为研究变几何进气道在不起动状态下的非定常流动现象,利用二维非定常数值计算方法对唇罩可前移的进气道流场进行模拟,探究唇罩位置变化对高超声速进气道不起动流场非定常特性的影响。对比了唇罩位于高马赫数位置及低马赫数位置时的进气道流动振荡情况,并对其流动振荡特性进行研究。结果表明,在唇罩位于高马赫数位置时,流动振荡幅度随来流马赫数升高明显增大,流量振荡幅值由Ma=4.0工况的0.8 kg/s增大至Ma=4.6工况的2.7 kg/s。而在唇罩位于低马赫数位置时,流动振荡幅度随来流马赫数升高反而逐渐减小。进气道中的小分离区与激波串会导致壁面压力的急剧上升,引发压力的非线性变化。在Ma=4.6工况下,壁面无量纲压强峰值在短时间内从20急剧上升至50以上,而在流场变化较为缓和的Ma=3.3工况,压力峰值仅在12.4~15.74小范围波动。在Ma=4.6工况,进气道流动振荡规律与各壁面监测点基本一致,而Ma=3.3工况下的流动振荡规律则与唇口及喉道处监测点之间出现较大差异。这是因为唇罩前移后进气道内的气流流速增大至声速以上,阻碍了上下壁面间的扰动传播及振荡耦合,因此减弱了进气道内的流动振荡现象。
To study the phenomenon of unsteady flow in unstart variable geometry inlets,a two-dimension-al unsteady numerical study is performed to simulate the internal flow of a hypersonic inlet with a mobile cowl.The effect of this variable geometry on the unsteady flow is investigated.The inlet flow oscillation scenarios with high and low Mach number positions of the cowl are compared and the flow oscillation characteristics are demon-strated.The results show that the amplitude of the flow oscillations increases significantly with the increase of Mach number when the cowl is located at the high Mach number position,and the amplitude of flow oscillations increases from 0.8 kg/s at Ma=4.0 to 2.7 kg/s at Ma=4.6,while the amplitude of flow oscillations decreases with the increase of Mach number when the cowl is located at the low Mach number position.The small separation bub-bles and the shock train in the inlet lead to the pressure surge,which triggers a fractional linear change in the pressure.At Ma=4.6,the peak pressure at the wall rises sharply from 20 to more than 50 in a short time,while the peak pressure only fluctuates in a small range between 12.4 and 15.74 at Ma=3.3,where the change of the flow field is more moderate.At Ma=4.6,the flow oscillation pattern of the inlet is basically consistent with that of the monitoring points on walls,whereas the flow oscillation pattern at Ma=3.3 shows a large discrepancy between that of the monitoring points at the cowl and throat.The flow velocity in the inlet increases above the speed of sound after the cowl is moved forward,and the propagation of disturbance and oscillatory coupling between the upper and lower walls is blocked,which weakens the flow oscillation phenomenon in the inlet.