反射面的轴向电磁散射及外形优化

本文联合运用几何光学和等效电磁流法,导出了金属反射面轴向散射场和雷达截面(RCS)的简洁表达式,研究了从旋转二次曲面(凹面或凸面)中寻找具有最低RCS值的曲面形状优化方法,给出了一个典型实例的单站RCS立体分布图,以及最低RCS值所对应的波谷曲线和最佳表面参数。     

翼面隐身结构在飞航导弹模型上的数值仿真研究

隐身结构是指由蒙皮和多种内部材料组成的、能满足承载要求、并具有明显降低雷达散射截面的结构。目的是探讨在常规布局飞航导弹上采用隐身结构的效果。以某常规布局飞航导弹模型为背景，设计出两种翼面隐身结构方案，并将这两种翼面隐身结构方案分别应用于飞航导弹模型的弹翼。应用时域有限差分法（FD-TD法）建立了飞航导弹模型电磁散射数值模型。通过数值仿真手段，计算、比较和分析了含有翼面隐身结构的飞航导弹和普通全金属飞航导弹的RCS值。数值仿真结果显示，与普通飞航导弹相比，这两种翼面隐身结构在许多方位上均能有效降低飞航导弹的RCS值。     

天线的散射机理和雷达截面减缩

飞行器头部的天线是鼻锥方向的一个强散射源,它对目标雷达截面的贡献包括了普通的结构散射项和再辐射引起的模式散射项,后者是天线作为一个加载散射体所特有的。本文给出了这两项雷达截面的散射机理和分析计算方法,并提出了减小天线雷达截面的若干技术途径及其实际效果。     

关于双向弯曲变形构件危险截面的讨论

本文通过具体例题，阐述了双向弯曲变形构件中危险截面的判定方法，论证了合成弯矩大的截面不一定是危险截面的结论。     

黄金分割自适应鲁棒控制器设计新方法

本文在全系数自适应控制理论基础上,给出了一种实用的黄金分割自适应鲁棒控制器的设计方法及理论分析。对于参数未知、线性定常或慢变的二阶对象,只要参数估计值在一个范围内,该控制器就能保证闭环系统稳定,且系统输出的动态性能较好。从而解决了二阶系统自适应控制在初始过渡过程阶段的实际应用问题。     

无人机模拟训练系统中的实时飞行仿真

为了降低无人机的试飞成本,提高操纵手的技能,设计了一种模拟训练系统。介绍了该模拟训练系统的特点和构成,着重对系统中实时飞行仿真的各模块设计方法进行了研究。在DOS操作系统中用C语言实现飞行仿真软件,并讨论了软件实现中的模态切换等关键问题。通过飞行剖面仿真实验,证明该仿真系统可靠性高、实时性好。     

反射面天线的双站雷达截面

 本文导出了任意旋转反射器天线在任意双站角的散射场和雷达截面(RCS),其中反射场由几何光学法(GO)求得,绕射场则利用基于物理绕射理论(PTD)与等效线电流辐射积分公式导出的等效电磁流法求得。分别计算了轴向入射和偏轴向入射时在任意散射方向上水平极化与垂直极化两种情况下的双站RCS,并给出了这些结果的立体图形式。方法简化为单站情况时的计算结果与实验值大致相符。     

不同进口截面下液力透平非定常压力脉动计算

为了研究不同进口截面对液力透平内压力脉动的影响,利用CFX软件对一单级液力透平进行非定常数值计算,通过设置监测点,计算各监测点在不同进口截面下的压力脉动,通过快速傅里叶变换将其压力脉动计算结果做相应分析,分析各监测点处压力脉动的时域和频域分布.结果表明:蜗壳内在大蜗壳进口下,随着蜗壳进口直径的增加,每个监测点处的压力逐渐增加,而在小蜗壳进口下,每个监测点处的压力逐渐减小.在距离蜗壳收缩管较远处,大蜗壳进口下的压力脉动较小,而在距离收缩管较近处,小蜗壳进口下的压力脉动较小.在叶轮内不同进口截面压力脉动的差异在同一时刻从进口到出口逐渐减小.尾水管内在小蜗壳进口下尾水管进口处的压力脉动最大.      

Cross-sectional deformation behavior of double-ridged rectangular tube with fillers in different stages of H-typed bending

The bent double-ridged rectangular tube (DRRT) with high forming quality is helpful to improve the microwave transmission accuracy. For reducing the cross-sectional deformation in the H-typed bending process, in addition to using rigid mandrel to support the inside of tube, ridge groove fillers are also added to restrict the deformation of ridge grooves. Because of the change of stress and strain state of bent tube in bending, rigid mandrel retracting and specially twice-springback stages, and the springback of fillers, the cross-sectional deformation of tube in each stage may be different. Therefore, based on the ABAQUS platform, the finite element models (FEM) for H-typed bending, mandrel retracting and twice-springback stages of H96 DRRT with fillers were established and validated. It is found that, for the height and width deformation of tube and spacing deformation of ridge grooves, retraction of mandrel can make the distribution of these deformations more uniform along the bending direction. The first springback can reduce these deformations significantly, which should be emphasized. But the second springback only increases them by less amount, which can be ignored. The smaller height deformation of ridge groove and filler can be neglected.     

Evolution of periodic orbits near the Lagrangian point L2

A study of the evolution of the periodic and the quasi-periodic orbits near the Lagrangian point L₂, which is located to the right of the smaller primary on the line joining the primaries and whose distance from the more massive primary is greater than the distance between the primaries, in the framework of restricted three-body problem for the Sun–Jupiter, Earth–Moon (relatively large mass ratio) and Saturn–Titan (relatively small mass ratio) systems is made. Two families of periodic orbits around the smaller primary are identified using the Poincaré surface of section method – family I (initially elliptical, gradually becomes egg-shaped with the increase in the Jacobi constant C and elongated towards the more massive primary) and family II (initially egg-shaped orbits elongated towards L₂ and gradually becomes elliptical with the increase in C). The family I in the Sun–Jupiter and Saturn–Titan systems contains two separatrix caused by third-order and fourth-order resonances, while the Earth–Moon system has only one separatrix which is caused by third-order resonances. Also in the Sun–Jupiter and the Saturn–Titan systems, family I merge with family II, around Jacobian constant 3.0393 and 3.0163, respectively, while in the Earth–Moon system, family II evolves separately from two different branches. The two branches merge at C = 3.184515. In the Earth–Moon system, the family II contains a separatrix due to third-order resonances which is absent in the other two systems.