On the Role of the Ionospheric Parameters B0 and B1 in the Matching of Calculated and Experimental Values of MUF

D. Blagoveshchensky, O. Maltseva, G. Zhbankov
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Abstract

Despite certain limitations, the RI model is widely used in the interpretation and prediction of oblique propagation characteristics, for example, MUF. A special role is played by the adaptation (assimilation) of the model to the current diagnostics data, which makes it possible to correct the model in real time. The most widely used adaptation is to the main parameters of the ionosphere foF2 and hmF2. With the possibility of measuring the total electron content TEC, the values of this parameter are used for adaptation through the definition of foF2 using, for example, the equivalent slab thickness of the ionosphere or other approaches. However, in almost all cases there is a residual deviation of the calculated values of the MUF from the experimental MOFs, which is attributed to the difference in the shapes of the model and real N(h)-profiles. In this paper, to eliminate the residual deviation, the values of the B0 and B1 parameters are used, determining the shape of the N(h)- profiles of the lower ionosphere, which is close to real. One of the most quiet days was chosen on February 13, 2014 on the Dickson-Pevek path of oblique sounding. It is shown that the use of B0 and B1 can reduce the residual discrepancy, but does not remove it completely. The reason is the lack of accuracy in determining B0 and B1 in the high-latitude zone.
电离层参数B0和B1在MUF计算值和实验值匹配中的作用
尽管有一定的局限性,但RI模型被广泛用于解释和预测斜向传播特征,例如MUF。模型对当前诊断数据的自适应(同化)作用使得实时修正模型成为可能。目前应用最广泛的是对电离层主要参数of2和hmF2的自适应。由于有可能测量总电子含量TEC,该参数的值可用于通过定义foF2进行调整,例如使用电离层的等效板厚度或其他方法。然而,在几乎所有情况下,MUF的计算值与实验mof存在残差,这是由于模型形状与实际N(h)-剖面的差异。为了消除剩余偏差,本文利用B0和B1参数的值,确定了电离层下部N(h)-剖面的形状,该形状接近真实。2014年2月13日是Dickson-Pevek斜向探测路径上最安静的一天。结果表明,使用B0和B1可以减小残余差异,但不能完全消除残余差异。原因是在高纬度地区确定B0和B1的精度不高。
本文章由计算机程序翻译,如有差异,请以英文原文为准。
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