某型飞机导航误差对CCD稳瞄系统目标搜索域的影响

分析了DG-1型多普勒／GPS组合导航系统，在不同工作方式下导航误差所引起的搜索方位角的误差；讨论了由于搜索方位角的变化引起的搜索域的变化。通过对机理的研究提出了解决办法。     

5A90铝锂合金型材折斜角成形性能的试验研究

型材一次折斜角成形是航空零件制造工艺的重要方法之一。本文通过新研制的5A90铝锂合金型材折斜角成形试验的研究，得到了极限开斜角和闭斜角值，为新机的设计及生产工艺提供了重要的指导依据。     

"直接升力控制"空中加油控制系统模拟

研究采用“直接升力控制系统”，在俯仰角保持不变（θ=const)的情况下，空中加油时飞机的飞行动力学和飞行控制问题。采用F-15飞机（静不安定飞机）参数，完成了飞机空中加油过程线代模型的建立和运动关系的推导；进行了空中加油闭环过程的计算机模拟；结果证明这种方法是有效的。     

双翼金属圆柱体散射场的整体计算

本文利用keller的几何绕射理论（GTD）推求出双翼金属圆柱体散射场高频快收敛整体解，弥补了传统分离解（把系统分解为一个金属圆柱和两个金属半平面，分别求解再简单迭加）的不足之处，最后，给出了整体解和分离解的散射电场的模值数值计算结果。     

角速度波动检测技术研究

标准转台等旋转体在转动时产生的角速度波动对被标定设备的数据可信度有很大影响。本文主要论述了角速度波动检测的重要性和可能性，并对检测的方法进行了介绍，用时域等信号处理方法对角速度波动数据进行了分析。     

民用客机后机身外形设计研究

CC-200是一款单通道、中程大型民用客机。CC-200民用客机具有大展弦比、小后掠角、相对较低的巡航速度等技术特点。CC-200的后机身的外形长度为6.458 m,上掠角为12°,与地面水平线的最小间隙值为0.15 m。后机身外形及其它部段的外形采用CATIA V5软件建立了三维数模,后机身采用ESDU 80006和ESDU7011中的方法进行阻力增量的计算、评估。计算表明,在机身迎角一定的情况下,后机身阻力增量随着上掠角的增大而增大。     

非圆实信号MIMO雷达中基于实值ESPRIT的角度估计

研究单基地多输入多输出(MIMO)雷达中的波达角(DOA)估计问题,提出了一种基于非圆(NC)实信号的实值旋转不变性信号参数估计(ESPRIT)算法.首先对接收信号进行降维变换,降低运算复杂度;之后根据非圆实信号特性构造中心Hermitian对称矩阵,通过酉(Unitary)变换将复数运算转为实数,进一步降低复杂度;最后根据ESPRIT得到角度估计.该算法无需谱峰搜索,运算复杂度较NC ESPRIT和Unitary ESPRIT大大降低,且该算法的角度估计性能优于后两种算法.论文分析了所提算法的复杂度,并推导了克拉美-罗界(CRB).仿真结果验证了该算法的有效性.     

Numerical study of unsteady starting characteristics of a hypersonic inlet

The impulse and self starting characteristics of a mixed-compression hypersonic inlet designed at Mach number of 6.5 are studied by applying the unsteady computational fluid dynamics (CFD) method. The full Navier-Stokes equations are solved with the assumption of viscous perfect gas model, and the shear-stress transport (SST) k-x two-equation Reynolds averaged Navier- Stokes (RANS) model is used for turbulence modeling. Results indicate that during impulse starting, the flow field is divided into three zones with different aerodynamic parameters by primary shock and upstream-facing shock. The separation bubble on the shoulder of ramp undergoes a generating, growing, swallowing and disappearing process in sequence. But a separation bubble at the entrance of inlet exists until the freestream velocity is accelerated to the starting Mach number during self starting. The mass flux distribution of flow field is non-uniform because of the interaction between shock and boundary layer, so that the mass flow rate at throat is unsteady during impulse starting. The duration of impulse starting process increases almost linearly with the decrease of freestream Mach number but rises abruptly when the freestream Mach number approaches the starting Mach number. The accelerating performance of booster almost has no influence on the self starting ability of hypersonic inlet.     

跨声速风扇叶片反扭影响因素研究

基于结构几何非线性大变形的静态分析和流场分析,使用叶片反扭设计的流固双向耦合的数值模拟方法,得到NASA Rotor67跨声速风扇叶片的冷态加工叶型。研究了材料、气动工况、转速对叶片静态变形和反扭设计参数的影响。结果表明:转速对叶片反扭的影响最显著,气动工况次之,材料的影响最弱;另外,这三种因素和叶片反扭的关系,与其和叶片静变形量的关系有较大相关性。     

Subsonic impulsively starting flow at a high angle of attack with shock wave and vortex interaction

Impulsively starting flow, by a sudden attainment of a large angle of attack, has been well studied for incompressible and supersonic flows, but less studied for subsonic flow. Recently, a preliminary numerical study for subsonic starting flow at a high angle of attack displays an advance of stall around a Mach number of 0.5, when compared to other Mach numbers. To see what happens in this special case, we conduct here in this paper a further study for this case, to display and analyze the full flow structures. We find that for a Mach number around 0.5, a local supersonic flow region repeatedly splits and merges, and a pair of left-going and right-going unsteady shock waves are embedded inside the leading edge vortex once it is sufficiently grown up and detached from the leading edge. The flow evolution during the formation of shock waves is displayed in detail. The reason for the formation of these shock waves is explained here using the Laval nozzle flow theory. The existence of this shock pair inside the vortex, for a Mach number only close to 0.5, may help the growing of the trailing edge vortex responsible for the advance of stall observed previously.