《单片机》课程教学研究

当前，单片机已成为电子系统智能化的最好工具。本文针对单片机教学过程中普遍存在的实际问题，从课堂教学、实验教学、课程实践三个方面进行了阐述，并提出了相应的解决方案。     

Yield Loci of TRIP590 Advanced High Strength Steel Based on Biaxial Loading Test

The main purpose of the paper is to obtain the experimental yield loci of TRIP590 advanced high strength steel,and to compare it with the theoretical loci in order to obtain the best yield criterion for this material. First,the biaxial loading tests under different loading paths in the method of load control are carried out. Then,the experimental yield loci of different deformation stages are obtained. Finally,the experimental yield loci are compared with the theoretical loci of Mises criterion and Hill48 criterion,the parameters of which are calculated based on the r-value and the yield stress method,respectively. The results show that the accuracy of the theoretical yield loci of Hill48 based on the yield stress is higher than that of Mises criterion and Hill 48 criterion based on r-value method.     

基于双向流固耦合方法的柔性变结构喷管性能分析

为研究柔性变结构喷管的高度补偿潜力,本项研究利用ANSYS平台,基于双向流固耦合方法,对柔性变结构锥型喷管进行数值模拟,分析了飞行高度和柔性材料的弹性模量对喷管性能的影响。模拟结果表明,随着飞行高度的升高,柔性喷管变形加剧,喷管内部流场呈现出膨胀波-激波-膨胀波的波系特征,喷管柔性段的最大型面变形量和壁面最大应力逐渐增大。当材料弹性模量大于100 MPa时,喷管柔性段型面变形对流场的影响将可以忽略。研究显示,该柔性喷管的低空比冲显著高于传统喷管,高空比冲仅略低于传统喷管,其6 km设计高度下较传统喷管有1.462%的高度积分比冲增益。     

基于DDK/XP的转台用测角板设备驱动及测试程序开发

基于WindowsXP下的DDK工具包,开发了转台用ISA测角板卡的设备驱动程序.阐述了WindowsXP的体系结构和驱动程序开发工具DDK.实现了I/O读写、内存读写和中断的设备驱动程序.介绍了设备驱动程序调试与安装.     

反导预警雷达部署方案的评价与优选

合理部署反导预警雷达对提高反导作战效能起着重要作用。反导预警雷达部署要考虑的因素较多,部分因素存在冲突。本文分析了反导预警雷达部署评价应考虑的因素,提出了相关评价指标,主要有不同配置距离下雷达对目标的发现概率、提供的预警时间、落点预报精度、全程跟踪目标时长等,建立了不同评价指标的计算方法,给出了反导预警雷达部署方案的综合评价与优选方法。本文方法对反导预警雷达部署方案的建立优选具有指导意义。     

VB与MATLAB混合编程在修磨机床软件中的应用

介绍了VB与MATLAB混合编程的4种方法,通过这些方法,可使VB的可视化界面和Matlab强大的计算及绘图功能得以实现,从而提高编程的效率,并在某产品CNC修磨机床的上位机数据处理软件中通过了验证.     

Review Article: MHD Wave Propagation Near Coronal Null Points of Magnetic Fields

We present a comprehensive review of MHD wave behaviour in the neighbourhood of coronal null points: locations where the magnetic field, and hence the local Alfvén speed, is zero. The behaviour of all three MHD wave modes, i.e. the Alfvén wave and the fast and slow magnetoacoustic waves, has been investigated in the neighbourhood of 2D, 2.5D and (to a certain extent) 3D magnetic null points, for a variety of assumptions, configurations and geometries. In general, it is found that the fast magnetoacoustic wave behaviour is dictated by the Alfvén-speed profile. In a ??=0 plasma, the fast wave is focused towards the null point by a refraction effect and all the wave energy, and thus current density, accumulates close to the null point. Thus, null points will be locations for preferential heating by fast waves. Independently, the Alfvén wave is found to propagate along magnetic fieldlines and is confined to the fieldlines it is generated on. As the wave approaches the null point, it spreads out due to the diverging fieldlines. Eventually, the Alfvén wave accumulates along the separatrices (in 2D) or along the spine or fan-plane (in 3D). Hence, Alfvén wave energy will be preferentially dissipated at these locations. It is clear that the magnetic field plays a fundamental role in the propagation and properties of MHD waves in the neighbourhood of coronal null points. This topic is a fundamental plasma process and results so far have also lead to critical insights into reconnection, mode-coupling, quasi-periodic pulsations and phase-mixing.     

An overview of RADOM results for earth and moon radiation environment on Chandrayaan-1 satellite

The RADiatiOn Monitor (RADOM) is a miniature dosimeter-spectrometer that flew onboard the Chandrayaan-1 lunar mission in order to monitor the local radiation environment. Primary objective of the RADOM experiment was to measure the total absorbed dose, flux of surrounding energetic particles and spectrum of the deposited energy from high energy particles both en-route and in lunar orbit. RADOM was the first experiment to be switched on after the launch of Chandrayaan-1 and was operational until the end of the mission. This paper summarizes the observations carried out by RADOM during the entire life time (22 October 2008–31 August 2009) of the Chandrayaan-1 mission and compares the measurement by RADOM with the radiation belt models such as AP-8, AE-8 and CRRESS.