空间绳网捕获动力学仿真

空间绳网捕获系统是一种很有前景的空间碎片清除方法。然而，绳网的部署与捕获过程非常复杂，截至目前仍存在少量关键问题有待解决。对绳网捕获过程的研究是为了得到更合理的初始释放条件，以便绳网在接触目标后能成功包裹目标。利用有限元法将绳网进行离散，建立弹簧质点模型，并通过有限元软件进行仿真。同时提出了与仿真相关的3个接触参数，通过对不同捕获模型接触参数的横向对比找出绳网系统在展开及捕获过程中接触行为的区别。仿真结果表明，采用方形绳网系统对于正方体与弧形薄壁体目标捕获效果相对较好，对球形目标的捕获效果相对较差。针对不同捕获物体，绳网中最大应力出现的位置也不同，但最大应力都是集中出现在绳网与捕获目标棱角接触处与牵引球连接处。该仿真结果对最优绳网初始释放条件与编织形式的选取具有指导意义。     

A novel adaptive lateral reentry guidance algorithm with complex distributed no-fly zones constraints

Aimed at complex distributed no-fly zones avoidance problems, a novel adaptive lateral reentry guidance algorithm is proposed. Firstly, by introducing the improved attractive and repulsive potential fields, an improved artificial potential field method is developed. Combined with the proposed judgment criterion for whether a no-fly zone has been avoided, the proposed improved artificial potential field method effectively solves the reference heading angle determination problem under the constrai...     

Autonomous mission reconstruction during the ascending flight of launch vehicles under typical propulsion system failures

In recent years, Chinese Long March(LM) launchers have experienced several launch failures, most of which occurred in their propulsion systems, and this paper studies Autonomous Mission Reconstruction(AMRC) technology to alleviate losses due to these failures. The status of the techniques related to AMRC, including trajectory and mission planning, guidance methods,and fault tolerant technologies, are reviewed, and their features are compared, which reflect the challenges faced by AMRC technology...     

短波红外全天时自主天文导航技术展望

基于2微米全天巡天（2MASS）短波红外巡天点源星表,分别从白天可探测恒星分布、天空背景辐射与大气传输、传感器性能和光学系统视场大小等方面,分析了短波红外波段相对于可见光波段,在大气层内白天观星实现全天时天文导航的优势,并展望了其发展方向。     

内并联型进气道模态转换过程中流道间干扰特性研究

针对组合动力进气道模态转换过程中存在的流道间干扰现象,采用数值模拟方法对一典型内并联型进气道模态转换过程中高/低速流道间的干扰特性展开了深入研究。结果表明：在模态转换过程中,当低速流道结尾激波位于低速流道内部时,高速流道节流至一定程度都将对低速流道形成干扰。该干扰现象出现后,高/低速流道的流动耦合,两流道的流量分配也随之发生变化,甚至导致了进气道流场的失稳。仅当β/α=0.25时,高/低速流道间的干扰造成了进气道流场的失稳且失稳后的振荡流场会先后出现两个不同的发展时期：前一时期的振荡流场的振幅较大但频率较低,约为335Hz；后一时期的振荡流场的振幅较小但频率较高,约为880Hz。