共查询到20条相似文献，搜索用时 93 毫秒
1.
为降低氢脉泽由C场不均匀导致的跃迁频率相对变化率,提出了三段螺线管和四组线圈两种C场组件设计方式。利用轴线上磁场的高阶展式计算了L=0.05～0.5的三段螺线管构造匀强磁场时的安匝比以及螺线管间距,并选择L=0.2～0.45的三段螺线管进行了磁场的有限元分析,给出了不同宽度的三段螺线管磁场非均匀度分布。其中L=0.45的三段螺线管在储存泡区域的最大非均匀度为0.105%,相应的跃迁频率相对变化率为1.02×10-13。采用相同的方法计算了四组线圈以及五组线圈构造匀强磁场时线圈间的安匝比和间距,并对线圈内的磁场进行了有限元仿真,给出了非均匀度分布,四组线圈式C场筒内磁场在储存泡区域的非均匀度最大值为0.066%,相应的跃迁频率相对变化率为6.42×10-14。 相似文献
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从准确的MHD方程组出发,本文用线性微扰法研究了无力磁场(1)与流场(2)偶合后的稳定性.求得的色散关系依赖于流速V_0与Alfven速度V_A的比值,变分近似计算给出不稳定产生的充要条件为β=1/3.与磁场正交的横向扰动是最不稳定的模式. 相似文献
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本文通过太阳活动区光球和色球速度场和磁场观测资料,讨论了黑子活动区附近流场的精细结构,论述了太阳大气中物质的流动呈纤维结构,以及速度场纤维与磁场,色球纤维和网络结构之间的关系。 相似文献
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太阳活动区中无作用力磁场偏离势场而积累了能量,对势场的偏离表现为磁场的切变。只要磁场松开扭转,就会释放能量而产生耀斑。本文根据这一基本思想,在无力因子α=常数的假定下,求出了无力磁场方程的分析解,并求出了扭转场磁能M_势场磁能M_p,可释放的自由磁能△M,磁通量Φ,总电流I,α和磁场衰减因子k等7个重要参量。这些量可表为场强B、扭转角和半影半径b的函数,后3个量可以测出,△M的公式可供太阳预报工作参考使用。将上述公式应用于1972年10月太阳活动区,算出各参量,其中△M的量级为10~(32)尔格,足够供给该活动区耀斑等活动现象的能量。与用Alfvén和Carlqvist的一维理论算出的结果比较,本文结果与观测结果更为符合。 相似文献
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024黑子(S.G.D编号为4964)是1988年3月份太阳上最大、磁场最强的黑子群。在日面上出现的半个月里,始终有耀斑产生。北京天文台怀柔太阳磁场望远镜对这个活动区作了常规观测,并获得了磁场和速度场资料。 024活动区是由一个偶极黑子和δ黑子组成的。12日01~h49~mUT,黑子刚从东部出现时就有耀斑和活动日珥产生。从速度场与H_β色球单色像对比来看,耀斑内有物质向里流动,而暗条中有物质向外抛射。024活动区的磁场十分复杂,S极、N极磁场互相包含、渗入、剪切,形成许多海湾结构。可能这就是产生了许多各种形状的耀斑的缘故。本文对磁场的形态作了描述。 相似文献
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本文利用最新的K型星视向速度资料,对太阳附近K型星运动学进行了研究,平均太阳运动的解算值是(u_0,v_0,w_0)=(-9.1±2.2,-20.4±2.6,-5.2±2.5)km/s,与早期一些研究结果的符合程度是令人满意的。按不同年龄组进行分析的结果表明,作为本地静止标准基础的年轻恒星可能存在着某种方向朝外的大尺度运动,另外,我们发现了近距K型星的平均太阳运动与Gould带的运动学状态有着某种表观上的一致性。 相似文献
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本文介绍了1980年7月14日日面(B.R.2562)3B级耀斑活动区的形态、光球磁场和视向速度分布特征。 结果表明,该耀斑是由两个部分组成的;活动区速度场的测量,对于探讨耀斑模型是重要的。 相似文献
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以1988年9月5日北京天文台怀柔太阳观测站高分辨率和高灵敏度磁强图为基础,首次给出了对一太阳宁静区小尺度磁场空间分布的二维功率谱。 尽管从总体上,功率谱的分布呈现从低频分量向高频分量迅速衰减的趋势,但是,反映小尺度磁场分布的不同尺度空间周期性的分离的尖峰,是功率谱的最主要特征。 本文的主要结果可概括为下列两点: (1)太阳宁静区的磁通量不仅凝聚在分离的、具有相对较强磁通量密度的磁结构内,而且磁结构的空间分布也呈现分离的尺度不同的周期。 (2)小尺度磁场空间分布的最显著的周期,具有超米粒的空间尺度。这与以往磁对流理论与有关观测结果相一致。在功率谱中,还可以证认相应于亚超米粒,及亚超米粒和超米粒之间尺度的空间周期的大量尖峰。这是本文首次得到的。 包含更多观测资料的进一步工作是必须的,特别是获得对同一宁静区的速度场和磁场同时性的二维功率谱,对研究磁场和对流速度场的相互作用是有重要意义的。观测的功率谱与理论预测谱的比较,将有助于理解太阳光球分离磁结构形成的物理过程。 相似文献
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We investigate the nonlinear evolution of resistive tearing mode in a current sheet with a sheared flow in a long, thin cylinder. The results show that a hyperbolic secant (sech) flow field will lead to instability of the resistive tearing mode, formation of magnetic islands and rapid release of magnetic energy. The coupling between sheared flow and the tearing mode and interaction between suprathermal instabilities change the degree of shear in the magnetic field (the electric current gradient) and drive the development of the instability. This process may be one of the mechanisms of solar flares. 相似文献
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Equations governing the coupling of the scalar and vector potentials for a resistive electron-positron plasma in a strong magnetic field are derived. It is shown that in the presence of magnetic shear, a tearing instability may occur. The latter can lead to magnetic field line reconnection and the formation of magnetic islands which could affect the dynamics of the pulsar magnetosphere. 相似文献
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A pictorial explanation for shear-Hall instability is suggested and shows that the shear flow is not necessary for the instability because its role can be played by the Hall effect of an inhomogeneous backgroundmagnetic field. Linear stability analysis for a simplemodel of magnetic field varying periodically in space confirms such a “double Hall” instability. Numerical computations show a considerable increase in Ohmic dissipation rate at the nonlinear stage of instability development. Field dissipation has a spiky character associated with magnetic reconnection in current sheets and X-points. Double Hall instability can be significant for magnetic field dissipation in neutron star crusts and, possibly, in the solar corona. 相似文献
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It has been demonstrated in the past that single, two-dimensional coronal arcades are very unlikely driven unstable by a simple shear of the photospheric footpoints of the magnetic field lines. By means of two-dimensional, time-dependent MHD simulations, we present evidence that a resistive instability can result if in addition to the footpoint shear a slow motion of the footpoints towards the photospheric neutral line is included. Unlike the model recently proposed by van Ballegooijen and Martens (1989), the photospheric footpoint velocity in our model is nonsingular and the shear dominates everywhere. Starting from a planar potential field geometry for the arcade, we find that after some time a current sheet is formed which is unstable with respect to the tearing instability. The time of its onset scales with the logarithm of the magnetic diffusivity assumed in our calculation. In its nonlinear phase, a quasi-stationary situation arises in the vicinity of the x-line with an almost constant reconnection rate. The height of the x-line above the photosphere and the distance of the separatrix footpoints remain almost constant in this phase, while the helical flux tube, formed above the neutral line, continuously grows in size. 相似文献
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Shear mixing is believed to be the main mechanism to provide extra mixing in stellar interiors. We present results of three-dimensional (3D) simulations of the magnetohydrodynamic Kelvin–Helmholtz instability in a stratified shear layer. The magnetic field is taken to be uniform and parallel to the shear flow. We describe the evolution of the fluid flow and the magnetic field for a range of initial conditions. In particular, we investigate how the mixing rate of the fluid depends on the Richardson number and the magnetic field strength. It is found that the magnetic field can enhance as well as suppress mixing. Moreover, we have performed two-dimensional (2D) simulations and discuss some interesting differences between the 2D and 3D results. 相似文献
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The stability properties of magnetized discs rotating with angular velocity Ω = Ω( s , z ), dependent on both the radial and the vertical coordinates s and z , are considered. Such a rotation law is adequate for many astrophysical discs (e.g., galactic and protoplanetary discs, as well as accretion discs in binaries). In general, the angular velocity depends on height, even in thin accretion discs. A linear stability analysis is performed in the Boussinesq approximation, and the dispersion relation is obtained for short-wavelength perturbations. Any dependence of Ω on z can destabilize the flow. This concerns primarily small-scale perturbations for which the stabilizing effect of buoyancy is strongly suppressed due to the energy exchange with the surrounding plasma. For a weak magnetic field, instability of discs is mainly associated with vertical shear, whilst for an intermediate magnetic field the magnetic shear instability, first considered by Chandrasekhar and Velikhov, is more efficient. This instability is caused by the radial shear which is typically much stronger than the vertical shear. Therefore the growth time for the magnetic shear instability is much shorter than for the vertical shear instability. A relatively strong magnetic field can suppress both these instabilities. The vertical shear instability could be the source of turbulence in protoplanetary discs, where the conductivity is low. 相似文献
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This study follows the numerical results presented in Marsenić & Ševčík (2010) that explored the influence of the critical level position on stability of a system. The model was a horizontal fluid layer between z = ±0.5d rotating with an angular velocity Ω = Ω0 ž about the vertical axis z . The fluid was considered to be inviscid, finitely electrically conducting and incompressible and was permeated by a horizontal magnetic field B 0 = ℬ︁0B0(z) y̌ , where ℬ︁0 was the magnitude of the field and the function B0(z) = tanh [γ (z –z0)]. When γ is large, the field gradient is concentrated near z = z0, the critical level, the field being almost homogeneous elsewhere. In this way it controls the width of the magnetic shear layer associated with the current sheet. It was found that at conditions when the magnetic field gradient was large enough (γ = O (10)) and the critical level was placed close enough to the (bottom) perfectly conducting boundary (z0 < –0.388d for γ = 80), magnetically driven convection appeared localized to a close neighbourhood of the critical level – the so called critical layer. Based on the circumstances of its rise and its properties it was identified with the resistive tearing‐mode instability. This paper presents an analytical treatment of the problem assuming γ ≥ 1. The approach consists in separation of the computational domain into an outer region where the diffusionless limit (Elsasser number Λ → ∞) applies and an inner region (the critical layer) of finite conductivity. According to the tearing‐mode theory in classical systems, the solution in the inner region is sought as long‐wavelength with respect to the width of the critical layer. The obtained solution shows features similar to the one obtained numerically and confirmed relevance of the simplifying physical assumptions made in each region. The convection in the critical layer is strictly conditioned by a sharp magnetic shear. If the shear region is removed by further positioning of the critical level towards the perfectly conducting boundary, the localized convection disappears. It is in compliance with the fact that the system is stabilised by a perfectly conducting boundary with respect to the tearing mode. Stability is then checked numerically in the layer bounded by perfectly conducting boundaries where the critical point of the magnetic field lies on one of them. The existence of a magnetically driven instability is confirmed. Depending on the value γ, it may rise as a stationary convection (for γ < 1.5) or as a wave which for γ > 16 exhibits similarity properties (© 2011 WILEY‐VCH Verlag GmbH & Co. KGaA, Weinheim) 相似文献
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J.R. Kan 《Planetary and Space Science》1979,27(4):351-354
A family of exact analytic solutions of the time-independent Vlasov-Maxwell equations is presented. The solutions describe two-dimensional equilibrium current sheet with magnetic field structures resembling that produced by the tearing instability. In particular, the solutions presented here do not restrict the field in the magnetic island to small magnitude. It is shown that as the scale length of the magnetic island increases, the thickness of the current sheet increases while the average current and the average magnetic energy decrease. The tearing structures described by the solutions may exist in the magnetotail current sheet, the magnetopause current layer and the field-aligned auroral sheet current. 相似文献
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The process of magnetic reconnection in anisotropic plasmas is studied numerically using a 2-dimensional, 3-component hybrid simulation. The results of the calculation show that, when the plasma pressure in the direction perpendicular to magnetic field is larger than that in the parallel direction (e.g. P/P = 1.5), instability may greatly increase, speeding up the rate of reconnection. When P is smaller than P, (e.g., when P/P = 0.6), fire hose instability appears, which will restrain the tearing mode instability and the process of magnetic reconnection. 相似文献
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Filaments and flares are prominent indicators of the magnetic fields of solar activity. These instability phenomena arise from the influence of weak transport effects (radiation and resistivity, respectively) on coronal magnetodynamics and energy flow. We have previously shown that the filament and flare (tearing or reconnection) mechanisms are resistively coupled in sheared magnetic fields of the kind existing in active regions. The present paper expands this treatment to include the effects of compressibility and viscosity, which are most prominent at short wavelengths. The results show that compressibility affects the radiative mode, including a modest increase of its growth rate, and that viscosity modifies the tearing mode, partially through a decrease of its growth rate. A comprehensive discussion of the mode structures and flows is presented. The strongest effect found is a reversal, at very long wavelengths, of the radiative cooling of the resistive interior layer of the tearing mode, caused by compressional heating. 相似文献