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Effects of Wall Cooling on Hypersonic Boundary Layer Receptivity Over a Cone

机译:壁冷却对锥体上高超音速边界层接受度的影响

摘要

Effects of wall cooling on the receptivity process induced by the interaction of slow acoustic disturbances in the free-stream are numerically investigated for a boundary layer flow over a 5-degrees straight cone. The free-stream Mach number is 6.0 and the Reynolds number is 7.8x10(exp 6)/ft. Both the steady and unsteady solutions are obtained by solving the full Navier-Stokes equations using 5th-order accurate weighted essentially non-oscillatory (WENO) scheme for space discretization and using 3rd-order total variation diminishing (T VD) Runge-K utta scheme for time integration. Computations are performed for a cone with nose radius of 0.001 inch for adiabatic wall temperature (T(sub aw)), 0.75*T(sub aw), 0.5*T(sub aw), 0.40*T(sub aw), 0.30*T(sub aw), and 0.20*T(sub aw). Once the mean flow field is computed, disturbances are introduced at the upstream end of the computational domain. Generation of instability waves from leading edge region and receptivity of boundary layer to slow acoustic waves are investigated. Computations showed that wall cooling has strong stabilization effect on the first mode disturbances as was observed in the experiments. T ransition location moved to upstream when wall cooling was applied It is also found that the boundary layer is much more receptive to fast acoustic wave (by almost a factor of 50). When simulations performed using the same forcing frequency growth of the second mode disturbances are delayed with wall cooling and they attained values two times higher than that of adiabatic case. In 0.20*T(sub aw) case the transition Reynolds number is doubled compared to adiabatic conditions. The receptivity coefficient for adiabatic wall case (804 R) is 1.5225 and for highly cooled cones (241, and 161 R); they are in the order of 10(exp -3).
机译:对于在5度直圆锥上的边界层流,数值研究了壁冷却对自由流中慢声干扰的相互作用引起的接收过程的影响。自由流马赫数为6.0,雷诺数为7.8x10(exp 6)/ ft。通过使用用于空间离散化的5阶精确加权基本非振荡(WENO)方案和使用3阶总变差减小(T VD)的Runge-K utta方案求解完整的Navier-Stokes方程,可以获得稳态和非稳态解用于时间整合。对于绝热壁温(T(sub aw)),0.75 * T(sub aw),0.5 * T(sub aw),0.40 * T(sub aw),0.30 *的鼻半径为0.001英寸的圆锥体进行计算T(sub aw)和0.20 * T(sub aw)。一旦计算出平均流场,就会在计算域的上游端引入干扰。研究了从前缘区域产生不稳定性波以及边界层对慢速声波的接受度。计算表明,如在实验中观察到的,壁冷却对第一模式扰动具有很强的稳定作用。当应用壁冷时,转变位置移至上游。还发现边界层更容易接受快速声波(几乎是50倍)。当使用相同强迫频率进行的第二模态扰动的模拟随着壁冷却而延迟时,其达到的值是绝热情况的两倍。在0.20 * T(sub aw)的情况下,与绝热条件相比,跃迁雷诺数增加了一倍。绝热壁盒(804 R)的接受系数为1.5225,高度冷却的锥体(241和161 R)的接受系数;它们的顺序为10(exp -3)。

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