无碰撞低β磁流管中的非线性波

对无碰撞低β磁流管中柱对称状态下等离子体非线性静电波的存在进行了研究, 其结果表明: (1)若参数满足0<|(a/M2-1)E₀|<1, 存在着非线性周期波;(2)若|(a/M2-1)E₀|=1, 存在着隆起和下凹的孤立波, 也存在着激波;(3)若|(a/M2-1)E₀|>1, 存在着周期波, 也存在着隆起的孤立波。还对波的某些特性进行了研究。      

离子迴旋波的参量激发

本文分析了极光区上空以低混杂波作为泵波激发静电离子迴旋波的可能性,并计算了增长率。结果表明,当泵波较强时(峰值100mV/m)增长率可达0.5ω_ci,大于电流驱动不稳定性及离子束流不稳定性等线性理论所可能期待的增长率。从而在某些情况下,离子迥旋波的这种参量激发可能是主要的。      

磁层顶边界区剪切流MHD不稳定性的数值模拟研究 III.大振幅MHD波

本文用MHD二维不可压模式, 对Kelvin-Helmholtz不稳定性激发的非线性波动进行数值模拟.指出:K-H波动有两个吸引子:(1)定常吸引子;(2)周期吸引子.在Alfvén马赫数M_A>8时, 波动长时间发展渐近于定常态;在M_A<8时, 波动渐近于周期吸引子.在磁层顶K-H波动中, 一般M_A<8, 波动幅度呈周期变化形态, 即包络孤立子形态.本文还讨论了磁场-磁层顶K-H不稳定性中的作用, 指出:磁场可大大加强从磁鞘向磁层顶的动量输运.      

太阳风状态参数的变化对地球磁鞘中磁场起伏特性的影响

本文利用MHD激波跳跃条件的精确解,具体讨论了行星际背景太阳风状态参数Alfvén马赫数M₁、等离子体β₁参数和磁场角θ₁的变化对地球磁鞘区中磁场起伏特性及其分布的影响.主要结果是:马赫数M₁的变化主要控制磁场起伏特性:放大倍数、相对起伏和各向异性程度的水准高低.磁场角θ₁的变化控制磁场起伏的空间分布特性.等离子体β₁参数的变化,不引起磁场起伏特性的明显变化(对于实际经常发生的情况M₁ 8而言).M₁、θ₁是强控制参数,而β₁是弱控制参数;磁鞘区磁场起伏对太阳风状态参数的变化响应呈现明显的晨-昏不对称性(行星际磁场位于黄道面时),响应主要发生在晨侧.晨侧的磁场起伏(或湍动)相当活跃,而昏侧相当稳定;磁鞘中不同地点磁场起伏特性对太阳风状态参数M₁、β₁的变化响应有大致相同的形式,而对其磁场角度θ₁的变化却有迥然不同的形式.      

中等相对论性电子环-束引起的束迴旋不稳定性

本文研究了在电子等离子体频率ω_e远大于电子迴旋频率Ω_e的等离子体内,由中等相对论性电子环-束激发的高频(ω≥ω_e)束迴旋不稳定性。结果表明,高能电子束迴旋模在N2cos2θ<1和N2cos2θ>1范围内都是不稳定的,在N2cos2θ=1时是稳定的,这里N为折射指数,θ为传播角。当束迴旋模频率近乎等于冷背景等离子体本征模频率之一(ω≈ω_e)时增长率最大。文中介绍和讨论了色散方程的数值计算结果。      

太阳风中动力论Alfven波的湍流谱(a)朗道衰减

提出一个太阳风中Alfven脉动湍流的新模式,动力论Alfven波是Alfven波和离子声波非解耦的新波模。由太阳向外传播的各种波长的动力Alfven波的非线性相互作用推导出动力论Alfven脉动湍流功率谱P_k,在Alfven半径以外,P_k∝k-3/2,而在Alfven半径以内,由太阳附近的P_k∝k-1变化成P_k∝k-3/2动力论Alfven脉动在Alfven半径以内完成朗道衰减。新模式克服了以前理论模式遇到的困难。      

Electrodynamic Coupling in the Solar Wind-Magnetosphere-Ionosphere System

This paper presents a brief summary of our recent work based on global MHD simulations of the Solar wind-Magnetosphere-Ionosphere (SMI) system with emphasis on the electrodynamic coupling in the system. The main conclusions obtained are summarized as follows. (1) As a main dynamo of the SMI system, the bow shock contributes to both region 1 Field-Aligned Current (FAC) and cross-tail current. Under strong interplanetary driving conditions and moderate Alfven Mach numbers, the bow shock's contribution may exceed more than fifty percent of the total of either region 1 or cross-tail currents. (2) In terms of more than 100 simulation runs with due southward Interplanetary Magnetic Field (IMF), we have found a combined parameter f = E_swP_swM_A-1/2 (E_sw, P_sw, and M_A are the solar wind electric field, ram pressure, and Alfven Mach number, respectively): both the ionospheric transpolar potential and the magnetopause reconnection voltage vary linearly with f for small f, but saturate for large f. (3) The reconnection voltage is approximately fitted by sin3/2θ_IMF/2, where θ_IMF is the IMF clock angle. The ionospheric transpolar potential, the voltage along the polar cap boundary, and the electric fields along the merging line however defined they may be, respond differently to θ_IMF, so it is not justified to take them as substitutes for the reconnection voltage.      

电离层参数行为的相轨道表示及其新的预测模型

以不同时间尺度的电离层参数时间序列重构的相轨道,表征了该参数的复杂行为,并由此提出了参量预测的相空间相似及回归模型。两模型用于海口(20°2'N,102°20'E)f₀F₂和M(3000)F₂的预测,取得了满意的结果。      

极光场线上上行氧离子(O+)束驱动的静电离子迥旋波和离子声波不稳定性

本文研究了由背景热电子、背景冷质子(H+)和强各向异性氧离子(O+)束组成的模型等离子体中静电O+迴旋波和离子声波不稳定性.结果表明,低频(|ω|<σ_p,σ_p表示质子迴旋频率)静电O+迴旋波和离子声波可以由极光场线上上行O+束来激发.上行O+束可能是极光场线上低频静电不稳定性一个重要的自由能源.      

一种电离层垂直剖面物理模型及其与IRI-90模型的比较

在80-500km范围内考虑了3种中性成份的4种离子,从严格的电子和离子密度连续方程出发,对中性风和扩散效应进行了全面、连续的考虑,由此建立了一种电离层的物理模式;在此模式的基础上针对北京地区分别对太阳活动低年(F_10.7=60)、高年(F_10.7=300)的春(DOY=90)、夏(DOY=180)、秋(DOY=270)、冬(DOY=365)进行计算,并将所得结果与IRI-90进行了比较.结果表明: E层为典型的Chapman层: E-F谷区深度一般为0.2-0.5之间,比IRI要深;F₁缘在太阳活动低年的四季都出现,其中夏天最明显,已形成了一个F₁层,冬天最不明显,仅表现为一个轻微的凸缘,在太阳活动高年只有夏天出现了F₁凸缘,这与现有理论相符合,而IRI-90较少出现明显的F₁缘;F₂层的电子密度是活动高年比低年大,平均冬天比夏天大,这与观测结果也基本符合.      

Effect of q-nonextensive hot electrons on bifurcations of nonlinear and supernonlinear ion-acoustic periodic waves

Nonlinear and supernonlinear ion-acoustic periodic waves are investigated in a three-component unmagnetized plasma which consists of mobile fluid cold ions, Maxwellian cold electrons and q-nonextensive hot electrons employing phase plane analysis. Using the traveling wave transformation, the plasma system is reduced to a planar autonomous dynamical system. Utilizing phase plane analysis of planar dynamical systems, all possible phase portraits including nonlinear homoclinic orbit, nonlinear periodic orbit, supernonlinear homoclinic orbit and supernonlinear periodic orbit are presented depending on physical parameters $q,\alpha ,\sigma$ and V. Using numerical simulations, nonlinear and supernonlinear ion-acoustic periodic waves are shown for different conditions. It is found that the nonextensive parameter q plays a crucial role in the bifurcations of nonlinear and supernonlinear ion-acoustic periodic waves. Our study may be applicable to understand the nonlinear and supernonlinear periodic features in auroral plasma.     

关于冲击波在环形磁场中的传播

本文求解了点源爆炸波在环形磁场中传播的非自型问题。以耀斑引起的击波传播为例讨论了解的应用。从中可以看到,磁场扰动呈U形,主要发生在0.5Re—1.0Re的击波区域;行星际磁场的存在使击波到达1AU的时间延长了几个小时;击波必须具有大于磁截止能量E_M=λ₁S2/4π J₀R时(符号意义见内容)才有可能传播到1AU以远的地方,日冕磁场结构对耀斑击波进入行星际空间的传播有重要作用。      

Bifurcation analysis of ion-acoustic waves for Schrödinger equation in nonextensive Solar wind plasma

Bifurcation analysis of ion-acoustic wave (IAWs) solutions of the nonlinear Schrödinger equation (NLSE) is explored for the first time in an electron-ion (e-i) magnetized solar wind plasma. The existence of ion-acoustic (IA) periodic, superperiodic, kink, antikink, compressive and rarefactive solitary wave solutions are revealed. Special values of Solar wind plasma parameters at a normalized distance from the Sun are considered for numerical simulation. The IA wave solutions are derived analytically. These solutions are analyzed numerically considering the influence of parameters, namely, wave number (k), velocity (V) of traveling wave and nonextensive parameter (q). Computational simulation reveals that only IA periodic wave grows in amplitude as waves moves from the Sun.     

磁化等离子体中斜传播的离子孤波

近几年卫星空间电场测量经常证认出局地非线性离子静电波,它们可能与极光粒子加速有直接关系。这些静电波被认为或者是离子声波模的演化,或者是静电离子逥旋波模的演化结果。本文研究了磁场中斜传播小振幅离子非线性波的演化,得到非线性Schrodinger方程。结果表明离子声孤波和离子迴旋孤波都是可能的。计算结果与卫星S(3-3)电场测量比较,可以很好说明部分测量结果。      

Gas-dynamic approach to the theory of non-linear ion-acoustic waves in plasma with Kaniadakis’ distributed species

The non-linear theory of ion-acoustic waves in two-spesies isotropic collisionless plasma is developed. Both light electron and heavy ion species in the plasma are distributed with Kaniadakis’ statistics. Kaniadakis’ gas law is derived. The exact formula for the Sagdeev pseudopotential in parametric form is derived by the method based on the integration of the inverse function. The pseudopotential is analyzed. It is shown that periodic ion-acoustic waves and solitons are possible in the studied plasma. The differential equation describing the profile of the ion concentration in the wave is derived. The profiles of this concentration in the periodic ion-acoustic wave and soliton are calculated.