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LARGE EDDY SIMULATIONS OF A THREE-ROW LEADING EDGE FILM COOLING GEOMETRY

机译:三行前缘膜冷却几何的大涡模拟

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A three-row leading edge film cooling geometry is investigated using Large-Eddy Simulations (LES) at a freestream Reynolds number of 32,000 and blowing ratio of 0.5 with lateral injection of 45° to the surface and 90° compound injection. The stagnation jet interacts with the mainstream through the generation of ring vortices which quickly breakdown and convect along the cylinder surface. The coolant penetrates the mainstream both laterally and normal to the surface resulting in increased mixing and turbulence generation. As the coolant loses transverse and lateral momentum it is pushed back to the surface in the stagnation region after which it convects downstream along the blade surface. Surface coverage is uniform but weak with spanwise-averaged effectiveness ranging from 0.1 to 0.3 in the stagnation region. The primary off-stagnation coolant and mainstream interaction is through the generation of a counter-rotating vortex pair in the immediate wake, but which quickly degenerates to a single vortex which entrains free-stream fluid near the surface at the aft-end of the jet. In contrast to the stagnation row, the coolant stays in close proximity to the surface and does not undergo a large lateral displacement along the spanwise pitch. As a consequence it provides good local coverage along its trajectory but barely covers half the lateral pitch. Hence, spanwise-averaged effectiveness is of the same order as at stagnation starting at 0.3 downstream of injection to 0.1 about 6d downstream.
机译:使用大涡模拟(LES)在自由流雷诺数为32,000且吹塑比为0.5的情况下对三排前缘膜冷却几何形状进行了研究,其中表面横向注入为45°,复合注入为90°。停滞射流通过产生环形涡旋而与主流相互作用,该环形涡旋沿圆柱体表面迅速破裂并对流。冷却剂从侧面和垂直于表面都渗入主流,导致混合和湍流增加。当冷却剂失去横向和横向动量时,它将被推回到停滞区域中的表面,然后沿叶片表面在对流中对流。表面覆盖均匀但较弱,在停滞区域的跨度平均有效范围为0.1到0.3。主要的停滞冷却剂和主流相互作用是通过在立即尾流中产生一个反向旋转的涡流对,但迅速退化为单个涡流,该涡流在喷嘴的尾端带走表面附近的自由流流体。 。与停滞排相反,冷却剂停留在表面附近,并且沿翼展方向的节距不发生较大的侧向位移。结果,它沿其轨迹提供了良好的局部覆盖,但几乎不覆盖横向间距的一半。因此,跨度平均有效性与停滞时的效率相同,停滞时从注入下游的0.3开始到下游注入的0.1d大约6 d。

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