首页> 外文会议>ASME Turbo Expo >FULL-COVERAGE FILM COOLING: FILM EFFECTIVENESS AND HEAT TRANSFER COEFFICIENTS FOR DENSE HOLE ARRAYS AT DIFFERENT HOLE ANGLES, CONTRACTION RATIOS, AND BLOWING RATIOS
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FULL-COVERAGE FILM COOLING: FILM EFFECTIVENESS AND HEAT TRANSFER COEFFICIENTS FOR DENSE HOLE ARRAYS AT DIFFERENT HOLE ANGLES, CONTRACTION RATIOS, AND BLOWING RATIOS

机译:全覆盖薄膜冷却:不同孔角,收缩比和吹幂的密集孔阵列的膜效果和传热系数

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Experimental results are presented for a full coverage film cooling arrangement which simulates a portion of a gas turbine engine, with appropriate streamwise static pressure gradient. The test surface utilizes varying blowing ratio along the length of the contraction passage which contains the cooling hole arrangement. For the different experimental conditions examined, film cooling holes are sharp-edged and streamwise inclined either at 20° or 30° with respect to the liner surface. The film cooling holes in adjacent streamwise rows are staggered with respect to each other. Data are provided for turbulent film cooling, contraction ratios of 1, 3, 4, and 5, blowing ratios (at the test section entrance) of 2.0, 5.0, and 10.0, coolant Reynolds numbers Re_(fc) of 10,000 to 12,000, freestream temperatures from 75°C to 115°C, a film hole diameter of 7 mm, and density ratios from 1.15 to 1.25. Non-dimensional streamwise and spanwise film cooling hole spacings, X/D and Y/D, are 6, and 5, respectively. When the streamwise hole inclination angle is 20°, spatially-averaged and line-averaged adiabatic effectiveness values at each x/D location are about the same as the contraction ratio varies between 1, 3, and 4, with slightly higher values at each x/D location when the contraction ratio Cr is 5. For each contraction ratio, there is a slight increase in effectiveness when the blowing ratio is increased from 2.0 to 5.0 but there is no further substantial improvement when the blowing ratio is increased to 10.0. Overall, line-averaged and spatially-averaged adiabatic film effectiveness data, and spatially-averaged heat transfer coefficient data are described as they are affected by contraction ratio, blowing ratio, hole angle a, and streamwise location x/D. For example, when α=20°, the detrimental effects of mainstream acceleration are apparent since heat transfer coefficients for contraction ratios Cr of 3 and 5 are often higher than values for Cr=1, especially for x/D >100.
机译:实验结果以适当的流动静态压力梯度模拟燃气涡轮发动机的一部分的全覆盖膜冷却装置。测试表面利用沿着包含冷却孔装置的收缩通道的长度的变化吹延比。对于检查的不同实验条件,薄膜冷却孔相对于衬垫表面在20°或30°处倾斜并流倾斜。相邻流动行中的膜冷却孔相对于彼此交错。提供数据,用于湍流膜冷却,1,3,4和5的收缩比,吹气比(在试验部分入口处)为2.0,5.0和10.0,冷却剂雷诺数Re_(FC)为10,000至12,000,FreeStream温度从75°C至115°C,薄膜孔直径为7mm,密度比为1.15至1.25。非尺寸流动和翼展膜冷却孔间距,X / D和Y / D分别为6和5。当流动孔倾斜角度为20°时,每个X / D位置处的空间平均和线平均绝热效能值大致与收缩率变化在1,3和4之间,每个x处有略微较高的值/ D当收缩比Cr为5时的位置。对于每个收缩率,当吹出比率从2.0增加到5.0时,有效的有效性略有增加,但当吹出比率增加到10.0时,没有进一步的大量改进。总体而言,线平均和空间平均的绝热膜效果数据和空间平均传热系数数据被描述为受收缩率,吹出比,孔角A和流动位置X / D的影响。例如,当α= 20°时,主流加速的不利影响是显而易见的,因为用于收缩率Cr的传热系数3和5的传热系数通常高于Cr = 1的值,特别是对于X / D> 100。

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