倍流整流DC-DC变换器近场耦合集成磁件分析

利用磁性元件磁场近场泄漏的耦合,分析其在倍流整流变换器磁集成结构上的应用。采用磁路-电路对偶等效变换获得近场耦合集成磁件的等效电路模型,直观地对两种现有磁集成方案进行统一描述。论文详细分析集成磁件磁心内部的交、直流磁通分布。基于磁件的回转器-电容模型,对不同近场磁阻下电路的工作情况进行深入的讨论。建立48V输入、12V/90W输出的磁集成原理样机,并进行实验验证和性能评估。     

差值法测量脉冲电容器的等效电感

本文对几种测量脉冲电容器等效电感的方法作了评述,介绍差值法测量的原理和方法。对差值法进行了误差分析,提出它的应用条件。对三种类型电容器作了实验研究,我们发现,当外回路电感小于脉冲电容器等效电感的8.3倍时,等效电感的相对误差小于放电电流周期或电压周期测量的相对误差的15倍。     

天线平面近场测量的扫描面位置误差分析

本文基于天线平面近场测量技术的基本理论,利用数值分析方法深入分析了天线平面近场测量中有限扫描面位置误差,及其对天线远场特性和测量精度的影响.通过与理论结果的比较,给出了扫描面位置误差源所产生误差和误差的数量级,即天线方向性图的不确定度.该研究为天线近场测量技术的误差补偿提供了一定的理论依据.     

基于多通道控制器的扫频近场测量

为了对被测天线进行快速？定量的动态测量,获得天线频带特性的实时测量结果,可以采用多通道扫频近场测量方法。本文提出了一种采用85301B天线自动测量系统,使用HP85330A作为系统控制器的多通道扫频近场测量方法。在一定的频段内进行点频和扫频测试,将点频和扫频近场数据变换成远场方向图,并对各频点的数据进行比较分析。最后分析了误差产生原因并给出了一种修正方法。测试数据表明与传统的点测法相比,有效地降低了测量时间,提高了测量系统的测试效率。     

天线平面近场测量的扫描面截断误差分析

本文基于天线平面近场测量技术的基本理论,利用解析法和数值分析法研究分析了天线平面近场测量中有限扫描面截断误差对天线远场特性结果的影响,给出了有限扫描面截断误差所带来的天线辐射方向性图的误差的数量级,即天线方向性图的不确定度,为天线近场测量技术的误差补偿提供了一定的理论依据,同时也得到了一些对实际测量有一定指导意义的结论.     

一种新型磁集成倍流整流半桥变换器

为提高开关电源的效率和功率密度,提出一种新型倍流整流变换器的磁集成方案.结合半桥变换器的工作原理,详细分析集成磁件内部交、直流磁通分布.推导出集成磁件的等效电路模型,评估集成磁件的等效参数测量.提出两种副边绕组为一匝的解决方案,可获得最短绕组路径或消除泄露磁场.建立样机验证该方案的可行性,并对各种集成磁件间转化机理和应用特点进行总结.     

天线近场测量分析仪系统的研究

本文主要论述了一种计算机辅助的天线近场测量分析仪系统的结构、控制系统的硬软件结构设计及实现方法，并给出了有关的测量数据。结果表明，该分析仪系统是一部多功能、高精度的天线自动化测量分析系统。     

近场声全息测量研究

本文探讨了进行近场声全息测量时需要考虑的问题。文中指出全息测量面到声源重建面的距离应在最小波长范围内,并且与系统的动态范围和空间分辨率有关,传声器之间的间距应不大于最小波长的二分之一,传声器阵所扫描的全息测量面的尺寸至少为最大波长的一倍以上。参考传声器须放置在非相干声源附近,数目不应小于非相干声源的数目。测量的数据需要进行波数域滤波,提高信噪比,改善重建精度。     

基于面积流测量先进技术的研究

风量测量装置发展几十年以来,出现了十几种形式各异的产品,取得了长足的进步,各种产品都有其优点和缺点,能否较好的解决测量问题,关键在于风量测量装置的选型。着重讨论了在火力发电领域几种主流的风量测量装置的技术对比情况。     

Circular scanning and equivalent magnetic currents for main plane near‐field to far‐field transformation

A method to obtain a main plane far‐field radiation pattern of an antenna under test (AUT) from the correspondent main plane near‐field pattern in a circular scanning is presented. The method is based on the reconstruction of a set of magnetic equivalent currents radiating in free space that represents the AUT. The method can be applied to the measurement of antennas with a linear distribution or with a two‐dimensional distribution under certain considerations that allow to establish integral equations relating field components and one‐dimensional current components. A Levenberg–Marquardt algorithm is used to minimize the least squares error between the fields radiated by the equivalent currents and the measured field. The far field at every aspect angle is obtained from the calculated sources. Calculations of co‐polar and cross‐polar far‐field pattern from measured near‐field data of array antennas have been carried out to compare the proposed method with a full spherical scanning followed by a spherical wave expansion method. Copyright © 2002 John Wiley & Sons, Ltd.     

基于等效磁荷法的永磁电机Halbach阵列磁极磁场分析

基于等效磁荷法推导出永磁电机转子磁极——瓦形磁体在空间的磁场分布。同时用有限元法进行了分析,表明两者之间偏差较小,等效磁荷法满足计算精度要求。进而利用该方法建立了永磁电机的Halbach分布转子磁极静态磁场的模型,通过改变影响转子磁极磁场分布的极弧比和副磁极磁化角度两个因素,得到在不同磁极结构下的转子磁极静态磁场径向分量变化规律:每一极中主磁极空间跨度变大会导致Halbach永磁电机转子磁极静态磁场的径向分量基波幅值变大,而谐波含量先减小后增大;随着副磁极磁化角度变大,转子静态磁场的基波幅值先变大后减小,而谐波含量刚好相反,先减小后变大。     

PLC近场测量天线适用性分析

讨论了PLC电磁辐射的近场测量问题,从近场耦合和相位不均2方面仿真分析了CISPR规定的鞭天线、环天线的适用性,为实际测量中天线的选用提供了依据。通过分析证明,近场时可以忽略两天线之间的近场耦合。     

分布式脉冲磁场测量系统研究

脉冲磁场测量是电磁防护领域的重要研究内容之一,是电磁脉冲研究的基础.基于巨磁电阻(GMR)片研制的三维脉冲磁场测量探头,具有结构简单、体积小、测量范围宽,响应频率高等优点.通过实验标定,探头可以较好地测量三维脉冲磁场,磁场强度的测量范围为-40～+40 Gs,测量频率范围0～1 GHz.将探头测量的磁场信号转换为电压信号后,由TMS320F28335 DSP采集并存储在SD卡后,通过CAN总线组网,构建分布式脉冲磁场测量系统.结果证明,该系统具有组态灵活、测点容量大、抗干扰能力强、并能够实现三维脉冲磁场测量等特点.     

非均绕等安匝法试验下电流互感器铁心磁场的研究

为更好揭示以非均绕等安匝法测试电流互感器误差的原理,用有限元法计算分析了电流互感器的三维非工作磁场、铁心中合成磁场的分布及其随一次绕组在铁心上缠绕角度改变的变化特征.研究表明,电流互感器铁心中因外部电流、短路故障等环境影响产生的杂散磁场,完全可能通过改变一次绕组在铁心圆周上缠绕角度得到的相应磁场加以模拟.     

Time-domain magnetic field waveform measurement near printed circuit boards

This paper describes a time domain magnetic field measurement process for measuring magnetic fields near printed circuit boards (PCBs) with a loop probe. In carrying out these measurements, the loop probe needs to be calibrated in the frequency domain. In this process, a microstrip line with a teflon substrate serving as the standard magnetic field source is employed as a means of calibrating the probe. The standard magnetic field intensities of the line are calculated by using an approximate equation obtained from Ampère's law to simplify the calibration. The sensor-factor of the probe obtained from this method agrees with that obtained through the use of a standard G-TEM cell in 2 dB at frequencies below 1 GHz. The waveforms of magnetic fields near a PCB having a four-layer construction are measured using a 10 mm diameter loop probe as the calibrated magnetic field sensor. The generation of magnetic field waveforms causing the radiated emission from the PCB is found to depend on the circuit operating conditions. Our results clarify the fact that the time domain magnetic field measurement process is an effective tool for analyzing the sources of emission radiated from PCBs and for investigating the radiation mechanism. © 1998 Scripta Technica, Electr Eng Jpn, 125(4): 9–18, 1998     

汽轮发电机在饱和与磁场畸变时负载励磁电流计算的新方法

磁路饱和与磁场畸变的共同作用会使发电机负载饱和特性显著偏离其空载特性,为了计算这种差异,提出了其负载励磁电流计算的一种改进方法.以300 MW汽轮发电机为例,以有限元方法为工具,获得了反映磁路饱和与磁场畸变共同作用下负载非线性特性的关系曲线族,提出了用这种新曲线族代替空载特性计算负载励磁电流的新方法.通过计算发电机在不同功角下的负载励磁电流,说明该方法比传统方法有较高的计算精度,比有限元方法有较快的计算速度.     

Calculation of magnetic near field generated by the contact discharge of an ESD gun

An ESD (electrostatic discharge) testing is specified in the IEC 61000‐4‐2, in which the detailed waveform of the discharge current injected by an ESD gun is prescribed. However, due to lack of understanding of the discharge process, it is difficult to confirm whether or not the IEC current waveform can be injected onto actual equipment. We thus previously proposed an equivalent circuit model for the ESD gun based on its geometrical structure, and showed decisive factors for the discharge current. In this study, in order to confirm the feasibility of the above equivalent circuit model, we measured with a 6‐GHz wide‐band digital oscilloscope the discharge current through an SMA connector and the resultant magnetic near field for the contact discharge of an ESD gun. As a result, we found that both measured waveforms approximately agree with those calculated from our equivalent circuit model. We then measured with respect to charge voltages the magnetic near fields for the contact discharge of the ESD gun to the ground, which revealed that the measured waveform around the first peak is in fair agreement with the calculated one. Furthermore, we found that the magnetic field peak increases with increasing charge voltage, whose dependence can be predicted from our equivalent model. © 2005 Wiley Periodicals, Inc. Electr Eng Jpn, 153(1): 17–24, 2005; Published online in Wiley InterScience ( www.interscience.wiley.com ). DOI 10.1002/eej.20194     

优化模拟电流法计算超高压输电线路三维磁场

为了获得更准确的输电线路下方磁场的三维分布,使用智能优化算法对模拟电流法中模拟电流的个数与位置参数进行寻优,解决了普通模拟电流法中模拟电流的位置和个数只能依靠经验来确定的问题,从而提高计算精度.建立基于输电线路实际物理形状的三维计算模型,通过不同方法计算上海市松江区洞泾-泗泾500 kV线路的三维磁场分布.将计算结果与...     

基于等效半波注入法的小电流接地故障选线

我国中压配电网多数采用小电流接地运行方式,由于小电流接地系统单相接地故障电流很小并且容易受到外界条件的干扰等原因,故障选线难题多年未得到有效解决。通过对目前已有的故障选线方法进行分析,在原有的直流注入原理的基础上形成了等效半波注入法,通过比较各条线路的零序电流来选线。对等效半波注入法的选线定位理论进行了分析,主要包括确定了注入的半波直流信号的流通路径、形成了该方法的等值电路,并组建了对应的数学模型,在原理上验证了该理论的正确性。最后通过Matlab搭建模型验证该方法能够准确地实现故障选线。