太阳风中航天器带电与尾迹效应的模拟

航天器充电和尾迹效应会对周围等离子体造成扰动,影响测量装置结果的准确性.利用SPIS （Spacecraft Plasma Interaction Software）分别模拟了航天器与太阳风的相互作用,考察了光电效应以及航天器尺度对表面充电情况和尾迹效应的影响.结果表明:太阳风环境下,等离子体密度稀薄,电子电流比光电子电流小得多,航天器表面为正电势,航天器后部有清晰的尾迹结构,尾迹带负电;光电效应可改变尾迹结构,与无光电效应相比,光电效应使得航天器尾迹尺度变大;由于太阳风定向运动动能大于航天器表面势能,航天器的尾迹结构与其几何尺寸有关,航天器尺寸越大,尾迹尺度越大.      

等离子体鞘层效应对磁层探测电场仪设计的影响

在空间环境探测中，卫星与等离子体的相互作用会改变背景环境的粒子和电位的分布，从而影响探测器对空间电场的测量.为了给磁层卫星电场探测仪器的研制和设计提供参考，本文以中国未来的磁层电离层探测为背景，针对不同轨道高度的等离子体环境，利用SPIS（Spacecraft Plasma Interaction Software）模拟了卫星平台和探针与等离子体的相互作用，从而得到了不同环境下卫星周围等离子体鞘层的厚度，以及探针电位与电流的对应关系.模拟结果表明:由于光电子和二次电子的影响，卫星鞘层的厚度小于等离子体的德拜半径，且温度越高其偏差越大；模拟得到的探针表面电流与电位的关系表明，施加偏置电流的探针可明显提高对电流扰动的抗干扰能力.此外，估计了不同轨道高度上探针处于最佳工作点时应施加偏置电流的大小.      

一种航天器太阳电池阵供电能力计算方法

太阳电池阵为航天器提供能源,在型号研制和在轨运营过程中需对其供电能力进行计算,为此提出了一种航天器太阳电池阵供电能力的计算方法。首先,利用太阳电池片的地面测试数据得到标准测试条件(STC)下的电池片伏安模型,并利用电池片在轨等效光强和温度修正电池片伏安模型的光生电流、串联电阻和并联电阻等参数,得到电池片在轨伏安模型,然后,根据基尔霍夫定律推导出电池阵中电池片工作电压、电流以及旁路二极管和隔离二极管的输出情况,从而得到太阳电池阵的伏安模型。仿真结果表明,本文方法可以精确计算航天器在任意光强、温度和遮挡下的太阳电池阵伏安模型,可以精确分析旁路二极管和隔离二极管对太阳电池阵供电能力的影响,较已有方法计算精度提高20%。     

高速撞击梯度电势靶板产生等离子体诱发的放电

针对在轨运行航天器在空间等离子体环境和空间带电粒子活动下诱发航天器表面梯度电势存在的客观现实,航天器在空间碎片的撞击下会诱发表面带电或深层电介质带电的航天器放电。为了在实验室模拟航天器表面存在电势差的真实情况,采用对航天器外表面分割的方法,在分割的表面间预留不同间距且在2靶板间加装电阻的方法创造具有梯度电势的高电势2A12铝板作为靶板。利用自行构建的梯度电势靶板的充放电测试系统、超高速相机采集系统和二级轻气炮加载系统,开展高速撞击梯度电势2A12铝靶的实验室实验。实验中,弹丸以入射角度为60°（弹道与靶板平面的夹角）、撞击速度约为3 km/s的条件撞击间距分别为2、3、4和5 mm的2A12铝高电势靶板,利用电流探针和电压探针采集放电电流和放电电压。实验结果表明:放电产生的等离子体形成了高电势与低电势靶板间的放电通道,且在梯度电势靶板间距分别为2、3 mm时诱发了一次放电,放电电流随高低电势靶板间间距的增加而减小;在梯度电势靶板间距分别为4、5 mm时诱发了二次放电,放电电流随高低电势靶板间间距的增加变化不明显。      

The plasma sheet and boundary layers under northward IMF: A multi-point and multi-instrument perspective

During conditions of northward interplanetary magnetic field (IMF), the near-tail plasma sheet is known to become denser and cooler, and is described as the cold-dense plasma sheet (CDPS). While its source is likely the solar wind, the prominent penetration mechanisms are less clear. The two main candidates are solar wind direct capture via double high-latitude reconnection on the dayside and Kelvin–Helmholtz/diffusive processes at the flank magnetopause. This paper presents a case study on the formation of the CDPS utilizing a wide variety of space- and ground-based observations, but primarily from the Double Star and Polar spacecraft on December 5th, 2004. The pertinent observations can be summarized as follows: TC-1 observes quasi-periodic (∼2 min period) cold-dense boundary layer (compared to a hot-tenuous plasma sheet) signatures interspersed with magnetosheath plasma at the dusk flank magnetopause near the dawn-dusk terminator. Analysis of this region suggests the boundary to be Kelvin–Helmholtz unstable and that plasma transport is ongoing across the boundary. At the same time, IMAGE spacecraft and ground based SuperDARN measurements provide evidence of high-latitude reconnection in both hemispheres. The Polar spacecraft, located in the southern hemisphere afternoon sector, sunward of TC-1, observes a persistent boundary layer with no obvious signature of boundary waves. The plasma is of a similar appearance to that observed by TC-1 inside the boundary layer further down the dusk flank, and by TC-2 in the near-Earth magnetotail. We present comparisons of electron phase space distributions between the spacecraft. Although the dayside boundary layer at Polar is most likely formed via double high-altitude reconnection, and is somewhat comparable to the flank boundary layer at Double Star, some differences argue in favour of additional transport that augment solar wind plasma entry into the tail regions.     

Laboratory experiments on spacecraft charging and its neutralization

Simulation experiments on spacecraft charging in space plasma and its neutralization are performed in relation to the electron beam experiment (SEPAC) on Space Shuttle Spacelab 1. A spacecraft simulator or a spherical probe is immersed in a magnetized plasma and a positive high voltage with respect to the plasma is externally applied to it. The current-voltage characteristics follow quite well with the theoretical model of Parker and Murphy [1] in the low voltage, low pressure region. When the voltage rises to more than the ionization potential of the surrounding neutral gas, it departs from the model and the effect of plasma production by the electron current becomes very important. The same kind of ionization effect as this has also been observed in our rocket experiments with an electron beam. The enhancement of the ionization effect by an additional neutral gas injection causes a considerable suppression of the potential rise of a spacecraft emitting an electron beam. This is demonstrated with the SEPAC accelerators in a large space chamber experiment.     

空间等离子体引起的高电压太阳阵之弧光放电

简单介绍了空间等离子体引起的高电压太阳阵（ＨＶＳＡ）之弧光放电的研究现状。利用已有的一些实验数据及Ｈａｓｔｉｎｇｓ的扩展理论进行了应用ＨＶＳＡ计算，得出了飞弧概率随工作电压增加而增大，随空间环境等离子体流增高而增大的合理结果。     

Symmetric model of spacecraft charging and plasma emission effects

The electrostatic charging of satellites in space and the interactions with the plasma in the near surroundings are investigated by making use of symmetric models. In this case, the Vlasov-Poisson system describing the ambient plasma disturbances and the plasma emitted from the surface can be integrated self-consistently within a numerical iteration scheme, and the current balance yields the floating potential of the probe. The spacecraft charging and the potentials in its surroundings are investigated for the following plasma and emission conditions: (1) in the ionosphere in the case of very negative surface potentials, (2) in the solar wind with regard to the HELIOS mission and (3) in the near vicinity of the comet Halley, where a very strong plasma emission due to the impact of neutral gases onto the surface must be regarded. Finally, the importance of the shielding due to the ambient plasma is discussed.     

ICMEs Likely From the Same Active Region Observed by Both Helios 1 and IMP 8

The chance of an Interplanetary Coronal Mass Ejection (ICME) observed by widely-separated spacecraft is rare. However, such an event provides us a good opportunity to study the propagation and evolution of ICMEs in the heliosphere. On day 72 of 1975, an ICME was observed by Helios 1 at 0.3 AU, while a similar solar wind structure was observed by IMP 8 at Earth on day 70 of 1975. On the basis of comparison of the plasma signatures and the transit time from Helios 1 to IMP 8, we hypothesize the observed ICMEs by both spacecraft are resulted from the same active region on the solar surface. A one-dimensional MHD model was used to track the ICME from Helios 1 (0.3 AU) to Earth. The observed plasma profiles and timing are close to those predicted by our MHD model and thus, give the supports to the model.      

基于BP神经网络的GEO等离子体环境参数反演分析

空间等离子体环境诱发的表面充电效应会对航天器运行产生干扰，严重时将导致太阳电池等部件失效。通过神经网络反演方法，以GEO环境中介质表面充电电位曲线作为输入，在双峰麦克斯韦分布假设下，可以逆向得到高能峰的等离子体参数。分析了GEO等离子体环境参数对表面充电电位曲线的影响，表明高能峰在充电过程中起决定性作用；其次通过MATLAB搭建BP神经网络，采用COMSOL计算得到多组充电曲线进行网络训练和反演计算，得到等离子体密度反演的平均相对误差为0.42%，温度反演的平均相对误差为0.03%，整体误差在0.1%～5.6%。结果表明，采用神经网络对等离子体环境进行反演具有可行性，该方法可以作为空间等离子体环境探测结果的对比参考和航天器非探测点表面电位计算的输入条件。     

空间太阳电池板银互连片原子氧效应模拟试验

空间太阳电池板可作为空间飞行器的动力源,但由于原子氧在空间太阳电池板银互连片上的腐蚀作用,可能影响空间太阳电池板的有效寿命.因此,在北航流体所设计的原子氧效应地面模拟试验设备中,对空间太阳电池板的银互连片进行了抗原子氧效应地面模拟试验研究.获得了银箔和不同防护镀层材料在原子氧环境中的不同剥蚀结果,这为进行银互连片表面的原子氧防护提供了必要的应用和设计依据.     

小行星远距离抵近轨道

讨论了小行星引力一阶项可被忽略情况下的小行星远距离轨道设计及动力学。此时,航天器的运动受太阳引力和太阳光压的影响。航天器和小行星的加速度之差在这两者之间形成的独特的相对动力学,为航天器在小行星附近停驻与观测提供特定轨道。完整解决了小行星处于圆形日心轨道这一较简单情况,也考虑和阐述了椭圆轨道情况,并取得了一些初步结果。     

航天用太阳电池地面标定测试装置研究

传统的标准太阳电池标定方法分为高空标定与地面标定,地面标定方法已纳入国际标准。地面标定由于操作简便、标定结果较为精准目前被广泛应用。太阳电池标定结果准确与否对航天器电源系统姿态敏感期、地面环境模拟的设计具有重要意义。本文对太阳电池地面标定方法展开研究,根据国家标准中地面标定方法原理研制了便携式、高准确度的地面标定测试设备,包括准直孔、太阳电池托盘、太阳跟踪器等标定装置,使地面标定过程简易化,对航天用太阳电池地面标定有着重要意义。     

Energetic ion emission for active spacecraft control

Future space missions aiming at the accurate measurement of cold plasmas and DC to very low frequency electric fields will require that the potential of their conductive surfaces be actively controlled to be near the ambient plasma potential. In the near-Earth space these spacecraft are usually solar-cell powered; consequently, parts of their surface are most of the time exposed to solar photons. Outside the plasmasphere, a positive surface potential due the dominance of surface-emitted photoelectrons over ambient plasma electrons is to be expected. Photo- and ambient electrons largely determine the potential and positive values between a few Volts up to 100 V have been observed. Active ion emission is the obvious solution of this problem. A liquid metal ion emitter and a saddle field ion emitter are nearing the stage of flight unit fabrication. We will attempt to clamp the spacecraft potential to values close to the plasma potential. We present first results from vacuum chamber tests and describe the emission behaviour and characteristics of emitters producing, respectively, In⁺ and N₂⁺ beams with an energy of ≥ 5 keV.     

Kevlar BF—2及GD414材料充电性能研究

Kevlar作为最新型的航天结构材料,BF-2作为太阳电池盖片玻璃,GD414作为航天器材料粘接剂,都是空间技术必不可少的重要而基本的材料。因而它们在空间电环境条件中的表面电荷积累性质受到极大注意。该文就此三种材料在综合模拟空间环境条件下,进行了材料表面电导和环境诱发电导的实验研究,并给出了实验结果的分析。     

Particle-in-cell simulation of the plasma environment of a spacecraft in the solar wind

The main interactions between the plasma and the spacecraft are the wake effects, the emission of a dense photoelectron cloud and the electric charging of the surface of the spacecraft. An electrostatic particle-in-cell computer simulation model is presented, that allows the simultaneous calculation of these related effects. For different plasma properties, two-dimensional simulations yielded the steady state self-consistent potential distributions around the probe. These potentials, especially the potential barriers produced by the photoelectron cloud, have great influence on the measurements of the low energy solar wind electrons. The essential features can be verified by a comparison with selected electron distributions measured onboard the HELIOS spacecraft.     

低轨道航天器的表面充电模拟

为研究航天器表面材料在空间环境中的充电现象, 利用SPIS (Spacecraft Plasma Interaction System)模拟了航天器在低轨道等离子体环境中的表面充电情况, 通过对模拟结果进行分析并与实际观测进行比较, 可以看出模拟结果基本能够反映出不同性质材料之间的充电差别, 特别是导电材料与非导电材料之间的充电差别. 模拟得到的充电电位及充电时间与充电的一般理论计算结果符合较好, 且能够清晰反映出航天器运动中产生的冲击流及尾流的结构特征. 根据SPIS低轨道航天器表面充电模拟的特点, 认为SPIS的模拟结果是合理的.      

利用孤立导体建立等离子体探测载荷参考电位方法

研究讨论了一种利用孤立导体在空间等离子体环境中建立探测器参考电位的技术.将一个金属导体与航天器进行电隔离，利用电路将孤立导体电位引入探测器电源模块，为探测器建立参考电位.该技术可安全方便地应用于卫星等航天器，使探测器的地电位与空间等离子体电位基本一致，避免航天器本体电位对探测器的影响.该技术将应用于中国空间站等离子体原位探测器，通过测试验证了该技术方法可以建立-210～+210V的参考电位，满足空间站等离子体原位探测器-200～+200V的参考电位技术需求.      

低轨道航天器高电压太阳电池阵电流泄漏效应分析计算

在一种简化的太阳电池阵结构模型基础上, 利用太阳电池阵电流收集经验模式,基于电流平衡, 建立了一种计算低轨道航天器高电压太阳电池阵在等离子体环境中电流泄漏的方法. 利用该方法, 对高电压太阳电池阵电流泄漏效应与低轨道等离子体环境、电池阵电压、电池阵裸露金属面积的关系进行了分析计算.结果表明, 随着轨道高度增加, 电流泄漏引起的电池阵功率损失迅速下降, 影响最严重的区域为电离层等离子体密度最高的300～400 km高度的轨道区域; 电流泄漏引起的功率损失与太阳电池阵电压呈指数关系, 电压越高功率损失越大; 200 V以下的电池阵功率损耗较小, 远低于电源系统总功率的1%;电流泄漏与太阳电池阵裸露金属导体的表面积呈正比关系, 因此, 通过减少太阳电池阵裸露面积, 可以降低电流泄漏的影响.      

太阳帆板驱动机构的表面充放电效应研究

空间等离子体环境效应导致的卫星表面充放电是造成卫星在轨工作异常及故障的重要原因之一. 太阳帆板驱动机构（Solar Array Drive Assembly,SADA）是长寿命、大功率卫星电传输环节的关键部件,易成为充放电效应的对象,可使卫星丧失能源,导致整星失效. 为验证空间等离子体环境导致的表面充放电对SADA特别是其功率传输可靠性和安全性的影响,利用等离子体环境模拟试验装置,模拟地球同步轨道（Geostationary Orbit,GEO）等离子体环境,针对SADA进行试验研究. 结果表明,使用两种不同绝缘材料的SADA在空间等离子体模拟环境下表现没有明显区别,表面充放电未对设计合理的SADA正常工作造成明显影响. 研究结果对未来GEO轨道SADA等空间机构的可靠性和安全性设计具有一定指导意义.