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Development of a new three-dimensional mathematical ionosphere model at european space agency/european space operations centre

机译:在欧洲航天局/欧洲航天运营中心开发新的三维数学电离层模型

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For several years a clear trend from the application of classical so-called “single layer” models to attempts to model the ionosphere in accordance to its real three-dimensional nature can be observed (see, e.g., Scherliess et al., 2003; Hernández-Pajares et al., 1999). European Space Agency (ESA)/European Space Operations Centre (ESOC) commenced in 1998 employing a three-dimensional (3-D) model for ionosphere processing (Feltens, 1998; Feltens et al., 1998). This first version of a 3-D model at ESOC model was based on a simple Chapman profile approach, assuming that the vertical component of the ionosphere could be mathematically expressed in terms of a single β-layer Chapman profile function. The profile function's parameters, maximum electron density N0 and its height h0, were in turn expressed as surface functions of geomagnetic latitude and local time whose coefficients were estimated. In this way a horizontal variation of N0 and h0 was modeled, and the profile function varied vertically, depending on the actual N0 and h0 values at a certain location. The ionosphere, however, consists of several layers. Additionally, the plasmasphere on top of the ionosphere must be accounted for, and the scale height, needed to compute the profile function z-parameter, is height-dependent. Furthermore, some of the ionosphere layers are so called α-layers and some parts of the ionosphere show special behavior. All these effects must be accounted for in a proper 3-D mathematical modeling. It is the intent of this paper to give a substantial overview over the 3-D ionosphere models developed at ESOC and their current testing and implementation status.
机译:多年来,可以观察到从应用经典的所谓“单层”模型到尝试根据电离层的真实三维性质对电离层建模的明显趋势(参见,例如,Scherliess等人,2003年;Hernández -Pajares等,1999)。欧洲航天局(ESA)/欧洲航天运行中心(ESOC)于1998年开始使用电离层处理的三维(3-D)模型(Feltens,1998; Feltens等,1998)。 ESOC模型的3-D模型的第一个版本基于简单的Chapman剖面方法,假设电离层的垂直分量可以用单个β层Chapman剖面函数来数学表示。剖面函数的参数,即最大电子密度N0及其高度h0依次表示为地磁纬度和当地时间的表面函数,并对其系数进行了估算。这样,就模拟了N0和h0的水平变化,轮廓函数垂直变化,具体取决于特定位置的实际N0和h0值。但是,电离层由几层组成。此外,必须考虑电离层顶部的等离子层,并且计算轮廓函数z参数所需的标尺高度取决于高度。此外,一些电离层被称为α层,电离层的某些部分表现出特殊的行为。所有这些影响都必须在适当的3D数学建模中加以考虑。本文的目的是对ESOC开发的3-D电离层模型及其当前的测试和实施状态进行实质性概述。

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