航天器空间碎片被动防护技术

文章介绍了航天器磁力矩器在低轨道等离子体环境中的一些效应。以某型号卫星为例,计算了某型号磁力矩器产生的磁场,分析了等离子体在磁力矩器产生的磁场中的运动状态。经过建模计算,磁力矩器周围等离子体中的电子将在磁力矩器两端往复运动,而距离磁力矩器较远的电子将聚集在磁力矩器的两端附近。     

圆柱形霍尔推力器内等离子体数值模拟

利用一维磁流体动力学模型,对圆柱形霍尔推力器的放电等离子体进行了数值模拟。考虑了等离子体的电离、中和、碰撞、玻姆扩散及阳极鞘层的影响,由龙格-库塔方法得到离子速度、离子数密度、电子的温度等分布,其与实验结果有很好的一致性。经分析可知,此分布与电磁场的分布、粒子碰撞及电子阻抗等因素有关,并分析了电子温度分布、电子速度与电磁场的关系。结果表明,离子数密度沿通道方向增加,但在出口附近略有下降;而中性粒子数密度逐渐降低;离子速度在出口达到最大值,电子速度在下游有较大的梯度分布。     

电磁波与TVP相互作用

基于时变等离子体(TVP)的场方程,根据麦克斯韦方程,推导了TVP对入射电磁波的频率上移、时间衰减常数、反射系数,以及TVP的透射波和反射波电场幅值计算公式。通过实例计算分析了不同时间的新波频率、时间衰减常数和电场幅值。方法简单易行,可为TVP的应用提供一定的理论依据。     

脉冲等离子体推力器羽流预测计算研究

为了能够将脉冲等离子体推力器成功地运用于空间,需对其羽流进行研究。将一维 MHD双温放电模型的计算结果作为入口条件,运用DSMC（Direct Simulation Monte\|Carlo ）／PIC（Particle in Cell）流体混合算法一体化模拟实验室PPT羽流。验证计算显示该模 型具有一体化模拟脉冲等离子体推力器羽流的能力。对不同初始放电能量下的羽流场进行模 拟,给出了离子、中性粒子、电子温度、轴线上质量流率和出口平面返流质量流率的变化情 况。计算结果显示高放电能量下返流量更大,同时中性粒子在返流中所占比例也越大。
     

Numerical analysis of deflection control of a gas plasma jet based on magnetohydrodynamic staggered electrode configuration

To control the deflection of the gas plasma jet, a new analytical method is proposed based on the Magnetohydrodynamic(MHD) technique. Based on the typical MHD power generation model, the applied voltage is applied to the staggered electrodes, that is, a pair of electrodes on the same side wall are connected to generate an axial current in the channel. Under the action of the magnetic field perpendicular to the direction of the flow, the plasma is subjected to electromagnetic forces perpendicular...     

基于新型丝状电极等离子体激励器的前体涡控制

本文首次将新型丝状暴露电极DBD等离子激励器应用于大迎角下细长体非对称涡控制.丝状暴露电极的材料的选择对DBD推力以及推力效率至关重要,通过地面精细推力测量对丝状暴露电极等离子体激励器进行了优化,结果表明,本文研究材料中采用钨丝作为暴露电极,其推力效率最优;且随着电极直径从d=0.3 mm减小到d=0.08 mm,DB...     

Mathematical modeling of plasma drifts over equatorial low latitude regions

This paper presents a mathematical model to simulate ionospheric plasma drifts at equatorial low latitude regions by coupling of E- and F-regions. The governing non-linear differential equations (of elliptic and parabolic nature) are solved numerically through finite-difference schemes and obtained neutral winds and electric fields. The temperature and electron density profiles are generated utilizing MSIS-86 atmospheric model. The continuity equation is employed to obtain night-time E-region density profile using measured ionograms at Trivandrum (India). The computed vertical and zonal plasma drifts are comparable with measured Jacamarca plasma drifts with little variations during noon and evening times. The plasma drifts at Trivandrum (8.5° N, 76.5° E, dip 0.5° N) are compared with those of Jicamarca (12° S, 76.9° W, dip 2° N). Neutral wind simulations of present model agree well with those of horizontal wind model (HWM-93). The post-sunset enhancement and its reversal are also discussed.     

Interplanetary Physics Research in China:2006—2008

This brief report summarized the latest advances of the interplanetary physics research in China during the period of 2006—2007,made independently by Chinese space physicists and through international collaboration.The report covers all aspects of the interplanetary physics,including theoretical studies,numerical simulation and data analysis.     

关于氩等离子体热导率的测量

本文对《空气动力学学报》１９９７年第４期上发表的氩等离子体的热导率的实验研究结果的可靠性做了讨论。提出了一些提高实验数据可靠性的建议。     

Propagation of non-linear ion-sound pulses in dusty plasma waveguides

There are a lot of objects in space associated with dusty plasma inclusions. Such inclusions may bear a prolonged shape and behave as waveguides for ion-sound waves. In the case of space plasmas, the dust particles can possess both negative charge, due to electron attachment, and positive one, due to photoionization. In this paper the propagation of linear and non-linear ion-sound wave pulses in the dusty plasma waveguides, possessing positive charge, is studied. It has been demonstrated that non-linear dynamics of baseband pulse propagation in plasma waveguide possesses essentially non-solitonic behavior. Namely, propagation of a long ion-sound pulse leads to an excitation of a shock-like wave but not a stable localized nonlinear pulse. Also, when a Korteveg–de Vries (KdV) soliton is incident onto the dusty plasma waveguide, some part of the soliton energy is captured by the waveguide and transformed into a multi-pulse structure. Additionally, an interaction of dusty plasma inclusions with KdV soliton can lead to the occurrence of transverse instabilities of the soliton and its eventual destruction.