本文中,将薄膜冷却前缘上的数值预测传热系数与来自公开文献的实验数据进行了比较。结果以薄膜冷却时的传热系数与未薄膜冷却时的传热系数之比表示,并对表面结果背后的物理性质进行了讨论。前缘模型是半圆柱体形状,后部虚张声势以匹配验证实验,其他几何参数与本研究的第一部分相匹配。通过三排圆柱形薄膜冷却孔注入密度等于主流流量的冷却剂。一行孔位于圆柱体的停滞线上,而其他两行位于停滞处+ -3.5孔直径。下游排交错排列,以使它们在停滞排中的孔之间横向居中。孔与表面成20°倾斜,与流向成90°角(径向注入)。在0.75至1.9范围内模拟了四个平均鼓风比,与本工作第一部分中相同的动量通量比相对应。多块非结构化数值网格的特点是高质量和高密度,尤其是在近壁区域,以最大程度地减少热传递预测中的误差。使用完全隐式方案来求解稳定的雷诺平均Navier-Stokes方程,并且可实现的k-ε模型提供了湍流闭合。通过两层近壁处理,可以解析粘性子层,从而在预测壁传热系数时获得最大的准确性。数值预测显示出与实验数据总体上良好的一致性。观察到传热系数在下游排中的孔的后部急剧增加。当结合本系列第一篇论文的绝热效果结果时,很明显,一种系统的计算方法可以有效地应用于研究和理解复杂的前缘薄膜冷却问题。

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