0.18 μm CMOS工艺的GPS/BDS双模可重构接收机射频前端

采用低中频架构设计了一种0.18μm CMOS工艺的GPS/BDS双模可重构接收机射频前端,能在GPS L1模式或BDS B1模式下工作。通过频率自适应电路调整中频滤波器的时间常数,降低其频率不确定度;压控振荡器中加入4位开关电容阵列,以提高频率调谐范围和相位噪声性能;通过硬件复用的方式降低系统功耗。测试结果表明,在1.8 V电源电压下,功耗37.8 m W,电压增益为103 d B,GPS L1和BDS B1波段噪声系数均小于3.2 d B。     

基于DDS的虚拟信号发生器LabVIEW程序设计

针对传统信号发生器存在的成本高、功能单一、电子线路复杂等缺点,设计了一种基于频率合成技术的虚拟任意信号发生器。通过动态链接库(DLL)与下位机设备DDS-3X25进行通信,基于"模块化"和事件结构的设计思想,用LabVIEW编程实现了基本波形、任意波形、噪声叠加、波形数据载入、波形数据量化转换和线性插值等程序模块。实验结果表明,该设计不仅能产生纯净和叠加噪声的正弦波、方波、三角波和锯齿波等基本波形,而且可以输出手绘的任意波形,验证了设计的有效性。     

基于路径规划的无人机飞行冲突解脱技术

在无人机与有人机共用空域时,随时可能发生飞行冲突,应当有一种可靠的冲突解脱技术,保证无人机的空域运行安全。为此,构建了基于正三角形栅格法的空域运行环境,改进了以往十字栅格环境规划动态路径的缺陷;提出了基于空间分割的改进蚁群算法,提高了算法的寻优性能与路径规划能力。最后结合ADS-B系统的工作原理,在利用卡尔曼滤波对ADS-B信息进行修正的基础上,设计了无人机冲突感知的技术方案,并用实时的路径重规划技术实现飞行冲突的解脱。最终的仿真实验验证了飞行冲突解脱技术方案的有效性,可为未来无人机的空域运行技术提供一定的理论参考。     

基于FRFT窄带滤波的LFM信号研究

随着分数阶傅里叶变换域窄带滤波技术的不断应用与发展,对分数阶域窄带滤波带宽的研究将变得尤为重要。研究了分数阶傅里叶变换域窄带滤波带宽与滤波后信号之间的关系,并以信号的失真度为准则,分析了分数阶域窄带滤波带宽的临界值。理论分析和仿真结果表明:线性调频信号经过分数阶域窄带滤波后信号的相位没有发生改变,信号的幅度为辛克函数积分的形式。为保证LFM信号频率信息不丢失,分数阶域窄带滤波的带宽必须不小于LFM信号在分数阶域幅度谱的主瓣宽度。为分数阶域滤波带宽的选取提供了参考标准。     

基于粒子群优化的蚁群算法在战场电磁频率分配中的应用

为对战场电磁频率进行有效分配以减少用频设备间的相互干扰,提出了将一种基于粒子群优化的蚁群算法应用于频率分配的方法。首先介绍了战场频率管控流程的相关内容,并以干扰度最低为目标函数,使用基于粒子群算法优化的蚁群算法进行频率分配管理。粒子群算法优化蚁群算法中启发信息的权重及信息素挥发系数,作为粒子群位置和速度参数进行初始化,将粒子群算法生成的分配结果作为蚁群算法的初始信息素,利用蚁群算法较强的寻优能力寻找最佳分配方案。实验结果验证了该算法和模型的可行性。     

玻璃瓶动态图像检测运动模拟平台

动态图像检测中,如何在指定位置快速而准确地捕捉到运动物体的图像是最基本的环节。试验验证图像检测装置的成像特性,成为动态图像检测研究的重要内容之一。以变频器控制电动机为核心,通过变频器内部参数编程和外部简单的辅助控制电路,构建了运动平稳、速度可调、具有自动保护功能的模拟平台。该平台适于动态图像检测中普通运动物体的快速模拟,已成功地用于玻璃瓶动态图像装置中,达到了预期目的。     

低频UWBSAR辐射校准模型

低频超宽带合成孔径雷达(Ultra Wide Band Synthetic Aperture Radar,UWBSAR)的辐射校准是系统研制和应用过程中必须面对的课题。低频UWBSAR的特点使得常规SAR辐射校准技术不再适用。充分考虑校准参数随频率和方位角的变化,给出适合该系统的辐射校准方法,得到低频UWBSAR图像辐射校准模型。利用该模型,对系统辐射校准误差进行了分析。     

非局部弹性杆固有频率的Ritz法求解

采用Ritz法求解了非局部弹性直杆的固有频率问题。非局部弹性理论与经典弹性理论相对应,区别在于非局部理论中,一点的应力与该点以及其周围区域的应变都有关,并采用核函数来表征这种相关性。基于Eringen提出的非局部弹性模型,针对三种给定核函数,用Ritz法进行了直杆的动力学分析。并针对两种边界条件给出直杆的固有频率,与其它方法比较,该方法具有可以针对多种核函数求解,精度可控,易于编程等优点。     

Sensor radiation interception risk control in target tracking

This paper is mainly on the problem of radiation interception risk control in sensor network for target tracking. Firstly, the sensor radiation interception risk is defined as the product of the interception probability and the cost caused by the interception. Secondly, the radiation interception probability model and cost model are established, based on which the calculation method of interception risk can be obtained. Thirdly, a sensor scheduling model of radiation risk control is established, taking the minimum interception risk as the objective function. Then the Hungarian algorithm is proposed to obtain sensor scheduling scheme. Finally, simulation experiments are mad to prove the effectiveness of the methods proposed in this paper, which shows that compared with the sensor radiation interception probability control method, the interception risk control method can keep the sensor scheduling scheme in low risk as well as protect sensors of importance in the sensor network.     

Experimental study on the detonation process of a pulse detonation engine with ionized seeds

An experimental platform of a pulse detonation engine (PDE) was established to study the effect of different K₂CO₃ ionized seed mass contents on the detonation process. The pressure and ion concentration were detected in the detonation process of the PDE with different contents of ionized seeds. The initiation process of the PDE at different ignition frequencies was studied. The results show that the gas conductivity in the detonation process increased by adding ionized seeds to the PDE tube, and the conductivity increased with the increase in ionized seed mass content. With the increase in ionized seed mass content, the range of the conductivity decreased. The PDE was successfully ignited and formed a stable detonation wave at ignition frequencies of 5 Hz and 10 Hz, and the peak pressure of the stable detonation with the ignition frequency of 5 Hz was 17% higher than that with an ignition frequency of 10 Hz. The detonation wave intensity was weakened and degenerated to a shock wave that propagated in the tube without the fuel filled at the ignition frequency of 20 Hz.