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Particle-Image Velocimetry Measurements of Film Cooling in an Adverse Pressure Gradient Flow

机译:逆梯度流中薄膜冷却的粒子图像测速技术

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The turbulent flow field of a film cooling flow is investigated using the particle-image velocimetry technique. Cooling jets are injected from a multirow hole configuration into a turbulent boundary layer flow of a flat plate in the presence of a zero and an adverse pressure gradient. I he investigations focus on full-coverage film cooling. Therefore, the film cooling configuration consists of three staggered rows of holes with a lateral spacing of p/D =3 and a streamwise row distance of I/D =6. 'The inclined cooling holes feature a fan-shaped exit geometry with lateral and streamwise expansions. Jets of air and CO_2 are injected separately at different blowing ratios into a boundary layer to examine the effects of the density ratio between coolant and mainstream on the mixing behavior and consequently, the cooling efficiency. For the zero pressure gradient case, the measurement results indicate the different nature oj the mixing process between the jets and the crossfiow after the first, second, and third row. The mainstream velocity distributions evidence the growth of the boundary layer thickness at increasing row number. The interaction between the undisturbed boundary layer and first two rows leads to maximum values of turbulent kinetic energy. The presence of an adverse pressure gradient in the mainstream clearly intensifies the growth of the boundary layer thickness and increases the velocity fluctuations in the upper mixing zone. The measurements considering an increased density ratio show higher turbulence intensities in the shear zone between the jets and the main flow, leading to a more pronounced mixing in this area. The results of the experimental measurements are used to validate numerical findings from a large-eddy .simulation. This comparison shows a very good agreement for mean velocity distributions and velocity fluctuations.
机译:使用粒子图像测速技术研究了薄膜冷却流的湍流场。在零压力和不利压力梯度的存在下,冷却喷嘴从多排孔结构注入到平板的湍流边界层流中。他的研究重点是全覆盖薄膜冷却。因此,薄膜冷却配置由三排交错的孔组成,孔的横向间距为p / D = 3,流向行距离为I / D = 6。倾斜的冷却孔具有扇形出口几何形状,具有横向和沿流方向的膨胀。空气和CO_2的射流分别以不同的吹入比注入边界层,以检查冷却剂和主流之间的密度比对混合行为的影响,并因此影响冷却效率。对于零压力梯度的情况,测量结果表明第一排,第二排和第三排之后的射流与横流之间的混合过程具有不同的性质。主流速度分布证明边界层厚度随着行数的增加而增加。未受干扰的边界层与前两行之间的相互作用导致了湍动能的最大值。主流中存在不利的压力梯度,显然会加剧边界层厚度的增长,并增加上部混合区的速度波动。考虑到密度比增加的测量结果表明,在射流和主流之间的剪切区内湍流强度更高,导致该区域的混合更加明显。实验测量的结果用于验证大涡模拟的数值结果。这种比较显示出平均速度分布和速度波动非常一致。

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