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TWO-DIMENSIONAL RADIATIVE MAGNETOHYDRODYNAMIC SIMULATIONS OF THE IMPORTANCE OF PARTIAL IONIZATION IN THE CHROMOSPHERE

机译:染色体中部分电离重要性的二维径向磁流体动力学模拟

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The bulk of the solar chromosphere is weakly ionized and interactions between ionized particles and neutral particles likely have significant consequences for the thermodynamics of the chromospheric plasma. We investigate the importance of introducing neutral particles into the MHD equations using numerical 2.5D radiative MHD simulations obtained with the Bifrost code. The models span the solar atmosphere from the upper layers of the convection zone to the low corona, and solve the full MHD equations with non-gray and non-LTE radiative transfer, and thermal conduction along the magnetic field. The effects of partial ionization are implemented using the generalized Ohm's law, i.e., we consider the effects of the Hall term and ambipolar diffusion in the induction equation. The approximations required in going from three fluids to the generalized Ohm's law are tested in our simulations. The Ohmic diffusion, Hall term, and ambipolar diffusion show strong variations in the chromosphere. These strong variations of the various magnetic diffusivities are absent or significantly underestimated when, as has been common for these types of studies, using the semi-empirical VAL-C model as a basis for estimates. In addition, we find that differences in estimating the magnitude of ambipolar diffusion arise depending on which method is used to calculate the ion-neutral collision frequency. These differences cause uncertainties in the different magnetic diffusivity terms. In the chromosphere, we find that the ambipolar diffusion is of the same order of magnitude or even larger than the numerical diffusion used to stabilize our code. As a consequence, ambipolar diffusion produces a strong impact on the modeled atmosphere. Perhaps more importantly, it suggests that at least in the chromospheric domain, self-consistent simulations of the solar atmosphere driven by magnetoconvection can accurately describe the impact of the dominant form of resistivity, i.e., ambipolar diffusion. This suggests that such simulations may be more realistic in their approach to the lower solar atmosphere (which directly drives the coronal volume) than previously assumed.
机译:太阳色球的大部分被弱电离,电离粒子和中性粒子之间的相互作用可能会对色球等离子的热力学产生重大影响。我们调查使用Bifrost代码获得的数值2.5D辐射MHD模拟将中性粒子引入MHD方程的重要性。这些模型涵盖了从对流区上层到低日冕的太阳大气层,并求解了具有非灰色和非LTE辐射传递以及沿磁场的热传导的完整MHD方程。部分电离的影响是使用广义欧姆定律实现的,即我们在感应方程中考虑了霍尔项和双极性扩散的影响。在我们的仿真中测试了从三种流体到广义欧姆定律所需的近似值。欧姆扩散,霍尔项和双极性扩散在色球中显示出很大的变化。使用半经验的VAL-C模型作为估计的基础时,对于这些类型的研究很常见,各种磁扩散率的这些强变化都没有出现或被大大低估了。此外,我们发现估算双极性扩散幅度的差异取决于使用哪种方法来计算离子中性碰撞频率。这些差异导致在不同的磁扩散率方面存在不确定性。在色球中,我们发现双极性扩散与稳定我们的代码所用的数值扩散具有相同的数量级,甚至更大。结果,双极扩散会对模拟大气产生强烈影响。也许更重要的是,它表明至少在色球层域,由磁对流驱动的太阳大气的自洽模拟可以准确地描述主要电阻率形式(即双极扩散)的影响。这表明,在模拟较低的太阳大气层(直接驱动日冕体积)时,这种模拟可能比以前设想的更为现实。

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