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Numerical MHD Simulation of the Coupled Evolution of Collisional Plasma and Magnetic Field in the Solar Chromosphere. I. Gradual and Impulsive Energisation

机译:碰撞等离子体耦合演化的数值mHD模拟   太阳色球层中的磁场和磁场。 I.渐进和冲动   通电

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摘要

The dynamical coupling between the solar chromospheric plasma and magneticfield is investigated by numerically solving a fully self-consistent,two-dimensional initial-value problem for the nonlinear collisional MHDequations including electric resistivity, thermal conduction, and, in somecases, gas-dynamic viscosity. The processes in the contact zone between twohorizontal magnetic fields of opposite polarities are considered. The plasma isassumed to be initially motionless and having a temperature of 50,000 K uniformthroughout the plasma volume; the characteristic magnetic field corresponds toa plasma $\beta\gtrsim 1$. In a physical-time interval of 17~seconds typicallycovered by a computational run, the plasma temperature gradually increases by afactor of two to three. Against this background, an impulsive (in 0.1 secondsor less) increase in the current-aligned plasma velocity occurs at the site ofthe current-layer thinning (sausage-type deformation, or $m=0$ pinchinstability). Such a "velocity burst" can be interpreted physically as an eventof suprathemal-proton generation. Further development of the sausageinstability results in an increase in the kinetic temperature of the protons tohigh values, even to those observed in flares. The form of our system of MHDequations indicates that such increases are a property of the exact solution ofthe system at an appropriate choice of the parameters. Magnetic reconnectiondoes not manifest itself in this solution: it would generate flows forbidden bythe chosen geometry. Therefore, the pinch-sausage effect can act as anenergiser of the upper chromosphere and be an alternative to themagnetic-reconnection process as the producer of flares.
机译:通过数值求解非线性碰撞MHD方程的完全自洽的二维初始值问题,包括电阻率,热传导以及某些情况下的气体动力粘度,研究了太阳色球等离子体与磁场之间的动力耦合。考虑极性相反的两个水平磁场之间的接触区中的过程。假定等离子体最初是不动的,并且在整个等离子体体积内温度均匀为50,000 K;特征磁场对应于等离子体$ \ beta \ gtrsim 1 $。在通常由计算运行发现的17秒的物理时间间隔中,等离子体温度逐渐升高2到3倍。在这种背景下,在电流层变薄的位置(香肠型变形,或$ m = 0 $夹入稳定性)发生了与电流对齐的等离子体速度的脉冲增加(0.1秒或更短)。这种“速度爆发”在物理上可以解释为超质子产生的事件。香肠不稳定性的进一步发展导致质子的动力学温度增加到很高的值,即使在火炬中观察到也是如此。我们的MHDequations系统的形式表明,在适当选择参数的情况下,这种增加是系统精确解的一个属性。磁性重新连接不会在此解决方案中显示出来:它将产生所选几何图形禁止的流量。因此,捏香肠效应可以充当上层色球的激励器,并且可以作为火炬产生器替代磁重联过程的替代者。

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