共面变相位星座多目标交汇序列优化方法

针对空间多目标交汇时空约束繁杂、轨道能量影响变量多的特点,从空间几何解析法入手,提出基于穿越点的共面变相位交汇方法,在Lambert椭圆轨道机动的基础上,给出了机动装置共面变轨相位快速确定方法,总结了变轨速度需求以及运载段分离条件已知情况下相位角和转移时间的包络区,并基于覆盖效能对目标发射序列进行了优化,仿真验证了相关结论,得到的结果符合预期。     

一种低轨双星雷达信号无模糊频差估计算法

针对低轨双星组合接收低脉冲重复频率(LPRF)雷达信号的频差(DFO)估计存在模糊的问题，提出一种基于时差差分的频差无模糊高精度估计算法，该算法通过对高精度的时差测量值进行中心差分获得无模糊的频差估值。仿真结果表明，新算法能对PRF低至300 Hz的雷达信号进行无模糊的频差估计，估计精度在信噪比高于15 dB时逼近克拉美劳下界，可有效扩大低轨双星时/频差定位系统对LPRF信号的适用范围。     

基于产业思维的航天发射服务研究

首先从核心驱动出发提出航天发展三阶段第一推动力,从产业要素出发分析航天产业进阶的市场、技术和产业政策三要素。而后从价值链出发研究航天产业产值分布和产业整合策略。最后分析了新兴航天发射服务公司的模式、产品和技术,为我国航天发射服务提供参考。     

机载移动端场面引导软件设计与仿真研究

为了减轻飞行员在繁忙机场场面运行的工作负荷，提升场面运行安全与效率，设计了一种基于移 动电子设备运行的场面引导软件。其采用可扩展架构和模块化功能设计，通过无线通信网络与综合场面监视系 统交联，实现场面引导功能。仿真测试表明，机载移动端场面引导软件能够为飞机在场面滑行操作提供路径引 导信息和冲突告警提示，可提升运行效率和安全性，具有一定的使用价值。     

多自由度振动环境下惯组非线性传递特性研究

惯组作为飞行器姿控系统的传感器,其局部安装结构的传递特性的测量精度直接关系到导航精度。目前,惯组普遍使用减振器进行隔振,而减振器都呈现出较强的非线性特征。为了考察惯组在不同工况下的传递特性,将惯组简化为六自由度Duffing模型,推导了基础激励下系统的运动微分方程,并用龙格-库塔法对方程进行求解,分析了自由衰减振动和强迫振动下不同工况的系统传递特性。结果表明,多自由度激励比单自由度激励工况得到的系统传递特性的频率和幅值都低。考虑到惯组真实的使用环境,应当在多自由度振动环境下进行传递特性试验。     

先进战斗机过失速机动大气数据融合估计方法

可控的过失速机动是先进战斗机超机动性能的重要标志，飞机飞行包线的扩大已超出传统的大气数据系统测量范围，可靠的迎角、侧滑角、总压、静压等飞行大气数据是制约先进战斗机过失速机动中飞行控制的关键因素。以中国推力矢量验证机为对象，基于过失速机动飞行试验的数据，开展大气参数估计与验证研究。结合过失速机动的时间与空间特性，研究了基于风速、地速、空速矢量和惯性姿态、导航参数的大气参数融合计算方法；针对过失速大迎角状态下飞机周围气流非定常、模型非线性导致的融合大气参数误差的复杂特性，进一步构建深度神经网络，对机动状态融合迎角、侧滑角的强非线性误差进行拟合。仿真和飞行试验表明：该方法可在大迎角飞行状态下实现主要大气参数的融合估计，过失速机动过程中融合迎角误差优于2.3°，融合得到的大气参数可为过失速大迎角机动飞行控制提供可靠的大气参数状态反馈。     

基于单应性矩阵的模型迎角单目视频测量方法

风洞试验中模型迎角的精准测量是降低阻力系数误差的重要途径之一，为此，提出了基于单应性矩阵的模型迎角单目视频测量方法。该方法通过两个单应性矩阵，获取试验过程中相机实时位姿和标记点物方空间位置坐标，应用坐标旋转关系，完成试验模型的迎角测量。数值仿真试验结果表明：迎角测量误差与待测标记点到风洞壁板间的距离偏差近似为线性关系，因此，当标记点不满足共面条件时，可根据该特点进行测量误差修正。静态标定和风洞迎角测量试验结果表明：修正系统误差后，迎角实测数据的测量准度在0.01°以内，精度不超过0.012°。本文方法易于实施，工程实用价值强。     

基于点云数据的发动机管路最小间距计算方案

为检测整机发动机管路是否满足最小间距的设计要求,提出了一种基于点云数据的发动机管路最小间距计算方案,方案包含5个步骤:①从点云数据中划分出不同管路的数据;②基于管路点云数据的空间分布构造等间隔栅格,计算栅格中心点作为管路的趋势线数据;③在管路各趋势线数据点位置上构造垂直平面,将管路点云数据投影到最近的垂直平面上,获得各个垂直平面上呈圆弧状分布的投影点数据;④对各垂直平面上的投影点数据进行最小二乘圆拟合,得到拟合圆圆心及其半径值,将拟合圆圆心作为管路中心线数据;⑤采用遍历法计算两条管路中心线数据的最小间距,中心线最小间距分别减去两条管路的半径值则得到两条管路的表面最小间距。通过12条管路验证了方案的准确度。实验结果表明:管路最小间距偏差在-0.35~0.46mm之间,管路半径偏差在-0.08~0.22mm之间。该方案的实施有助于管路间距数字化检测的实现,且方案的计算结果具有较好的鲁棒性。      

Thrusting maneuver control of a small spacecraft via only gimbaled-thruster scheme

The thrust vector control (TVC) scheme is a powerful method in spacecraft attitude control. Since the control of a small spacecraft is being studied here, a solid rocket motor (SRM) should be used instead of a liquid propellant motor. Among the TVC methods, gimbaled-TVC as an efficient method is employed in this paper. The spacecraft structure is composed of a body and a gimbaled-SRM where common attitude control systems such as reaction control system (RCS) and spin-stabilization are not presented. A nonlinear two-body model is considered for the characterization of the gimbaled-thruster spacecraft where, the only control input is provided by a gimbal actuator. The attitude of the spacecraft is affected by a large exogenous disturbance torque which is generated by a thrust vector misalignment from the center of mass (C.M). A linear control law is designed to stabilize the spacecraft attitude while rejecting the mentioned disturbance torque. A semi-analytical formulation of the region of attraction (RoA) is developed to ensure the local stability and fast convergence of the nonlinear closed-loop system. Simulation results of the 3D maneuvers are included to show the applicability of this method for use in a small spacecraft.     

L-band nighttime scintillations at the northern edge of the EIA along 95°E during the ascending half of the solar cycle 24

The characteristics of nighttime ionospheric scintillations measured at the L-band frequency of 1.575 GHz over Dibrugarh (27.5°N, 95°E, MLAT ～ 17°N, 43° dip) during the ascending half of the solar cycle 24 from 2010 to 2014 have been investigated and the results are presented in this paper. The measurement location is within or outside the zone of influence of the equatorial ionization anomaly depending on solar and geomagnetic activity. Maximum scintillation is observed in the equinoxes irrespective of solar activity with clear asymmetry between March and September. The occurrence frequency in the solstices shifts from minimum in the June solstice in low solar activity to a minimum in the December solstice in high solar activity years. A significant positive correlation of occurrence of scintillations in the June solstice with solar activity has been observed. However, earlier reports from the Indian zone (～75°E) indicate negative or no correlation of scintillation in June solstice with solar activity. Scintillations activity/occurrence in solstices indicates a clear positive correlation with Es recorded simultaneously by a collocated Ionosonde. In equinoxes, maximum scintillations occur in the pre-midnight hours while in solstices the occurrence frequency peaks just after sunset. The incidence of strong scintillations (S₄ ≥ 0.4) increases with increase in solar activity. Strong (S₄ ≥ 0.4) ionospheric scintillations accompanied by TEC depletions in the pre-midnight period is attributed to equatorial irregularities whereas the dusk period scintillations are related to the sporadic-E activity. Present results thus indicate that the current location at the northern edge of the EIA behaves as low as well as mid-latitude location.