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Comparison between calculated and observed F region electron density profiles at Jicamarca, Peru

机译:秘鲁Jicamarca的F区电子密度分布图和观测到的F区电子密度分布图的比较

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摘要

Electron density profiles and isodensity contours derived from Jicamarca incoherent scatter radar observations in Peru for October 1–2, 1970, are compared in detail with results from the Phillips Laboratory global theoretical ionospheric model. This model solves the ion continuity equation for 0 concentration through production, loss, and transport of ionization. The primary factor controlling the peak plasma density at Jicamarca is the vertical E × B drift, which drives the ionization upward during the day and downward at night. When we use the measured drift in the model, we achieve excellent results with the measured electron density profiles. We illustrate the sensitivity of the low-latitude plasma density calculations to changes in the vertical E × B drift and changes in the neutral winds. We also compare the calculated profiles and peak parameters with an empirical model, the International Reference Ionosphere (IRI). We illustrate several limitations associated with the IRI that contribute to its limited capability at the magnetic equator.
机译:将从1970年10月1日至2日在秘鲁的Jicamarca非相干散射雷达观测得到的电子密度分布和等密度线轮廓与Phillips实验室全球理论电离层模型的结果进行了详细比较。该模型通过电离的产生,损失和传输来求解浓度为0的离子连续性方程。控制Jicamarca处的峰值等离子体密度的主要因素是垂直E×B漂移,该漂移在白天驱动向上电离,而在晚上推动向下电离。当我们在模型中使用测得的漂移时,用测得的电子密度分布图可获得出色的结果。我们说明了低纬度等离子体密度计算对垂直E×B漂移变化和中性风变化的敏感性。我们还将计算的剖面和峰参数与经验模型国际参考电离层(IRI)进行比较。我们举例说明了与IRI相关的一些局限性,这些局限性导致了IRI在磁赤道上的能力有限。

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