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首页> 外文期刊>The Astrophysical journal >NUMERICAL SIMULATIONS OF CORONAL MASS EJECTION ON 2011 MARCH 7: ONE-TEMPERATURE AND TWO-TEMPERATURE MODEL COMPARISON
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NUMERICAL SIMULATIONS OF CORONAL MASS EJECTION ON 2011 MARCH 7: ONE-TEMPERATURE AND TWO-TEMPERATURE MODEL COMPARISON

机译:2011年3月7日冠状气体喷射的数值模拟:一温度模型和两温度模型的比较

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During Carrington rotation (CR) 2107, a fast coronal mass ejection (CME; 2000?km?s–1) occurred in active region NOAA 11164. This event is also associated with a solar energetic particle event. In this study, we present simulations of this CME with one-temperature (1T) and two-temperature (2T: coupled thermodynamics of the electron and proton populations) models. Both the 1T and 2T models start from the chromosphere with heat conduction and radiative cooling. The background solar wind is driven by Alfvén-wave pressure and heated by Alfvén-wave dissipation in which we have incorporated the balanced turbulence at the top of the closed field lines. The magnetic field of the inner boundary is set up using a synoptic map from Solar Dynamics Observatory/Helioseismic and Magnetic Imager. The Titov-Démoulin flux-rope model is used to initiate the CME event. We compare the propagation of fast CMEs and the thermodynamics of CME-driven shocks in both the 1T and 2T CME simulations. Also, the synthesized white light images are compared with the Solar and Heliospheric Observatory/Large Angle and Spectrometric Coronagraph observations. Because there is no distinction between electron and proton temperatures, heat conduction in the 1T model creates an unphysical temperature precursor in front of the CME-driven shock and makes the shock parameters (e.g., shock Mach number, compression ratio) incorrect. Our results demonstrate the importance of the electron heat conduction in conjunction with proton shock heating in order to produce the physically correct CME structures and CME-driven shocks.
机译:在卡灵顿旋转(CR)2107期间,在活动区域​​NOAA 11164中发生了快速日冕物质抛射(CME;> 2000?km?s-1)。该事件也与太阳高能粒子事件有关。在这项研究中,我们用一个温度(1T)和两个温度(2T:电子和质子种群的耦合热力学)模型对这种CME进行了模拟。 1T和2T模型都从色球层开始,具有热传导和辐射冷却功能。背景太阳风是由Alfvén波压力驱动的,并由Alfvén波消散的热量加热,其中我们在封闭的场线顶部合并了平衡湍流。内边界的磁场是使用来自太阳动力学天文台/流变和磁成像仪的天气图建立的。 Titov-Démoulin助熔剂绳缆模型用于启动CME事件。我们在1T和2T CME模拟中比较了快速CME的传播和CME驱动的冲击的热力学。同样,将合成的白光图像与太阳和日球天文台/大角度观测仪和光谱日冕仪观测仪进行比较。由于电子温度和质子温度之间没有区别,因此1T模型中的热传导会在CME驱动的电击之前产生非自然的温度前体,并使电击参数(例如电击马赫数,压缩比)不正确。我们的结果证明了电子热传导与质子激波加热相结合的重要性,以便产生物理上正确的CME结构和CME驱动的激波。

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