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Effects of Angle of Attack and Bluntness on Heating Rate Distribution of Blunt Models at Hypersonic Speeds

机译:攻击角度与钝化对高音速度钝化模型加热速率分布的影响

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摘要

The effects of nose radius on stagnation and surface heat transfer rate along the surface are addressed in this research paper. Experiments are carried out in hypersonic shock tunnel, at hypersonic Mach number of 6.56 for 11.38 degrees apex angle blunt cone with nose radius of 0.2R, base radius of R. Similarly, experiments are carried out at Mach 7.32 for 13.87 degrees apex angle blunt cone models with nose radius of 0.18R ', base radius of R '. Test is performed at stagnation enthalpy of 1.4 and 2 MJ/kg with effective test time of 3.5 ms. Convective heat transfer measurements have been carried out on the test model at two different angles of attack, namely 0 degrees and 5 degrees with angle of rotation of 0 degrees, 90 degrees,180 degrees with platinum thin film sensors. ANSYS-Fluent used to simulate the flow over the blunt models at different Mach numbers. The measured shock standoff distance from Schlieren visualization images compared with theory and computational fluid dynamic study for both configurations. The measured stagnation heating value is compared with theoretical value estimated using Fay-Riddell expression and numerical simulation. The measured heat transfer rate is higher for configuration 1 than configuration 2. The increases in heat transfer rate is due higher density ratio across the shock wave and the reduced shock layer thickness. The measured shock layer thickness is 2.06 mm for Mach 6.56 and 3.45 mm for Mach 7.32. The heat transfer rate is higher for Mach 6.56 as compared to Mach 7.32.
机译:在本研究论文中解决了鼻径半径对表面停滞和表面传热率的影响。实验在超音声冲击隧道中进行,在高度高的马赫数为6.56的11.38度顶角钝锥,鼻径为0.2r,基部半径R.类似地,在Mach 7.32中进行实验13.87度顶角钝锥鼻径半径为0.18r',r'的基础半径。测试在1.4和2 MJ / kg的停滞焓下进行,具有3.5ms的有效测试时间。在测试模型上以两种不同的攻击角进行对流传热测量,即0度和5度,旋转角度为0度,90度,180度,具有铂薄膜传感器。 ANSYS-FLUENT用于以不同的MACH数字模拟钝模型上的流量。与Schlieren可视化图像相比,测量的冲击静止距离与两种配置的理论和计算流体动力学研究相比。将测量的停滞加热值与使用Fay-Riddell表达和数值模拟估计的理论值进行比较。对于配置1,测量的传热速率较高。传热速率的增加在冲击波和减小的冲击层厚度上具有更高的密度比。用于Mach 7.32的Mach 6.56和3.45mm的测量的冲击层厚度为2.06 mm。与Mach 7.32相比,Mach 6.56的传热速率较高。

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