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Nonlinear wave structures in collisional plasma of auroral E-region ionosphere

机译:极光E区电离层碰撞等离子体中的非线性波结构

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Studies of the auroral plasma withsmall-scale inhomogenieties producing the VHF-radar reflections (radar aurora)when observed in conditions of the saturated Farley-Buneman instability withinthe auroral E region, show strong nonlinear interactions and densityfluctuations of 5–15%. Such nonlinearity and high fluctation amplitudes areinconsistent with the limitations of the weak turbulence theory, and thus atheory for arbitrary amplitudes is needed. To this end, a nonlinear theory isdescribed for electrostatic MHD moving plasma structures of arbitrary amplitudefor conditions throughout the altitude range of the collisional auroral Eregion. The equations are derived, from electron and ion motion self-consistentwith the electric field, for the general case of the one-dimensional problem.They take into account nonlinearity, electron and ion inertia, diffusion,deviation from quasi-neutrality, and dynamical ion viscosity. The importance ofthe ion viscosity for dispersion is stressed, while deviation from thequasi-neutrality can be important only at rather low plasma densities, nottypical for the auroral E region. In a small amplitude limit these equationshave classical nonlinear solutions of the type of "electrostatic shockwave" or of knoidal waves. In a particular case these knoidal waves degradeto a dissipative soliton. A two-dimensional case of a quasi-neutral plasma isconsidered in the plane perpendicular to the magnetic field by way of thePoisson brackets, but neglecting the nonlinearity and ion inertia. It is shownthat in these conditions an effective saturation can be achieved at thestationary turbulence level of order of 10%.
机译:在极光E区域内的饱和Farley-Buneman不稳定性条件下观察到的具有小范围非均质性的极光等离子体产生VHF-雷达反射(雷达极光)时,显示出强烈的非线性相互作用和5-15%的密度波动。这种非线性和高涨幅幅度与弱湍流理论的局限性不一致,因此需要任意幅度的理论。为此,描述了一种非线性理论,用于在碰撞极光E区域的整个高度范围内,任意振幅的静电MHD移动等离子体结构。对于一维问题的一般情况,这些方程是从与电场自一致的电子和离子运动中得出的,它们考虑了非线性,电子和离子惯性,扩散,准中性偏差和动态离子粘度。强调了离子粘度对分散的重要性,而偏离准中性仅在相当低的等离子体密度下才很重要,这对于极光E区而言并不常见。这些方程在较小的幅度范围内具有“静电冲击波”或节形波类型的经典非线性解。在特定情况下,这些节状波退化为耗散孤子。通过泊松括号,在垂直于磁场的平面中考虑了一个准中性等离子体的二维情况,但忽略了非线性和离子惯性。结果表明,在这些条件下,静止湍流水平约为10%时,可以达到有效的饱和度。

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