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Boundary Layer Transition and Trip Effectiveness on an Apollo Capsule in the JAXA High Enthalpy Shock Tunnel (HIEST) Facility

机译:JAXA高焓冲击隧道(HIEST)设施中阿波罗胶囊的边界层过渡和跳闸有效性

摘要

Computational assessments were performed to size boundary layer trips for a scaled Apollo capsule model in the High Enthalpy Shock Tunnel (HIEST) facility at the JAXA Kakuda Space Center in Japan. For stagnation conditions between 2 MJ/kg and 20 MJ/kg and between 10 MPa and 60 MPa, the appropriate trips were determined to be between 0.2 mm and 1.3 mm high, which provided kappa/delta values on the heatshield from 0.15 to 2.25. The tripped configuration consisted of an insert with a series of diamond shaped trips along the heatshield downstream of the stagnation point. Surface heat flux measurements were obtained on a capsule with a 250 mm diameter, 6.4% scale model, and pressure measurements were taken at axial stations along the nozzle walls. At low enthalpy conditions, the computational predictions agree favorably to the test data along the heatshield centerline. However, agreement becomes less favorable as the enthalpy increases conditions. The measured surface heat flux on the heatshield from the HIEST facility was under-predicted by the computations in these cases. Both smooth and tripped configurations were tested for comparison, and a post-test computational analysis showed that kappa/delta values based on the as-measured stagnation conditions ranged between 0.5 and 1.2. Tripped configurations for both 0.6 mm and 0.8 mm trip heights were able to effectively trip the flow to fully turbulent for a range of freestream conditions.
机译:在日本JAXA角田航天中心的高焓冲击隧道(HIEST)设施中,对比例化的阿波罗胶囊模型的边界层行程大小进行了计算评估。对于介于2 MJ / kg和20 MJ / kg之间以及介于10 MPa和60 MPa之间的停滞条件,确定的合适行程为0.2 mm至1.3 mm高,这在隔热板上提供的Kappa /δ值为0.15至2.25。脱扣结构由一个刀片组成,该刀片沿停滞点下游的隔热屏具有一系列菱形的脱扣。在直径为250 mm,比例为6.4%的胶囊上获得表面热通量,并在沿喷嘴壁的轴向位置进行压力测量。在低焓条件下,计算预测与沿隔热板中心线的测试数据吻合良好。但是,随着焓的增加,协议变得不太有利。在这些情况下,通过HIEST设施测得的隔热板上的表面热通量被计算不足。测试了平滑配置和脱扣配置以进行比较,测试后的计算分析表明,基于所测得的停滞条件,κ/δ值介于0.5和1.2之间。对于0.6 mm和0.8 mm跳闸高度的跳闸配置,能够在一定范围的自由流条件下有效地将流量跳闸至完全湍流。

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