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A theoretical model of the inner proton radiation belt

机译:内质子辐射带的理论模型

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A theoretical calculation provides inner radiation belt proton intensities as a function of time and of the three adiabatic invariants, M, K, and L, in the kinetic energy range from ∼10 MeV to ∼4 GeV and the L range from 1.1 to 2.4. Long residence times for trapped protons of up to several thousand years require similarly long input time series for the geomagnetic field, solar activity, and solar proton fluences. Additional inputs include galactic cosmic ray spectra, nuclear scattering cross sections, and the neutral and plasma densities in the atmosphere, ionosphere, and plasmasphere. Trapped proton sources are cosmic ray albedo neutron decay (CRAND), calculated from a Monte Carlo particle transport simulation, and solar proton injection using a derived empirical injection efficiency that is ∼10 at 10 MeV. Radial diffusion provides inward transport of injected solar protons. Calculated intensities at energies ≲ 100 MeV and for L ≳ 1.3 are dominated by solar protons, CRAND being the dominant source otherwise. Losses are by ionization of the neutral atmosphere, energy transfer to plasma electrons, and inelastic nuclear scattering. Numerical trajectory tracing determines trapping limits and drift shell averages of the albedo neutron intensity and of neutral and plasma densities for loss rate calculations. Geomagnetic secular variations cause adiabatic energy and drift shell changes. Intensities are greater than they would be in a constant geomagnetic field by factors up to ∼10, a result of long proton residence times and the presently decreasing geomagnetic dipole moment.
机译:理论计算提供了内部辐射带质子强度随时间的变化以及三个绝热不变量M,K和L的时间函数,其动能范围为〜10 MeV至〜4 GeV,L范围为1.1至2.4。长达数千年的质子滞留时间长,对于地磁场,太阳活动和太阳质子通量也需要同样长的输入时间序列。其他输入包括银河系宇宙射线光谱,核散射截面以及大气,电离层和等离子体层中的中性和等离子体密度。陷获的质子源是通过蒙特卡洛粒子传输模拟计算出的宇宙射线反照率中子衰变(CRAND),以及使用导出的经验注入效率在10 MeV下约为10的太阳质子注入。径向扩散提供了注入的太阳能质子的向内传输。能量≲100 MeV和L≳1.3时的计算强度主要由太阳质子决定,否则CRAND是主要来源。损失是由于中性大气的电离,能量转移到等离子电子以及无弹性的核散射造成的。数值轨迹跟踪确定了反照率中子强度以及中性和等离子体密度的俘获极限和漂移壳平均值,用于损耗率计算。地磁长期变化会导致绝热能量和漂移壳的变化。由于质子停留时间长以及目前地磁偶极矩减小,强度比在恒定地磁场中的强度高出约10倍。

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