火星大气进入段抗饱和固定时间阻力加速度跟踪制导律设计

研究了具有固定时间收敛特性的火星探测器大气进入段的标称轨迹跟踪制导问题。首先，针对横向运动，给出与速度成线性关系的航向误差漏斗走廊形式，完成了倾侧角的反号逻辑设计。与横程漏斗走廊反号逻辑相比，该逻辑计算量小，更适用于宇航计算机。与航向误差宽度走廊反号逻辑相比，该逻辑在高速状态下能够避免倾侧角的频繁切换，可提高任务成功的概率。其次，针对纵向运动，通过RBF神经网络补偿了倾侧角饱和问题，利用积分滑模设计了阻力加速度固定时间饱和跟踪制导律，其不仅可有效消除滑模控制的抖振问题，且将跟踪误差以两种不同形式引入制导律，能够加速收敛，能够保证跟踪误差在固定时间内快速收敛至0。最后，通过数值仿真验证了所设计的横向倾侧角切换逻辑和纵向制导律对标称轨迹的快速、精确跟踪能力。     

退化发动机加速性能恢复控制方法

针对退化发动机加速性能下降的现象,提出一种变喘振裕度约束的模型预测控制方法。通过分析退化发动机在加速过程中的工作特点,将加速过程分为三个阶段,在不同阶段采取不同的喘振裕度约束。鉴于模型预测控制能够显式处理约束、采用在线滚动优化来获取最优控制输入,采取模型预测控制方法,并采用具有较高实时性的交替方向乘子法求解优化问题,实现了退化发动机加速性能的恢复。数字仿真结果表明,采用本文所提出的加速性能恢复控制方法后,相比退化发动机,加速过程中所耗费的时间缩短了35%以上。     

小样本条件下多应力加速寿命试验预测方法

鉴于导弹中的电子设备价格昂贵、可用于试验的样本量少,在开展加速试验以及寿命预测的实际工作中通常为小样本的背景。文章研究探索小样本条件下多应力加速试验寿命预测方法,分别建立通用对数线性模型、 BAS-BP神经网络模型、灰色–支持向量回归模型,结合多应力加速试验数据在各应力条件下的样本容量分别为 56组、20组、10组、5组的情况下,比较 3种模型的预测效果,分析各模型的适用场合和时机,探索小样本条件下模型的选优问题,为小样本条件下多应力加速试验寿命预测提供有益的借鉴。     

基于加速度测量的智能桁架结构振动主动控制

加速度传感器具有频带宽、结构简单、重量轻等优点而获得了广泛使用，因此研究基于加速度测量的结构控制系统具有较大的实用价值。文中的只能获得加速度时，采用模态滤波器技术实现从物理加速度响应解耦得到单模态加速度的响应。然后改变Ｌｕｅｎｂｅｒｇｅｒ观测器的结构形式，从模态加速度响应观测得到模态们移和模态速度响应。基于模态滤波器和最优控制理论，采用独立模态空间控制策略，实现了具有密集模态的三维柔性智能桁架结构     

利用航天器分舱段振动试验数据获取整器响应的方法

未来大型组合体航天器振动试验可能难以在现有设备上进行,需要进行分舱考核。文章针对此问题开展了利用分舱段振动试验获取整器响应的方法研究。提出的方法为:根据不同界面下模态的映射关系,利用单舱段的振动试验数据辨识出舱段的两端固支模态;采用模态综合技术计算出整器组合体模态参数,拟合出结构的加速度响应传递函数;结合整器的加速度试验条件可以给出整器的试验响应曲线。仿真验证结果表明该方法合理可行,具有工程应用价值。     

MP＊中的等值完全析取范式

讨论中介逻辑命题演算扩张系统ＭＰ＊中在等值意义下的完全析取范式的存在性和唯一性。引入ＭＰ＊中等值全板范式的概念，并用分步构造法证明这种范式在等值意义下是存在的，且是唯一的。     

一种支持 NF￣2 和多媒体的数据模型

支持ＮＦ２（Ｎｏｎ－ｆｉｒｓｔ－ｎｏｒｍａｌ－ｆｏｒｍ）和多媒体的数据库系统ＮＦＭＤＢ是在关系数据库ＲＤＢＭＳ的基础上研制的，它是一种扩充了的ＤＢＭＳ。系统采用了扩充的关系数据模型，它支持ＮＦ２和多媒体的数据存储和数据操作。本文重点介绍了ＮＦＭＤＢ系统支持ＮＦ２和多媒体的数据模型，以及基于数据字典的实现方案，系统具有处理复杂对象的能力。     

Cosmic ray acceleration by supernova shocks

We analyse the results of recent measurements of nonthermal emission from individual supernova remnants (SNRs) and their correspondence to the nonlinear kinetic theory of cosmic ray (CR) acceleration in SNRs. It is shown that the theory fits these data in a satisfactory way and provides the strong evidences for the efficient CR production in SNRs accompanied by significant magnetic field amplification. Magnetic field amplification leads to considerable increase of CR maximum energy so that the spectrum of CRs accelerated in SNRs is consistent with the requirements for the formation of Galactic CR spectrum up to the energy ∼10¹⁷ eV.     

Particle Acceleration Mechanisms

In this paper we review the possible mechanisms for production of non-thermal electrons which are responsible for the observed non-thermal radiation in clusters of galaxies. Our primary focus is on non-thermal Bremsstrahlung and inverse Compton scattering, that produce hard X-ray emission. We first give a brief review of acceleration mechanisms and point out that in most astrophysical situations, and in particular for the intracluster medium, shocks, turbulence and plasma waves play a crucial role. We also outline how the effects of the turbulence can be accounted for. Using a generic model for turbulence and acceleration, we then consider two scenarios for production of non-thermal radiation. The first is motivated by the possibility that hard X-ray emission is due to non-thermal Bremsstrahlung by nonrelativistic particles and attempts to produce non-thermal tails by accelerating the electrons from the background plasma with an initial Maxwellian distribution. For acceleration rates smaller than the Coulomb energy loss rate, the effect of energising the plasma is to primarily heat the plasma with little sign of a distinct non-thermal tail. Such tails are discernible only for acceleration rates comparable or larger than the Coulomb loss rate. However, these tails are accompanied by significant heating and they are present for a short time of <10⁶ years, which is also the time that the tail will be thermalised. A longer period of acceleration at such rates will result in a runaway situation with most particles being accelerated to very high energies. These more exact treatments confirm the difficulty with this model, first pointed out by Petrosian (Astrophys. J. 557:560, 2001). Such non-thermal tails, even if possible, can only explain the hard X-ray but not the radio emission which needs GeV or higher energy electrons. For these and for production of hard X-rays by the inverse Compton model, we need the second scenario where there is injection and subsequent acceleration of relativistic electrons. It is shown that a steady state situation, for example arising from secondary electrons produced from cosmic ray proton scattering by background protons, will most likely lead to flatter than required electron spectra or it requires a short escape time of the electrons from the cluster. An episodic injection of relativistic electrons, presumably from galaxies or AGN, and/or episodic generation of turbulence and shocks by mergers can result in an electron spectrum consistent with observations but for only a short period of less than one billion years.     

Alfvénic Electron Acceleration in Aurora Occurs in Global Alfvén Resonosphere Region

Auroral emission caused by electron precipitation (Hardy et al., 1987, J. Geophys. Res. 92, 12275–12294) is powered by magnetospheric driving processes. It is not yet fully understood how the energy transfer mechanisms are responsible for the electron precipitation. It has been proposed (Hasegawa, 1976, J. Geophys. Res. 81, 5083–5090) that Alfvén waves coming from the magnetosphere play some role in powering the aurora (Wygant et al., 2000, J. Geophys. Res. 105, 18675–18692, Keiling et al., 2003, Science 299, 383–386). Alfvén-wave-induced electron acceleration is shown to be confined in a rather narrow radial distance range of 4–5 R _E (Earth radii) and its importance, relative to other electron acceleration mechanisms, depends strongly on the magnetic disturbance level so that it represents 10% of all electron precipitation power during quiet conditions and increased to 40% during disturbed conditions. Our observations suggest that an electron Landau resonance mechanism operating in the “Alfvén resonosphere” is responsible for the energy transfer.