Whistler waves in plasmas with time-varying magnetic field: Laboratory investigation

Modulation of whistler waves in a plasma with time-dependant magnetic field perturbations was investigated experimentally. The experiments were performed on large “Krot” device, which was specially designed to study space plasma physics phenomena. It is shown that magnetic field variations on the wave propagation path can lead to splitting of initially continuous whistler wave into the sequence of bursts, whose repetition rate corresponds to magnetic field perturbation period. The frequency inside each burst is changing from its front edge to the back edge. Relative shift of the wave frequency can be as large as the relative magnetic disturbance. Distortion of whistler wave frequency spectrum after its passing through magnetically disturbed areas can be used as a diagnostics for low-frequency magnetic field variations. The applicability of our laboratory results to space plasma is discussed.     

A question raised from the observation of dynamic cusp formation: When and where does particle acceleration occur?

We present observations of a C9.4 flare on 2002 June 2 in EUV (TRACE) and X-rays (RHESSI). The multiwavelength data reveal: (1) the involvement of a quadrupole magnetic configuration; (2) loop expansion and ribbon motion in the pre-impulsive phase; (3) gradual formation of a new compact loop with a long cusp at the top during the impulsive phase of the flare; (4) appearance of a large, twisted loop above the cusp expanding outward immediately after the hard X-ray peak; and (5) X-ray emission observed only from the new compact loop and the cusp. In particular, the gradual formation of an EUV cusp feature is very clear. The observations also reveal the timing of the cusp formation and particle acceleration: most of the impulsive hard X-rays (>25 keV) were emitted before the cusp was seen. This suggests that fast reconnection occurred during the restructuring of the magnetic configuration, resulting in more efficient particle acceleration, while the reconnection slowed after the cusp was completely formed and the magnetic geometry was stabilized. This observation is consistent with the observations obtained with Yohkoh/Soft X-ray Telescope (SXT) that soft X-ray cusp structures only appear after the major impulsive energy release in solar flares. These observations have important implications for the modeling of magnetic reconnection and particle acceleration.     

小型磁悬浮CMG高速转子动框架效应前馈补偿与实验

磁悬浮控制力矩陀螺是航天器快速姿态控制与快速机动的新型空间执行机构。由于动框架效应,框架转动输出力矩反作用于飞轮转子,会导致磁轴承的径向载荷和控制电流发生改变。为抑制动框架效应对磁浮转子的影响,在分析力矩输出时高速磁浮转子受力特性的基础上,采用角速率前馈控制策略实现对动框架效应引发的力矩扰动的有效抑制,并在所研制的75Nms立式小型磁悬浮控制力矩陀螺上进行了整机输出特性测试。试验结果表明：该方法能在保证磁浮转子高速稳定的前提下有效抑制动框架效应,满足整机力矩输出的要求。     

X波段波导端头裂缝的数值分析

用矩量法(MOM)导出求解X波段波导端头裂缝口面等效磁流的公式。在此基础上,计算波导不同频率下的反射系数和驻波系数等参数。给出了BJ-100波导端头裂缝口参数的计算结果,据此讨论了裂缝长度、宽度、厚度与谐振频率的关系。另外检验了圆头与方头裂缝的等效性,并给出了波导端头裂缝谐振频率的近似设计公式。分析结果表明,该算法简单,计算结果与测试值吻合较好。     

磁悬浮柔性转子系统变学习速率单神经元PID控制

磁悬浮轴承柔性转子系统的转速范围较大,固定的控制参数很难同时保证系统所需的低频和高频特性。本文在一般单神经元PID控制的基础上,将转速信号引入磁悬浮轴承数字控制器,在不同转速段选择不同的学习速率以调节控制参数得到合适的磁悬浮轴承的刚度和阻尼。试验结果表明,变学习速率单神经元自适应PID控制能够明显减小转子在各阶临界转速时的振幅,有助于磁悬浮轴承柔性转子系统的安全稳定运行。     

电磁轴承支承的柔性转子在轴承失效后坠落过程中的瞬态响应

研究了主动电磁轴承支承的单盘柔性转子系统在磁轴承失效后转子坠落在带有固定间隙的滚动型备用轴承上的瞬态响应,分析了备用轴承的各种参数对瞬态响应的影响。结果发现系统出现了以自由落体-碰撞弹起-自由落体为特征的在间隙圆底部的摆动运动、以碰撞弹起-加速落体-碰撞弹起为特征的在整个间隙圆范围的碰撞型回转运动以及轴颈与备用轴承始终接触在一起的摩擦型回转运动等3种运动形式。碰撞型回转运动实际上是由碰撞过程中部分周向的摩碰引起,而摩擦型回转运动是由轴颈与备用轴承之间的全周干摩擦所致。碰撞型回转运动和反向摩擦型回转运动对备用轴承的影响最为严重。     

磁射流抛光中磁场的分析与设计

介绍了一种新型抛光技术——磁射流抛光中磁场对磁流变液粘度的影响,设计了相适应的磁场形式,重点分析了铁磁喷嘴头部形状对磁场的影响,并通过ANSYS有限元软件仿真了结构形状对磁场空间特性的影响。     

磁探仪应召搜潜建模与仿真

依据经典的磁探仪应召搜潜方法,以某型反潜巡逻机为背景,建立了反潜巡逻机利用磁探仪执行平行航线、扩展矩形和螺旋形搜潜模型.对3种方法的搜潜概率进行分析,仿真了相同潜艇运动模型条件下,潜艇初始位置散布、初始距离、潜艇经济航速和海洋环境磁噪声对搜潜概率的影响.实验结果表明:相同条件下,螺旋形搜潜效能最高;潜艇只进行航速机动时...     

核磁共振陀螺信号仿真及噪声分析

核磁共振陀螺具有体积小、精度高、功耗低等优势,有望成为下一代惯性导航系统的核心部件,目前正受到人们的广泛关注。比较全面的介绍了核磁共振陀螺的基本理论,在此基础上利用时间离散化方法推导并建立了能够充分考虑核磁共振陀螺系统动态特性的仿真模型。利用该模型研究分析了锁相环相位、磁场、温度以及探测光强在1×10-5均方根幅度下均匀白噪声对陀螺信号的影响,发现它们对角随机游走、零偏不稳定性影响依次减小,且都具有自身独特的频率响应特性。其中,锁相环相位噪声引起的角随机游走与零偏不稳定性分别为5.1985×102(°)/h1/2、3.4593×103(°)/h,而探测光强噪声引起的角随机游走与零偏不稳定性分别为3.1623×10-1(°)/h1/2、4.7603×10-1(°)/h。该研究对深入分析核磁共振陀螺动力学机理、寻找主要噪声来源、提高陀螺性能具有重要意义。     

1978—1988年间磁扰的分析与日地耦合

用1978-1988年间行星际磁场(IMF)的B_z分量、极光区AL指数和赤道附近地磁台Z分量等资料探讨了日地耦合中的主要物理过程。B_z的11年变化大致与太阳活动程度相当,但AL和赤道附近ΔZ更多地受磁层和电离层内部过程所控制。分析中强调了对国际磁抗日按物理过程进行分类的必要性。