弹道式导弹自由飞行段弹头控制分析

文章基于相平面分析法 ,对弹道导弹弹头控制系统在自由飞行段产生的极限环进行深入的分析和推导 ,依照弹头控制系统在设计时所需要的数据推导出所需公式 ,为深入设计和理解弹头控制系统提供了有力的工具     

激励器结构对三电极等离子体高能合成射流流场及其冲量特性的影响

等离子体激励器以其结构简单、响应速度快、环境适应性强等优势,已成为主动流动控制技术和流体力学研究的前沿与热点。相比于传统两电极激励器,三电极等离子体高能合成射流激励器具有更高的能量效率,形成射流冲量更大,有望成为新型快响应直接力产生装置。为揭示激励器结构对射流流场和冲量特性的影响规律,进而优化激励器结构参数,利用电参数测量装置、高速阴影系统及自主设计的单丝扭摆式微冲量测量系统对不同射流孔径、腔体体积和电极间距的三电极激励器放电特性、射流流场及其冲量进行了实验研究。为对比激励器在不同工况条件下的工作特性,定义无量纲能量沉积ε和无量纲射流冲量 I *,并分析了激励器结构参数对ε和 I *的影响。结果表明对于给定无量纲能量沉积ε,激励器存在最优射流孔径;激励器无量纲能量沉积ε和无量纲射流冲量I *随腔体体积增加而减小,随激励器电极间距增加而增加;射流强度及其流场影响区域随腔体体积增加而减小,随激励器电极间距增加而增加。对比不同腔体体积和电极间距工况条件下 I *随ε的变化可知,为设计具有较好射流冲量水平的激励器,在相同无量纲能量沉积ε条件下,应尽量增大激励器无量纲射流冲量 I *。当设计激励器无量纲能量沉积ε小于初始工况时,应增大初始工况激励器腔体体积使无量纲能量沉积ε降低至设计值;当设计激励器无量纲能量沉积ε大于初始工况时,应增大初始工况激励器电极间距使无量纲能量沉积ε增加至设计值,使设计激励器具有较好的射流冲量水平。     

弹道导弹中段监视与跟踪仿真系统设计

随着反导防御系统的发展,弹道导弹突防将受到更大的威胁,而弹道导弹中段是攻防对抗集中体现的区域。本文以美国的天基红外预警系统为参考,对弹道导弹中段监视与跟踪仿真系统进行了研究,提出了仿真系统的体系结构,并对仿真模型的具体实现进行了详细的描述。系统的建立可为弹道导弹作战模拟提供研究平台,并可对面向空间预警的信息处理算法进行评估,为中段反导作战的具体影响提供有益的参考信息。     

捷联式重力定高引信的力学分析及其关键技术

根据地球的重力场特性控制弹道导弹的引爆高度，不但安全可靠，而且可以对抗电子干扰。保持惯性空间是测量重力场的重要保证。本文论证捷联式重力定高引信的力学原理，给出了详细的数学证明。最后根据实验结果，讨论了捷联式重力测高引信的关键技术。     

弹道导弹显式制导的分析与研究

弹道导弹的制导方法是影响弹道导弹命中精度的关键因素。本文对此进行了深入研究。文章首先分析了影响制导精度和速度的原因。在此基础上，提出了一种基于神经网络的显式制导方法，这种方法利用神经网络进行弹道约束函数的解算，利用微分控制算法进行控制量求解，具有较好的应用价值，文中算例验证了算法的有效性。     

Whipple防护屏弹道极限参数试验

在中国空气动力研究与发展中心FD-18A超高速碰撞靶上进行了Whipple防护屏的超高速撞击试验。弹丸为LY12铝球,撞击速度为4.5km/s,撞击角为0°。通过固定弹丸速度、变弹丸直径、寻找弹丸临界直径的办法获得了该Whipple防护屏在试验条件下的弹道极限参数。试验结果表明速度为4.5km/s时的弹丸临界直径为0.35cm,大于用Christiansen方程预测的0.27cm。     

旋转倒立摆的神经网络控制

本文针对一种新型的倒立摆系统,设计了一个四输入单输出三层BP网络,并对一级旋转倒立摆控制器进行逼近。仿真结果表明,BP神经网络有很广阔的应用领域。     

旋转倒立摆的神经网络控制

本文针对一种新型的倒立摆系统,设计了一个四输入单输出三层BP网络,并对一级旋转倒立摆控制器进行逼近.仿真结果表明,BP神经网络有很广阔的应用领域.     

Properties of transit trajectory in the restricted three and four-body problem

In the restricted three-body problem if the Jacobi constant is just below the value corresponding to Lagrangian point only a little neck exists around the equilibrium point and capture trajectories are indicated as low-energy. Capture properties depend on the dynamics around these critical points and qualitative results can be obtained using linearized systems. In this paper, to study transit trajectory properties in the restricted three and four-body problem, the Earth–Moon–Sun–Satellite system is considered as example and studied using different models. In the circular restricted three-body problem (Earth–Moon–Satellite), transit, non transit and asymptotic trajectories, are easily identified by using the principal reference frame. Dynamics around Lagrangian point are then studied introducing the Moon eccentricity into the elliptical restricted three-body model. A preferential region for transit orbit is individuated and studied as a function of eigenvalue properties. To introduce the Sun effect, the bi-circular four-body model is considered and dynamics around Lagrangian points studied as a function of angular distance between Earth–Sun and Earth–Moon line. Finally, results obtained in the elliptical three-body model and bi-circular four-body model, are compared with numerical simulations using real Sun–Moon–Earth ephemeris.     

Contingency and recovery options for the European Student Moon Orbiter

This paper presents an overview of the analysis performed on the lunar orbit and some of the possible contingencies for the European Student Moon Orbiter (ESMO). Originally scheduled for launch in 2014 –2015 as a piggyback payload, it was the only ESA planned mission to the Moon. By way of a weak stability boundary transfer, ESMO is inserted into an orbit around the Moon. Propellant use is at a premium, so the operational orbit is selected to be highly eccentric. In addition, an optimization is presented to achieve an orbit that is stable for 6 months without requiring orbit maintenance. A parameter study is undertaken to study the sensitivity of the lunar orbit insertion. A database of transfer solutions across 2014 and 2015 is used to study the relation between the robustness of weak capture and the planetary geometry at lunar arrival. A number of example recovery scenarios, where the orbit insertion maneuver partially or completely fails, are also considered.