连续逻辑DYL电路在测试系统中的应用

本文利用DYL多元逻辑电路的特点,提出求极值和中间值的“地址”的方法和电路。使DYL多元逻辑电路的应用更加完善。     

复合材料壳体磁场固化技术

环氧树脂基复合材料及缠绕壳体在磁场中缠绕和固化的技术为前苏联独有,美国只作了一些验证研究。这种技术使得复合材料加工过程中树脂基体发生物理和化学变化,固化后力学性能显著改善,而且质量更加稳定。实现该技术的设备已在前苏联应用。磁场中固化还适用于树脂涂层和粘接层。     

潜在电路分析中的拓扑模式图形生成算法研究

在电路网络树拓扑模式被识别出来的基础上 ,推导出网络树的基本拓扑模式图形生成算法 ,以便于分析设计人员使用拓扑模式图形的方式对电路系统进行具体的潜在电路分析     

电路特性仿真软件OrCAD／Pspice的应用

本文通过实例介绍了电路仿真特性软件OrCAD／Pspice在模拟电路、数字电路及数模混合电路几方面的应用。     

2000年行星际南向磁场事件及相关CME的若干分析

根据WIND飞船的观测资料，讨论了2000年发生的南向磁场（BS）事件，分析了它们的源，发现12次事件中11次的源是日冕物质抛射（CME）。运用从地球向太阳时间倒推的方法和LASCO，EIT195A的观测资料，确定了这些CME。它们都是快速CME，伴有行星际激波，都具有晕状（Halo)形态，它们在日面上发生的位置是在一个不对称的区域内。还分析了5个强南向磁场（BS≥20nT)事件，发现它们的CME源，或者具有很高的能量，或者抛射方向正对地球，或者是具有叠加效应的CME系列，分析表明，在我们所讨论的太阳活动高年，大的行星际扰动和强地磁暴与高速流的联系并不密切。     

1958年7月8日磁暴的电离层响应

本文用遍布全球的52个电离层垂测台站资料,研究1958年7月8日磁暴期间全球电离层扰动的发展变化;各扇区的响应特性;扰动的传播轨迹及速度等。获得以下结果:1.几大扇区的电离层扰动始于南北两极,美洲扇区除具这一特征外,其赤道地区在磁暴急始后不久,出现一个扰动中心,邻近区域的扰动受其控制。2.扰动由高纬向低纬发展,由扰动中心向外传播。3.扰动峰面几乎与地磁力线垂直,即扰动沿磁力线方向发展,其传播速度大约在150—600m/s范围。     

磁云—高速流相互作用的数值模拟

对１９７８年８月２７至２８日期间观测到的磁云与尾随高速流的相互作用进行数值模拟，基本拟合了１ＡＵ处的观测剖面。模拟结果表明，磁云－高速流系统将导致前向快，慢激波和后向快激波的形成。     

微带电路和天线的时域仿真

介绍了运用FDTD设计和分析微带电路和天线的基础理论,分析了误差产生的原因。利用FDTD法分别对微带传输线、矩形微带贴片天线和微带分支耦合器进行了仿真和特性分析。     

Eruptive prominences as sources of magnetic clouds in the solar wind

Large amounts of coronal material are propelled outward into interplanetary space by Coronal Mass Ejections (CMEs). Thus one might expect to find evidence for expanding flux ropes in the solar wind as well. To prove this assumption magnetic clouds were analyzed and correlated with H-observations of disappearing filaments. When clouds were found to be directly associated with a disappearing filament, the magnetic structure of the cloud was compared with that of the associated filament. Additionally the expansion of magnetic clouds was examined over a wide range of the heliosphere and compared with the expansion observed for erupting prominences.     

Observations of loops and prominences

We review recent observations by the Yohkoh-SXT in collaboration with other spacecraft and ground-based observatories of coronal loops and prominences. These new results point to problems that SoHO will be able to address. With a unique combination of rapid-cadence digital imaging (32 s full-disk and 2 s partial-frame images), high spatial resolution (2.5 arcsec pixels), high sensitivity (EM 10⁴² cm^–3), a low-scatter mirror, and large dynamic range, SXT can observe a vast range of targets on the Sun. Over the first 21 months of Yohkoh operations, SXT has taken over one million images of the corona and so is building up an invaluable long-term database on the large-scale corona and loop geometry. The most striking thing about the SXT images is the range of loop sizes and shapes. The active regions are a bright tangle of magnetic field lines, surrounded by a network of large-scale quiet-Sun loops stretching over distances in excess of 10⁵ km. The cross-section of most loops seems to be constant. Loops displaying significant increase in the ratio of the footpoint to loop-top diameter () are the exception, not the rule, implying the presence of widespread currents in the corona.All magnetic structures show changes. Time scales range from seconds to months. The question of how these structures are formed, become filled with hot plasma, and are maintained is still open. While we see the propagation of brightenings along the length of active-region loops and in X-ray jets with velocities of several hundred km/s, much higher velocities are seen in the quiet Sun. In XBP flares, for example, velocities of over 1000 km/s are common. Active-region loops seem to be in constant motion, moving slowly outward, carrying plasma with them. During flares, loops often produce localized brightenings at the base and later at the apex of the loop. Quiescent filaments and prominences have been observed regularly. Their coronal manifestation seems to be an extended arcade of loops overlying the filament. Reliable alignment of the ground-based data with the X-ray images make it possible to make a detailed intercomparison of the hot and cold plasma structures over extended periods. Hence we are able to follow the long-term evolution of these structures and see how they become destabilized and erupt.