一个功能较强的等离子体电磁波粒子模拟程序

本文发展了一个功能较强的1 2/2D 等离子体粒子模拟程序。文中就一维情况,论述了等离子体粒子模拟的原理、方法和计算机编程中的处理技巧。最后讨论了电磁模拟的应用。     

15cm×15cm 磁悬挂天平系统(MSBS)的电磁场分析与计算

本文采用二维电磁场有限元法及磁路的简化计算法对15cm×15cm磁悬挂天平系统（MSBS）的阻力线圈间距、磁场的分布情况进行了分析计算,并与测试结果进行了分析比较,给出了15cm×15cm磁悬挂天平系统（MSBS）的结构方案。     

一种基于三角面元的目标RCS实用计算方法

提出一种计算复杂目标高频区RCS的实用方法。首先采用3DStudioMax对装甲车进行三角面元模拟,然后运用路德维格积分[1]和物理绕射理论(PTD)计算目标的雷达散射截面积,通过对方柱RCS的计算,验证了所提方法的有效性,最后给出了C波段和X波段不同极化的装甲车和坦克RCS的方位分布图。     

某加农炮身管内膛烧蚀磨损对内弹道性能的影响

通过对某加农炮的身管烧蚀磨损特征数据进行分析整理,确定了身管烧蚀磨损特征面,采用了多特征面来表述火炮内弹道性能变化。将该研究方法具体用于某加农炮身管特性的研究,建立了该加农炮的内弹道性能与其身管内膛烧蚀磨损特征量之间的关系模型。     

弹道导弹防御系统的现状与发展

本文综述了美国退出《反弹道导弹条约》以来,如何调整弹道导弹防御计划,制定新的发展战略,实施各种防御技术,初步建立防御能力,并论述了美国弹道导弹防御系统的现状与发展趋势。     

BM弹头雷达一维像干扰初探

根据目前反导雷达使用宽带信号对目标进行一维成像,检测目标几何特征的特点,从弹道导弹(BM)弹头雷达一维像(HRRP)特征出发,参照宽带线性调频雷达成像原理,讨论了对BM弹头HRRP可采取的几种电子干扰措施,包括对BM弹头HRRP的模拟和遮盖,给出了模拟BM弹头HRRP时所需生成的各信号特征,分析了每种遮盖干扰信号的功率利用情况,最后分析了每种干扰措施的优缺点。     

"标准-3"拦截弹对机动弹头的拦截有效性分析

以"标准-3"拦截弹的多次拦截试验情况为参考,根据其能力及试验中的表现,分析其总体设计方案和各项性能参数,建立数学仿真模型.在研究海基导弹防御指挥控制流程、拦截弹动力学模型和仿真算法的基础上,对拦截具有机动突防能力的弹道导弹目标进行仿真分析.获得拦截弹对机动突防目标拦截有效性的仿真结果.分析仿真结果可知,拦截弹对机动弹头的拦截能力有限.     

反解法在再入机动弹道设计中的应用研究

简要分析了一般的再入机动弹道设计方法,即正解法.针对正解法对模型依赖性强和对初值非常敏感的问题,提出了一种基于误差补偿的机动弹道设计方法——反解法.该方法从弹道终端出发反解弹道,将计算结果误差转化为机动点参数误差,再通过关机点或中制导的调整进行误差补偿,从而有利于命中精度和打击效果的实现.仿真结果表明,该方法计算简便,对工程应用有一定的参考价值.     

5GHz雷达的干扰计算模型概述

文章从开发5 GHz模型的目的入手,简要介绍了5 GHz模型的结构组成,详细讨论了5 GHz模型的干扰计算流程,包括无线局域网和雷达的场景设置、技术参数设置、总干扰计算等,最后给出了5 GHz模型的一个运行范例,以期为其它干扰模型的开发提供借鉴参考。     

Effects of nano-sized aluminum on detonation characteristics and metal acceleration for RDX-based aluminized explosive

Nano-sized aluminum(Nano-Al)powders hold promise in enhancing the total energy of explosives and the metal acceleration ability at the same time.However,the near-detonation zone effects of reaction between Nano-Al with detonation products remain unclear.In this study,the overall reaction process of 170 nm Al with RDX explosive and its effect on detonation characteristics,detonation reaction zone,and the metal acceleration ability were comprehensively investigated through a variety of experiments such as the detonation velocity test,detonation pressure test,explosive/window interface velocity test and confined plate push test using high-resolution laser interferometry.Lithium fluoride(LiF),which has an inert behavior during the explosion,was used as a control to compare the contribution of the reaction of aluminum.A thermochemical approach that took into account the reactivity of aluminum and ensuing detonation products was adopted to calculate the additional energy release by afterburn.Combining the numerical simulations based on the calculated afterburn energy and experimental results,the param-eters in the detonation equation of state describing the Nano-Al reaction characteristics were calibrated.This study found that when the 170 nm Al content is from 0％to 15％,every 5％increase of aluminum resulted in about a 1.3％decrease in detonation velocity.Manganin pressure gauge measurement showed no significant enhancement in detonation pressure.The detonation reaction time and reaction zone length of RDX/Al/wax/80/15/5 explosive is 64 ns and 0.47 mm,which is respectively 14％and 8％higher than that of RDX/wax/95/5 explosive(57 ns and 0.39 mm).Explosive/window interface velocity curves show that 170 nm Al mainly reacted with the RDX detonation products after the detonation front.For the recording time of about 10 μs throughout the plate push test duration,the maximum plate velocity and plate acceleration time accelerated by RDX/Al/wax/80/15/5 explosive is 12％and 2.9 μs higher than that of RDX/LiF/wax/80/15/5,respectively,indicating that the aluminum reaction energy significantly increased the metal acceleration time and ability of the explosive.Numerical simulations with JWLM explosive equation of state show that when the detonation products expanded to 2 times the initial volume,over 80％of the aluminum had reacted,implying very high reactivity.These results are significant in attaining a clear understanding of the reaction mechanism of Nano-Al in the development of aluminized explosives.