RCD箝位正激变换器的分析研究

正激变换器因电路简单而广泛应用于中小功率变换场合。但是它的一个固有缺陷是功率晶体管截止期间变压器必须磁复位，因而需要采用附加的复位电路。本文详细介绍了ＲＣＤ箝位正激变换器的工作原理，给出了ＲＣＤ箝位网络的设计准则和步骤。实验结果证实了理论分析的正确性。     

磁悬挂天平的数字控制技术(磁悬挂天平技术研究之三)

本文研究磁悬挂天平的数字控制技术。在 φ60mm 单分力天平装置上,配置了以8031单片计算机为核心的控制系统,不仅实现了飞行器模型的稳定悬挂,而且在外力作用下模型悬挂点保持不变。反馈控制律的设计分三步进行:首先对电磁铁特性进行补偿,使其阶次降低,简化后续的设计工作;然后采用比例微分控制达到系统的稳定最后在系统稳定的基础上,设计了位置积分环节,使系统在常值外力作用吋,能实现模型的悬挂点不发生偏离。这种三段设计法在实验调试时具有实用意义。文中具体介绍了控制系统的实现技术,包括 PWM 功率放大器,单片机硬件和软件。     

用假想磁荷模型计算三维静磁场的解耦问题

本文提出了用假想磁荷模型计算三维静磁场的解耦概念和实施方法,较好地解决了假想磁荷模型中的磁位跃变边界问题。通过实例计算,证明了该概念和方法的正确性。     

ENTROPY CHARACTERISTICS OF MAGNETIC REFRIGERANTS

ＥＮＴＲＯＰＹＣＨＡＲＡＣＴＥＲＩＳＴＩＣＳＯＦＭＡＧＮＥＴＩＣＲＥＦＲＩＧＥＲＡＮＴＳ￥ＹｏｕＬｉｘｉｎ；ＧｕｏＸｉａｎｍｉｎｇ；ＸｕＳｈｅｆａ（ＤｅｎａｒｔｍｅｎｔｏｆＡｉｒｃｒａｆｔＥｎｇｉｎｅｅｒｉｎｇ．ＮＵＡＡ，２９ＹｕｄａｏＳｔｒｅｅｔ．...     

磁悬挂天平系统的磁场分析与计算(60mm×60mm 磁悬挂天平技术研究之一)

磁悬挂天平系统的磁场设计好坏是磁悬挂天平系统结构设计成败的关键。而磁悬挂天平系统的磁场结构比较复杂,用简单的磁路设计方法已经不能满足更高的设计要求。本文介绍了一种求解电磁场的方法——二维电磁场有限元法,建立了相应的磁悬挂天平系统的数学模型,并应用此法,对磁悬挂天平的均匀磁场和梯度磁场分布进行了分析计算;提出了一种用于求解磁场开域问题的方法。文章中还介绍了根据磁场的计算结果来确定线圈间间距和铁芯厚度的方法。在此基础上,提出了一个60mm×60mm 的磁悬挂天平系统的设计方案,并给出了此设计方案的理论计算与实验结果的对比表。     

矩形栅格波导阵列单元的阵中特性

根据等效原理,用矩量法(MOM)导出求解仅激励中心单元条件下矩形栅格开口波导阵列各单元口面等效磁流的模型,在此基础上给出了激励单元的内部场、耦合场、反射系数、驻波系数,激励波导与阵中其他波导的耦合系数,以及远区场等阵中特性的计算公式。在不同工作频率下计算了一7单元×7单元开口波导矩形栅格阵中激励单元的等效磁流和阵中方向图,以及激励单元与阵中其他单元的耦合系数。研究表明:互耦对单元的阵中特性影响明显,阵中驻波系数明显大于孤立单元,单元间的耦合随工作频率增大而减弱。     

日冕膨胀和太阳角动量向行星际空间的转移

本文讨论了日冕膨胀中的角动量问题。利用大量I型彗尾资料的计算,证实了日冕膨胀中方位分量的存在;它不仅是随机量,而是具有大小为9.8km/s的定常量。太阳演化到主序星阶段以来,由于日冕膨胀丢失了80％的角动量,太阳自转角速度正以指数律下降。因此,这将对太阳动力演化起到很大的影响。     

Coupling of the interstellar and interplanetary magnetic fields at the heliospheric interface: The effect of neutral hydrogen atoms

We present numerical results showing the effect of neutral hydrogen atoms on the solar wind (SW) interaction with the local interstellar medium (LISM), where the interstellar magnetic field (ISMF) is coupled to the interplanetary magnetic field (IMF) at the surface of the heliopause. The IMF on the inner boundary surrounding the Sun is specified in the form of a Parker spiral and self-consistently develops in accordance with the SW motion inside the heliopause. The model of the SW–LISM interaction involves both plasma and neutral components which are treated as fluids. The configuration is chosen where the ISMF is orthogonal to the LISM velocity and tilted 60° to the ecliptic plane. This orientation of the magnetic field is a possible explanation of the 2–3 kHz emission data which is believed to originate ahead of the heliopause. It is shown that the topology of the heliospheric current sheet is substantially affected by the ISMF. The interaction pattern dependence on the neutral hydrogen density is analyzed.     

What is the role of magnetic null points in large flares?

We have performed the analysis of the magnetic topology of active region NOAA 10486 before two large flares occurring on October 26 and 28, 2003. The 3D extrapolation of the photospheric magnetic field shows the existence of magnetic null points when using two different methods. We use TRACE 1600 Å and 195 Å brightenings as tracers of the energy release due to magnetic reconnections. We conclude on the three following points:

1. The small events observed before the flares are related to low lying null points. They are long lasting and associated with low energy release. They are not triggering the large flares.

2. On October 26, a high altitude null point is found. We look for bright patches that could correspond to the signatures of coronal reconnection at the null point in TRACE 1600 Å images. However, such bright patches are not observed before the main flare, they are only observed after it.

3. On October 28, four ribbons are observed in TRACE images before the X17 flare. We interpret them as due to a magnetic breakout reconnection in a quadrupolar configuration. There is no magnetic null point related to these four ribbons, and this reconnection rather occurs at quasi-separatrix layers (QSLs).

We conclude that the existence of a null point in the corona is neither a sufficient nor a necessary condition to give rise to large flares.     

Influence of Fast Global Variations of Solar Magnetic Fields on Space Weather in Cycle 23

It is established that the large-scale and global magnetic fields in the Sun's atmosphere do not change smoothly, and long-lasting periods of gradual variations are superseded by fast structural changes of the global magnetic field. Periods of fast global changes on the Sun are accompanied by anomalous manifestations in the interplanetary space and in the geomagnetic field. There is a regular recurrence of these periods in each cycle of solar activity, and the periods are characterized by enhanced flaring activity that reflects fast changes in magnetic structures. Is demonstrated, that the fast changes have essential influencing on a condition of space weather, as most strong geophysical disturbances are connected to sporadic phenomena on the Sun. An explanation has been offered for the origin of anomalous geomagnetic disturbances that are unidentifiable in traditionally used solar activity indices. Is shown, main physical mechanism that leads to fast variations of the magnetic fields in the Sun's atmosphere is the reconnection process.