Symmetric Mach reflection configuration with asymmetric unsteady solution

Symmetric Mach reflection in steady supersonic flow has been usually studied by solving a half-plane problem with the symmetric line treated as reflecting surface, thus losing the opportunity to discover antisymmetric flow structures. Here in this paper we treat this problem as an entire-plane problem. Using an unsteady numerical approach, we find that the two sliplines exhibit antisymmetric unsteadiness if the Mach stem height is small while the flow remains symmetric if the Mach stem height is large. The mechanism by which disturbance, generated in the downstream of the flow duct between the two sliplines, propagates upstream is identified and it is also shown that the interaction between the transmitted expansion waves and the sliplines increases the amplitude of the unstable modes. The present study suggests a new type of compressible jet that deserves further studies.     

Hypersonic shock wave and turbulent boundary layer interaction in a sharp cone/flare model

A direct numerical simulation of hypersonic Shock wave and Turbulent Boundary Layer Interaction(STBLI) at Mach 6.0 on a sharp 7° half-angle circular cone/flare configuration at zero angle of attack is performed. The flare angle is 34° and the momentum thickness Reynolds number based on the incoming turbulent boundary layer on the sharp circular cone is Re_θ = 2506. It is found that the mean flow is separated and the separation bubble occurring near the corner exhibits unsteadiness. The Reynolds analogy factor changes dramatically across the interaction, and varies between 1.06 and 1.27 in the downstream region, while the QP85 scaling factor has a nearly constant value of 0.5 across the interaction. The evolution of the reattached boundary layer is characterized in terms of the mean profiles, the Reynolds stress components, the anisotropy tensor and the turbulence kinetic energy. It is argued that the recovery is incomplete and the near-wall asymptotic behavior does not occur for the hypersonic interaction. In addition, mean skin friction decomposition in an axisymmetric turbulent boundary layer is carried out for the first time. Downstream of the interaction, the contributions of transverse curvature and body divergence are negligible, whereas the positive contribution associated with the turbulence kinetic energy production and the negative spatial-growth contribution are dominant. Based on scale decomposition, the positive contribution is further divided into terms with different spanwise length scales. The negative contribution is analyzed by comparing the convective term, the streamwise-heterogeneity term and the pressure gradient term.     

星箭分离减冲击环结构优化设计

针对星箭分离过程，建立了减冲击环结构模型，并分析了该结构的减冲原理。利用冲击响应谱的时域合成算法计算获得符合冲击谱规范的时域载荷，并以此作为结构优化设计中动力学模型的输入载荷工况。以减冲击环的连续层数、单层支撑块数、连续层厚度、支撑块层高度以及环的外半径和内半径6个结构参数为设计变量，以减冲效果和结构强度、刚度为约束，以质量最轻为目标，建立减冲击环的结构优化设计模型，这是一包含离散变量和连续变量的混合优化问题。为了在跨平台下求解该混合优化问题，采用代理模型策略和自适应模拟退火算法求解，并在最优点处开展结构性能对设计变量的敏度计算，对计算结果进行了分析评估。本研究对强冲击动力学环境下的航天器结构分析与设计有一定的指导意义。     

A numerical study of segmented cooling-stream injection in supersonic film cooling

The present study proposes a segmented cooling-stream injection structure based on a certain coolant mass flow rate, and numerically investigates the effect of segmented cooling-stream injection on supersonic film cooling. The results indicate that without shock-wave impingement and with helium as the coolant, segmented cooling-stream injection can reduce the mixing between the mainstream and the cooling stream to produce better cooling performance than single injection, especially at larger coo...     

激光脉冲能量作用下隔离段激波形态及发展控制的数值研究

为了寻求有效的流动控制方法来降低隔离段总压损失，本文基于非定常雷诺平均的Navier-Stokes方程，探究激光脉冲能量沉积对二维及三维隔离段流场马赫反射的控制效果。在来流马赫数分别为1.61和2.51的隔离段流场马赫反射上游，加入脉冲能量沉积，对比激励流场与基础流场，结果表明：能量沉积主要通过高温热核和其诱导的压力波两种方式对马赫反射结构施加作用，显著地影响了马赫反射结构，促使Ma∞ =1.61来流工况下马赫杆的高度减小，马赫反射强度减弱；Ma∞ =2.51来流工况下的马赫反射结构转变为稳定的正规反射，减小了总压损失。控制过程包括：(1)能量沉积产生的局部高温降低当地马赫数，减小马赫反射强度；(2)高温热核诱导的弓形波与马赫反射相互作用，马赫反射结构变形；(3)以反压形式影响马赫反射。     

标定脉宽对冲击传感器标定结果的影响

不同冲击脉宽在标定压电式冲击传感器过程产生不同的结果，主要原因是脉宽冲击频率处于传感器安 装频响的放大区，不同的脉宽作用于传感器后放大效应不同，导致标定结果差异。冲击传感器使用空气炮和霍普金 生杆进行单独标定，对标定结果进行了差异分析。对传感器安装频响曲线进行了定性分析，符合冲击脉宽差导致不 同标定结果的事实。对标定过程中标定脉宽控制提出了具体的措施，对于正确标定冲击传感器具有指导意义。     

Oblique detonation wave triggered by a double wedge in hypersonic flow

Pressure-gain combustion has gained attention for airbreathing ramjet engine applications owing to its better thermodynamic efficiency and fuel consumption rate. In contrast with traditional detonation induced by a single wedge, the present study considers oblique shock interactions attached to double wedges in a hypersonic combustible flow. The temperature/pressure increases sharply across the interaction zone that initiates an exothermic reaction, finally resulting in an Oblique Detonation Wav...     

高马赫数V字形钝化前缘平板表面压力特性

针对三维内转式进气道V字形唇口下游面临的严酷压力载荷问题，将唇口简化为V字形钝化前缘平板，在来流马赫数为6的条件下，采用数值模拟结合激波风洞压敏涂料测量方法，研究了半径比R/r = 0 ~ 20（V字形根部倒圆半径R与前缘钝化半径r之比）的平板表面压力演化特性。结果表明，随着R/r增大，V字形钝化前缘产生的三维波系结构发生变化，引起下游平板表面压力演变出4种类型。R/r较小时，V字形钝化前缘激波干扰产生的大范围流动分离，诱导形成了偏离中心线较远的分叉状高压区（Type Ⅰ，分叉型）；随着R/r增大，流动分离减弱，分叉状高压区逐渐消失，由透射激波扫掠壁面所形成的条带状高压和超声速射流对撞所形成的中心线高压区逐渐显露，依次出现过渡型（Type Ⅱ）、严酷型（Type Ⅲ）和渐匀型（Type Ⅳ）压力分布。平板上分叉型和过渡型的压力最大值仅为4.3 ~ 7.2p∞（p∞为来流静压），但V字形钝化前缘处的流场品质恶劣；严酷型的压力最大值，随着射流对撞强度的增强而增大，最高可达19p∞；渐匀型的压力最大值，随着射流对撞强度的减弱，逐渐趋近于二维钝前缘平板产生的压力最大值4p∞。