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Slip Effects on the Stability of Supersonic Laminar Flat Plate Boundary Layer

机译:对超声波平板边界层稳定性的滑移效果

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Current worldwide efforts to develop maneuverable vehicles flying in rarefied gas hypersonic environments require quantification of laminar-turbulent transition in the hypersonic boundary layers formed on lifting surfaces and control fins. The present contribution commences efforts to document the effect of wall-slip velocity and temperature distributions on the linear stability of hypersonic laminar boundary layers developing on a semi-infinite flat plate, for Knudsen numbers Kn ~ 0(0.05), corresponding to flight altitudes of 35km ≤ h ≤ 65km and, at first instance, low Reynolds numbers, Re ~ O( 10~3 - 10~4). The steady laminar base flow is obtained using the Direct Simulation Monte Carlo (DSMC) method. Results on the mean-free-path and wall-normal velocity and temperature gradients obtained are used to construct slip-velocity and temperature-jump boundary conditions along the plate surface, following recent updates of the Maxwell / von Smoluchowski theory. Linear stability analysis of the DSMC profiles extracted from the simulation and those obtained by the updated compressible boundary layer theory reveals quantitative but not qualitative differences on the characteristics of the leading flow eigenmodes over the range of parameters examined. Work is underway to characterise whether the observed differences are a result of a residual pressure gradient present in the DSMC simulation, or intrinsic to kinetic fluctuations unaccounted for in the framework of Navier-Stokes/boundary layer theory.
机译:目前在全球范围内开发稀有气体高度环境中的机动车辆的努力需要在升降表面和控制翅片上形成的高超声音边界层中的层压湍流过渡。本贡献开始努力记录墙面滑移速度和温度分布对在半无限平板上显影的高超声伸层边界层的线性稳定性的努力,对于knudsen Number Kn〜0(0.05),对应于飞行高度35km≤h≤65km,并且在第一例,低雷诺数,RE〜O(10〜3-10〜4)。使用直接仿真蒙特卡罗(DSMC)方法获得稳定的层压流。在最近MaxWell / von Smoluchowski理论的最新更新之后,所获得的平均直接路径和壁正常速度和温度梯度用于构造沿着板表面的滑移速度和温度跳边界条件。从模拟中提取的DSMC型材的线性稳定性分析和通过更新的可压缩边界层理论获得的那些揭示了对所检查参数范围内的前导流特征模码的定量但不是定性差异。正在进行工作以表征观察到的差异是DSMC模拟中存在的残余压力梯度的结果,或者在Navier-Stokes /边界层理论的框架中未负责的动力学波动。

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