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Influence of asymmetries in the magnetic draping pattern at Titan on the emission of energetic neutral atoms

机译:土卫六磁悬垂模式的不对称性对高能中性原子发射的影响

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We model the emission of energetic neutral atoms (ENAs) that are generated by the interaction between energetic ions from Saturn's magnetosphere and neutrals from the upper atmosphere of the giant planet's largest moon Titan. The trajectories of the parent ions and the resulting ENA emission morphology are highly sensitive to the electromagnetic field configuration near the moon. We therefore compare the ENA emission pattern for spatially homogeneous fields to the emission obtained from a magnetohydrodynamic (MHD) and a hybrid (kinetic ions, fluid electrons) model of Titan's magnetospheric interaction, by computing the trajectories of several billion energetic test particles. While the MHD model takes into account the draping of the magnetic field lines around Titan, the hybrid approach also considers the significant asymmetries in the electromagnetic fields due to the large gyroradii of pick-up ions from Titan's ionosphere. In all three models, the upstream parameters correspond to the conditions during Cassini's TA flyby of Titan. The shape, magnitude, and location of the ENA emission maxima vary considerably between these three field configurations. The magnetic pile-up region at Titan's ramside deflects a large number of the energetic parent ions, thereby reducing the ENA flux. However, the draped magnetic field lines in Titan's lobes rotate the gyration planes of the incident energetic ions, thereby facilitating the observable ENA production. Overall, the ENA flux calculated for the MHD model is weaker than the emission obtained for the electromagnetic fields from the hybrid code. In addition, we systematically investigate the dependency of the ENA emission morphology on the energy of the parent ions and on the upstream magnetic field strength.
机译:我们对高能中性原子(ENA)的发射进行建模,该发射是由土星磁层的高能离子与巨型星球最大的卫星土卫六上层大气的中性相互作用产生的。母离子的轨迹和所得的ENA发射形态对月球附近的电磁场配置高度敏感。因此,我们通过计算数十亿个高能测试粒子的轨迹,将空间均匀场的ENA发射模式与从磁流体动力学(MHD)和泰坦磁层相互作用的混合模型(动力学离子,流体电子)获得的发射进行了比较。虽然MHD模型考虑了土卫六周围磁场线的悬垂,但混合方法还考虑了由于土卫六电离层吸收离子的大回旋半径而引起的电磁场中的显着不对称性。在所有三个模型中,上游参数都对应于卡西尼号(Cassini)在泰坦(Titan)飞越时的情况。在这三个场配置之间,ENA发射最大值的形状,大小和位置有很大不同。泰坦斜面上的磁性堆积区域会偏转大量高能母离子,从而降低ENA通量。但是,泰坦波瓣中的垂线磁场线旋转了入射高能离子的回转平面,从而促进了可观察到的ENA的产生。总体而言,为MHD模型计算出的ENA通量要弱于从混合代码中为电磁场获得的发射。此外,我们系统地研究了ENA发射形态对母离子能量和上游磁场强度的依赖性。

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