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Full-Coverage Film Cooling: Film Effectiveness and Heat Transfer Coefficients for Dense and Sparse Hole Arrays at Different Blowing Ratios

机译:全覆盖薄膜冷却:在不同的吹塑比下,密集和稀疏孔阵列的薄膜效率和传热系数

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摘要

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 and varying blowing ratio along the length of the contraction passage which contains the cooling hole arrangement. Film cooling holes are sharp-edged, streamwise inclined at 20 deg with respect to the liner surface, and are arranged with a length to diameter ratio of 8.35. 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 and 4, blowing ratios (at the test section entrance) of 2.0,5.0, and 10.0, coolant Reynolds numbers Re_(fc)from 10,000 to 12,000 (for a blowing ratio of 5.0),freestream temperatures from 75 ℃ to 115℃, a film hole diameter of 7 mm, and density ratios from 1.15 to 1.25. Changes to X/D and YID, nondimensional streamwise and spanwise film cooling hole spacings, with YID of 3,5, and 7, and with X/D of 6 and 18, are considered. For all X/D=6 hole spacings, only a slight increase in effectiveness (local, line-averaged, and spatially-averaged) values are present as the blowing ratio increases from 2.0 to 5.0, with no significant differences when the blowing ratio increases from 5.0 to 10.0. This lack of dependence on blowing ratio indicates a condition where excess coolant is injected into the mainstream flow, a situation not evidenced by data obtained with the X/D=18 hole spacing arrangement. With this sparse array configuration, local and spatially-averaged effectiveness generally increase continually as the blowing ratio becomes larger. Line-averaged and spatially-averaged heat transfer coefficients are generally higher at each streamwise location, also with larger variations with streamwise development, with the X/D=6 hole array, compared to the X/D= 18 array.
机译:给出了全覆盖膜冷却装置的实验结果,该装置模拟了燃气涡轮发动机的一部分,具有适当的沿流方向的静压力梯度,并且沿着包含冷却孔装置的收缩通道的长度方向具有不同的鼓风比。薄膜冷却孔是锋利的,相对于内衬表面沿流向倾斜20度,并且其长径比为8.35。相邻的流向行中的膜冷却孔彼此交错。提供了湍流薄膜冷却,收缩比为1和4,吹塑比(在测试段入口处)为2.0、5.0和10.0,冷却剂雷诺数Re_(fc)从10,000到12,000(吹塑比为5.0)的数据),自由流温度为75℃至115℃,膜孔直径为7 mm,密度比为1.15至1.25。考虑了X / D和YID的变化,YID为3,5和7以及X / D为6和18的无尺寸流向和跨膜冷却孔间距。对于所有X / D = 6的孔间距,当吹塑比从2.0增加到5.0时,有效性值(局部,行平均和空间平均)仅略有增加,当吹塑比增加时,效率没有显着差异从5.0到10.0。这种对吹气比的依赖性不足表明,有多余的冷却剂注入主流的情况,这种情况没有通过X / D = 18孔距布置获得的数据证明。使用这种稀疏阵列配置,随着吹风比变大,局部和空间平均效率通常会不断提高。与X / D = 18阵列相比,在X / D = 6孔阵列中,线平均和空间平均的传热系数通常在每个沿河方向的位置都较高,并且随着沿河方向的发展也有较大的变化。

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  • 来源
    《Journal of turbomachinery》 |2012年第6期|p.061039.1-061039.13|共13页
  • 作者单位

    Department of Engineering Science University of Oxford, Oxford, OX1 3PJ UK;

    Department of Engineering Science University of Oxford, Oxford, OX1 3PJ UK;

    Solar Turbines, Inc., San Diego, 92101 CA;

    Solar Turbines, Inc., San Diego, 92101 CA;

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