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Characteristics of electromagnetic Rayleigh-Taylor modes in nighttime equatorial plasma

机译:电磁瑞利泰勒的特点在夜间模式赤道等离子体

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The unstable Rayleigh-Taylor plasma modes that are believed to be responsible for the density irregularities in the nighttime F region equatorial ionosphere have been studied before by assuming that the modes are electrostatic. In this paper, these plasma modes are studied without such assumption in order to determine the strength and the characteristics of the magnetic field fluctuations and to determine the physical condition under which the electrostatic assumption is justified. It is found that the relevant magnetic field fluctuations ( Bρ), which arise from the fluctuating parallel (to B 0) current density, are associated with the shear Alfven waves. The parameter that determines the amplitude of Bρ is α(s) ≡ D m (s)k 2/γ, where D m k 2 represents the rate at which magnetic field fluctuations with perpendicular wavelength λφ (≡ 2π/k φ) diffuse away due to parallel resistivity and γ is the rate at which the fluctuations grow. Typically, α 1 in the equatorial ionosphere, which means that the excited magnetic field fluctuations diffuse at a rate much faster than their growth rate and, consequently, their amplitudes remain very small (compared to B 0). Thus the Rayleigh-Taylor modes in the equatorial ionosphere are predominantly electrostatic in nature, and the electrostatic assumption of the previous analyses is quite justified. If the maximum amplitude of the electric field fluctuations ( ) is taken to be 1 mV/m, then the maximum amplitude of ρ is found to be less than 0.2 nT when λφ is 500 m, and it increases to about 2.4 nT when λ is 20 km. Longer wavelength modes have somewhat larger magnetic field fluctuations, but their growth rates are smaller. While the maximum amplitude of occurs at the magnetic equator, that of Bρ occurs at a distance away from it.
机译:瑞利泰勒不稳定的等离子体模式相信负责密度在夜间F地区违规行为赤道电离层研究之前假设模式是静电。摘要,这些等离子体模式进行了研究没有这样的假设来确定力量和磁性的特点场波动和确定的物理条件下静电假设是合理的。相关的磁场波动(Bρ)出现波动的平行B (0)电流密度,与剪切相关联阿尔芬波。振幅Bρα(s)≡D m (s) k 2 /γ,在D mk 2表示磁场的速度波动与垂直波长λφ(≡2π/ kφ)分散由于并联电阻率和γ的速率波动增长。通常情况下,α1在赤道电离层,这意味着激动的磁场吗波动扩散速度快得多他们的增长速度,因此,他们的振幅保持非常小(相对于B 0)。因此,瑞利泰勒模式在赤道电离层主要是静电自然,和静电的假设先前的分析很有道理的。最大电场的振幅波动()为1 mV / m,那么最大振幅的ρ是发现不到0.2元,当λφ500,它增加当λ是20公里约2.4元。模式有更大的磁场波动,但是他们的增长率更小。而最大振幅的发生磁赤道,B的ρ发生在距离远离它。

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