根据线性迭加理论实现微小卫星姿态磁控制

根据地磁力矩定向阻尼特性和线性迭加理论,提出仅用磁力矩器实现对地指向微小卫星三轴姿态稳定的控制律。推导了采用迭加补偿,并考虑附加磁矩影响时改进的卫星姿态动力学方程。理论分析和仿真结果表明,该控制律简单、姿态控制精度高。     

GAP贫氧推进剂的常压热分解特性研究

采用DSC方法研究了GAP模拟贫氧推进剂的常压热分解特性．同时考察了TMO催化荆对GAP模拟贫氧推进剂热分解特性的影响。实验结果表明，TMO催化剂对GAP、AP和KP的催化作用不同，复配催化荆可能是GAP贫氧推进荆系统中催化效果较好的催化剂。     

TMO对铝镁贫氧推进剂低压燃烧性能影响

研究了过渡金属氧化物（TMO）及其复配物对非壅塞固体火箭冲压发动机铝镁贫氧推进剂燃烧特性的影响。研究发现，氧化铁对提高铝镁贫氧推进剂燃速的作用显著。过渡金属氧化物组合（氧化钴／氧化铬和氧化铜／氧化铬）对提高铝镁贫氧推进剂的燃速催化作用显著，且含组合催化剂（氧化钴／氧化铬、氧化铜／氧化铬和氧化铁／氧化铜）的盆氧推进剂具有高的燃速压强指数。     

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。     

非晶态(Fe_(0.5)Ni_(0.5))_(80-x)Cr_xP_(14)B_6合金薄带的磁场敏感特性的研究

本文对非晶态(Fe_(0.5)Ni_(0.5))_(80-x)Cr_xP_(14)B_6(x=0,1,2,3,4,6,10)合金薄带样品的室温直流磁场敏感特性进行了测量。结果表明,在几十个A/m范围的外磁场内,样品具有开关型磁场敏感特性。对影响开关特性的三个因素进行了一些讨论。     

LAS词法及语法分析器自动生成工具

LAS是在VAX/VMS操作系统上用Ada语言开发的词法分析器和语法分析器的自动生成工具。词法分析器由词法执行程序和LAS根据词法规则说明文件生成的词法树组成,语法分析器由语法执行程序和LAS根据语法规则说明BNF范式生成的状态序列集组成,在BNF范式中插入语义标志,就可以在语法分析器分析到该语义标志时,使控制转入用户提供的语义处理程序。     

磁壳参数L与磁暴Dst指数和行星际条件的关系

用磁坐标L-/A来描述地球近地空间粒子特性和卫星位置是近年来空间物理探测研究和数据分析中的一个新趋势.利用T96磁场模型计算了L值,并比较了在地球磁层剧烈活动期间和不同行星际条件下,用偶极子模型,国际参照磁场(IGRF)模型,和T96磁场模型这三种方式计算得到的地球表面L-A磁坐标之间的区别.在地磁纬度大于30°时偶极子近似和IGRF磁场模型计算得到的L值差别开始增大.在地磁纬度大于50°时,用IGRF磁场模型和T96磁场模型计算得到的L值差别开始增大.由于T96磁场模型引入了行星际磁场南北和东西分量,计算的L值包含了行星际条件的影响,并具有了随地方时变化的特性.本工作对于辐射带粒子动态模式的建立,以及正确理解卫星磁坐标位置等具有重要意义.     

关于IMF北向分量特强时的太阳风－磁层－电离层耦合

关于ＩＭＦ北向分量特强时的太阳风－磁层－电离层耦合沈长寿，资民筠（北京大学地球物理系，１００８７１）（中国艺术研究院，北京）关键词行星际磁场，太阳风－磁层能量耦合函数为检验Ａｋａｓｏｆｕ提出的能量融合函数“’在ＢＺ强北向时能否反映太阳风与磁层扰动间的...     

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.