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首页> 外文期刊>Annales Geophysicae >Influence of the finite ionospheric conductivity on dispersive, nonradiative field line resonances
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Influence of the finite ionospheric conductivity on dispersive, nonradiative field line resonances

机译:电离层有限电导率对色散,非辐射场线共振的影响

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The influence of the finite ionosphericconductivity on the structure of dispersive, nonradiative field line resonances(FLRs) is investigated for the first four odd harmonics. The results are basedon a linear, magnetically incompressible, reduced, two-fluid MHD model. Themodel includes effects of finite electron inertia (at low altitude) and finiteelectron pressure (at high altitude). The ionosphere is treated as ahigh-integrated conducting substrate. The results show that even very lowionospheric conductivity (ΣP = 2 mho) is notsufficient to prevent the formation of a large-amplitude, small-scale,nonradiative FLR for the third and higher harmonics when the backgroundtransverse plasma inhomogeneity is strong enough. At the same time, thefundamental FLR is strongly affected by a state of low conductivity, and whenΣP = 2 mho, this resonance forms onlysmall-amplitude, relatively broad electromagnetic disturbance. The difference inconductivities of northern and southern ionospheres does not produce significantasymmetry in the distribution of electric and magnetic fields along the resonantfield line. The transverse gradient of the background Alfvén speed plays animportant role in structure of the FLR when the ionospheric conductivity isfinite. In cases where the transverse inhomogeneity of the plasma is not strongenough, the low ionospheric conductivity can prevent even higher-harmonic FLRsfrom contracting to small scales where dispersive effects are important. Theapplication of these results to the formation and temporal evolution ofsmall-scale, active auroral arc forms is discussed.
机译:研究了前四个奇数谐波的有限电离层电导率对色散,非辐射场线谐振(FLR)结构的影响。结果基于线性,磁不可压缩,简化的双流体MHD模型。该模型包括有限电子惯性(在低空)和有限电子压力(在高空)的影响。电离层被视为高度集成的导电基质。结果表明,即使非常低的电离层电导率(Σ P = 2 mho)也不足以防止第三次大幅度,小规模,无辐射的FLR的形成当背景横向等离子体不均匀性足够强时​​,会产生较高的谐波。同时,基本的FLR受低电导率状态的强烈影响,当∑ P = 2 mho时,该共振仅形成小幅度,相对宽泛的电磁干扰。北部和南部电离层的电导率差异不会在沿共振场线的电场和磁场分布中产生明显的不对称性。当电离层电导率一定时,背景Alfvén速度的横向梯度在FLR的结构中起着重要作用。在等离子体的横向不均匀性不够强的情况下,较低的电离层电导率可以防止什至更高谐波的FLR收缩到小尺度,而小尺度的弥散效应很重要。讨论了这些结果在小规模,活跃的极光弧形的形成和时间演化中的应用。

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