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PARTICLE ACCELERATION BY SLOW MODES IN STRONG COMPRESSIBLE MAGNETOHYDRODYNAMIC TURBULENCE, WITH APPLICATION TO SOLAR FLARES

机译:强可压缩磁流体动力湍流中慢模的颗粒加速及其在太阳耀斑中的应用

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摘要

Energetic particles that undergo strong pitch-angle scattering and diffuse through a plasma containing strong compressible MHD turbulence undergo diffusion in momentum space with diffusion coefficient D_p. If the rms turbulent velocity is of the order of the Alfven speed v_A, the contribution to D_p from slow-mode eddies is approx=(2p~2v_A/9l)[ln(lv_A/D_‖) + 2γ - 3], where l is the outer scale of the turbulence, γ approx= 0.577 is Euler's constant, and D_‖ is the spatial diffusion coefficient of energetic particles, which is assumed to satisfy D_‖ lv_A. The energy spectrum of accelerated particles is derived for this value of D_p, taking into account Coulomb losses and particle escape from the acceleration region with an energy-independent escape time. Slow modes in the D_‖ lv_A limit are an unlikely explanation for electron acceleration in solar flares to energies of 10-100 keV, because for solar flare conditions, the predicted acceleration times are too long, and the predicted energy spectra are too hard. The acceleration mechanism discussed in this paper could in principle explain the relatively hard spectra of gyrosynchrotron-emitting electrons in the 100-5000 keV range, but only if D_‖ lv_A for such particles.
机译:经历强螺距角散射并通过包含强可压缩MHD湍流的等离子体扩散的高能粒子在动量空间中以扩散系数D_p扩散。如果均方根湍流速度约为Alfven速度v_A,则慢模涡旋对D_p的贡献约为(2p〜2v_A / 9l)[ln(lv_A /D_‖)+2γ-3],其中l是湍流的外部尺度,γ近似= 0.577是欧拉常数,D_‖是高能粒子的空间扩散系数,假定满足D_‖ lv_A。对于D_p的这个值,可以得出加速粒子的能谱,其中要考虑库仑损耗和粒子从加速区域逸出的能量独立逸出时间。 D_ lv_A极限中的慢模式不可能解释太阳耀斑中电子加速到10-100 keV的能量,因为对于太阳耀斑条件,预测的加速时间太长,并且预测的能谱太难。本文讨论的加速机制原则上可以解释在100-5000 keV范围内发射回旋回旋加速器的电子的相对较硬的光谱,但前提是此类粒子的D_″ lv_A。

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