C4ISR仿真系统分析和设计

分析了指挥、控制、通讯、计算机、信息、监视和侦察(C4ISR)系统的复杂性特点,指出C4ISR系统在应用过程中,需要仿真系统对系统操作员和指挥员进行训练.研究了C4ISR仿真系统及其各子系统的实现模型,最后以舰艇C4ISR为例进行设计,通过分布式交互仿真协议(DIS)实现各子系统信息的互连.仿真结果表明,系统也可以为检测各种实际系统提供仿真环境和数据.     

坦克激光测距在虚拟仿真中的研究与实现

激光测距仿真是坦克火控模拟训练系统的一个重要组成部分,也是构建坦克射击虚拟战场环境仿真研究的重点.以坦克激光测距为仿真研究对象,依据光点式火控系统功能模拟原理和激光测距机性能指标,建立了三维视景中激光测距仿真的变换模型,实现了火控仿真系统中坦克对任意目标的激光测距.该模型仿真精度较高,效果逼真,对提高坦克射击乘员在观察测距、瞄准目标的训练成绩上有较好的促进作用.     

坦克火控系统误差分析及仿真系统设计与实现

分析了坦克火控系统的误差源,并以误差分析问题为背景,设计并实现了一个仿真平台,并将其应用于火控系统设计过程中,为精度分配算法提供支持.仿真系统应用火控系统的基本数学模型,通过模拟实际射击来获得火控系统输入误差与输出误差的传递关系,以此分析各误差源对系统精度影响的敏感程度,帮助设计者选择影响较为显著的误差源来进行修正,从而获得较高的系统精度.     

综合航电显控仿真系统的设计与实现

讨论了航空电子综合化仿真系统中显控子系统的设计与实现,主要探讨了此仿真系统的系统设计、系统管理、软件开发,以及整个系统的总线信息流管理.仿真系统的设计是采用某型飞机的总线拓朴结构,将各个子系统连接起来,以达到综合显示、综合处理、综合控制、数据综合传输、资源共享的目的.     

美军HPM效能评估模型及仿真工具箱

鉴于高功率微波(HPM)效应研究耗时、昂贵及其效能评估的复杂性,美国多个军种开发了能够在减少效应实验需求的同时进行效能评估的HPM评估模型及仿真工具箱.本文重点介绍了美军开发的DREAM、RF-PROTEC、JERM和HPM LAVA四款模型和仿真工具箱,对每款模型和工具箱的主要功能、特点、开发机构及诞生时间等进行了介...     

微机上运行的多功能仿真语言GASP/PC

文中介绍了IRM-PC机上多功能仿真软件GASP/PC的开发,叙述了GASP/PC仿真语言的形成以及对于连续、离散和复合仿真模型的GASP/PC语言的结构与仿真方法。     

系统仿真技术初探

为了对系统仿真技术有一个总体认识,采用归纳和分析的方法,对系统仿真技术的体系进行了初步探讨.     

基于测试码并行的同步时序电路故障模拟方法

将组合电路故障模拟的一些加速技术推广到时序电路故障模拟中,提出并实现了一个功能块级的基于测试码并行的同步时序电路故障模拟方法,对部分ISCAS89 Benchmark电路的模拟结果表明,该故障模拟方法有较好的性能.     

Study on performance degradation and failure analysis of machine gun barrel

An increase in the use of the gun barrel will cause wear of the inner wall, which reduces the muzzle velocity and the spin rate of the projectile. The off-bore flight attitude and trajectory of the projectile also change, affecting the shooting power and the accuracy. Exterior ballistic data of a high-speed spinning projectile are required to study the performance change. Therefore, based on the barrel's accelerated life test, the whole process of projectile shooting is reproduced using numerical simulation technology, and key information on the ballistic performance change at each shooting stage are acquired. Studies have shown that in the later stages of barrel shooting, the accuracy of shooting has not decreased significantly. However, it is found that the angle of attack of the projectile increases as the wear of the barrel increases. The maximum angle of attack reaches 0.106 rad when the number of shots reaches 4300. Meanwhile, elliptical bullet hole has appeared on the target at this shooting stage. Through combining external ballistic theory with simulation results, the primary reason of this phenomenon is found to be a significant decrease in the muzzle spin rate of the projectile. At the end of the barrel life, the projectile muzzle spin rate is 57.5% lower than that of a barrel without wear.     

Numerical simulation of the blast wave of a multilayer composite charge

The numerical simulation of a blast wave of a multilayer composite charge is investigated. A calculation model of the near-field explosion and far-field propagation of the shock wave of a composite charge is established using the AUTODYN finite element program. Results of the near-field and far-field calculations of the shock wave respectively converge at cell sizes of 0.25–0.5 cm and 1–3 cm. The Euler––flux-corrected transport solver is found to be suitable for the far-field calculation after mapping. A numerical simulation is conducted to study the formation, propagation, and interaction of the shock wave of the composite charge for different initiation modes. It is found that the initiation mode obviously affects the shock-wave waveform and pressure distribution of the composite charge. Additionally, it is found that the area of the overpressure distribution is greatest for internal and external simultaneous initiation, and the peak pressure of the shock wave exponentially decays, fitting the calculation formula of the peak overpressure attenuation under different initiation modes, which is obtained and verified by experiment. The difference between numerical and experimental results is less than 10%, and the peak overpressure of both internal and external initiation is 56.12% higher than that of central single-point initiation.