遥控两栖车控制系统的软硬件设计

遥控两栖车的控制系统由控制端和受控端2部分组成.控制端负责采集各种驾驶信号,然后通过电台将控制信号传输到受控端.受控端接收到控制信号后,使相应的执行机构动作,达到车辆的遥控驾驶.本文着重进行了控制端的软硬件设计.该系统在试验中各项性能达到了使用要求.     

两栖装甲车辆车体应力试验分析

针对两栖装甲车辆装甲板裂纹现象,设计了表面应力测试试验.通过对某型两栖装甲车辆进行试验,并对采集的数据处理分析,获得了车体裂纹频发位置的主应力分布,验证了装甲板表面主应力是导致产生裂纹的主要因素,为解决裂纹问题提供了理论依据.     

系统动力学C3I系统作战效能评估

C3I系统效能评估是C3I系统发展的重要问题,现有的ADC法、指数法、层次分析法和SEA方法等都存在着某种局限性,也无法度量C3I系统与作战结果的关系.系统动力学是一门分析研究信息反馈系统的学科,适合于研究C3I系统的系统效能和作战效能之间的定量关系.以一个具体的关于C3I系统的作战想定为例,构建了该C3I作战系统的因...     

面向多学科语义的运载火箭集成设计数据管理方法

针对当前集成设计系统中多学科数据管理存在的不足,在分析运载火箭集成设计工作流数据特点基础上,提出了面向多学科语义的统一数据描述方法和数据的动态集成与调度策略,简化了集成设计中数据的描述和访问机制,分离了软件开发员与多学科用户的职责权限.通过在某型运载火箭集成设计系统中的应用,表明该方法可将流程处理与数据处理分离,能有效...     

载机军舰航空燃油分段接力式补给模型

为解决载机军舰远洋作战时所需的航空燃油按时补给问题,建立了带有自动调节系统的载机军舰航空燃油分段接力式补给的预测模型。对航空燃油分段接力式补给进行研究,采用系统动力学方法,构建影响补给船队补给效率的各元素因果回路图与存量流量图及预测模型,并以系统动力学软件Vensim PLE 5.9为平台进行建模仿真。运行结果表明,该模型在扰动条件下能进行航空燃油分段接力式补给趋势的预测,可为航空燃油分段接力式补给方案的制定提供理论依据。     

履带装甲车辆采用永磁同步电动机驱动研究

为了提高车辆的机动性能,世界各国纷纷开展电传动系统研究。采用永磁同步电动机控制系统作为电传动车辆的驱动系统是可行方案之一。文中建立了永磁同步电动机控制系统的数学模型,提出了适合于履带车辆电传动系统的电机控制策略与方法,并将永磁同步电动机控制系统在履带车辆电传动中应用进行仿真与分析,最后,给出了永磁同步电动机控制系统在装甲车辆电传动中应用可行的结论。     

反辐射无人机在电子战中的应用及其效能分析

简要讨论了反辐射无人机系统的组成和两种典型的反辐射无人机,指出了其在电子战中的应用。并针对某型反辐射无人机的系统能力,即命中概率和毁伤概率进行了理论分析和计算。     

复合固体推进剂颗粒填充模型及其统计特性分析

复合固体推进剂属于高填充比颗粒类复合材料,氧化剂和金属颗粒在基体中的随机分布使其在细观尺度具有非均质的特点。从细观尺度研究固体推进剂燃烧及力学性能时,必须考虑颗粒级配、空间分布和种类等因素的影响。采用分子动力学方法,以硝酸酯增塑聚醚高能复合固体推进剂为研究对象,将固体颗粒模型化为球形,生成其在基体内随机分布的颗粒填充模型。利用Monte-Carlo算法模拟计算颗粒填充模型细观结构的两点概率函数,并研究了颗粒填充体积分数、尺寸与级配等参数对其的影响规律。从统计意义上给出具有各态历经性、统计均匀性和各向同性特点的颗粒填充构型最小周期性代表体元尺寸,可有效减小后续研究的计算量,节约计算成本。所构建的推进剂细观几何构型及对最小周期性代表体元尺寸的计算为后续开展复合固体推进剂细观尺度燃烧、燃面处铝团聚及力学性能数值研究奠定了基础。     

An efficient and modular modeling for launch dynamics of tubed rockets on a moving launcher

This paper develops a modular modeling and efficient formulation of launch dynamics with marching fire (LDMF) using a mixed formulation of the transfer matrix method for multibody systems (MSTMM) and Newton-Euler formulation. Taking a ground-borne multiple launch rocket systems (MLRS), the focus is on the launching subsystem comprising the rocket, flexible tube, and tube tail. The launching subsystem is treated as a coupled rigid-flexible multibody system, where the rocket and tube tail are treated as rigid bodies while the flexible tube as a beam with large motion. Firstly, the tube and tube tail can be elegantly handled by the MSTMM, a computationally efficient order-N formulation. Then, the equation of motion of the in-bore rocket with relative kinematics w.r.t. the tube using the Newton-Euler method is derived. Finally, the rocket, tube, and tube tail dynamics are coupled, yielding the equation of motion of the launching subsystem that can be regarded as a building block and further integrated with other subsystems. The deduced dynamics equation of the launching subsystem is not limited to ground-borne MLRS but also fits for tanks, self-propelled artilleries, and other air-borne and naval-borne weapons undergoing large motion. Numerical simulation results of LDMF are given and partially verified by the experiment.     

Noise and vibration measurements in a Viking military vehicle

Noise and whole-body vibration measurements were made in a Viking military vehicle to determine the variation that should be expected during repeat measures, the effect of speed (up to 60 km/h in 5 km/h increments), and during travel over different types of terrain (comprising concrete road, gravel track and rough cross-country). Measurements were made at various crew positions (including the driver and commander) in both the front and the rear cabs in the vehicles. Three translational axes of vibration were measured in each seat. Two speeds were investigated over road (35 km/h and 55–60 km/h) and gravel (20 km/h and 35 km/h) surfaces. The effect of varying speed of the vehicle on the measured noise and vibration magnitudes was also investigated. The highest sound pressure level (L_Aeq) of 104 dB(A) was measured at the commander’s standing position during travel over concrete road at 55 km/h. Higher noise levels occurred for a standing commander compared with when sitting on the seat. A maximum single axis frequency-weighted vibration magnitude of 1.0 m/s² r.m.s. was measured on the driver’s seat during travel over track at 35 km/h. Higher vibration magnitudes occurred during travel over track compared with travel over road. Both noise and vibration exposure of crew within the Viking vehicle increased with increasing speed of the vehicle.