Valence Habyarimana, John Bosco Habarulema, Daniel Okoh, Teshome Dugassa, Jean Claude Uwamahoro
{"title":"Single station modelling of ionospheric irregularities using artificial neural networks","authors":"Valence Habyarimana, John Bosco Habarulema, Daniel Okoh, Teshome Dugassa, Jean Claude Uwamahoro","doi":"10.1007/s10509-023-04261-8","DOIUrl":null,"url":null,"abstract":"<div><p>An empirical model of ionospheric irregularities over Mbarara (MBAR, 30.7<sup>∘</sup>E geographic longitude, 0.6<sup>∘</sup>S geographic latitude, 10.22<sup>∘</sup>S geomagnetic latitude) based on Artificial Neural Networks (ANNs) is developed using Global Navigation Satellite System (GNSS) derived Total Electron Content (TEC) data from 2001–2022. This long term data helped to study the climatology of the trends, the diurnal, seasonal, and solar activity dependence of ionospheric irregularities. We used the rate of change of TEC index (ROTI) to quantify the strength of irregularities. The input space consisted of time of the day (Hr), day of the year (doy), z-component of the Interplanetary magnetic field (IMF Bz), symmetric horizontal component of the ring current (SYM-H), solar activity factor (F10.7P), and vertical <b>E</b>×<b>B</b> drift, all of which are thought to influence irregularity occurrence, though with different percentage contributions. Of these inputs, Hr, doy, and F10.7P constituted the primary input parameters (PIP). We investigated the contribution of each input to the ROTI changes by developing seven models adding an input to the PIP at each time. The greatest contributor to the modelling results was SYM-H with a percentage contribution of ≈2% (8%) for the model with both quiet and disturbed (only disturbed) conditions. The accuracy of the overall model during both geomagnetically quiet and disturbed (only disturbed) conditions was 0.1479 (0.1494) TECU/min with a correlation coefficient of 0.72 (0.65). The diurnal variability of ROTI was observed with higher values of ROTI existing between 1600 UT (1900 LT) and 2300 UT (0200 LT) than during other UT hours of the day. The ROTI values exhibited the semi-annual/seasonal variability with higher values during the March equinox than during the September equinox, and lower values during the solstice months. We further confirmed that irregularities depend on the solar activity. They are strong during high solar activity and minimal/weak during low/minimum solar activity periods.</p></div>","PeriodicalId":8644,"journal":{"name":"Astrophysics and Space Science","volume":null,"pages":null},"PeriodicalIF":1.8000,"publicationDate":"2023-12-12","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":"0","resultStr":null,"platform":"Semanticscholar","paperid":null,"PeriodicalName":"Astrophysics and Space Science","FirstCategoryId":"101","ListUrlMain":"https://link.springer.com/article/10.1007/s10509-023-04261-8","RegionNum":4,"RegionCategory":"物理与天体物理","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":null,"EPubDate":"","PubModel":"","JCR":"Q3","JCRName":"ASTRONOMY & ASTROPHYSICS","Score":null,"Total":0}
引用次数: 0
Abstract
An empirical model of ionospheric irregularities over Mbarara (MBAR, 30.7∘E geographic longitude, 0.6∘S geographic latitude, 10.22∘S geomagnetic latitude) based on Artificial Neural Networks (ANNs) is developed using Global Navigation Satellite System (GNSS) derived Total Electron Content (TEC) data from 2001–2022. This long term data helped to study the climatology of the trends, the diurnal, seasonal, and solar activity dependence of ionospheric irregularities. We used the rate of change of TEC index (ROTI) to quantify the strength of irregularities. The input space consisted of time of the day (Hr), day of the year (doy), z-component of the Interplanetary magnetic field (IMF Bz), symmetric horizontal component of the ring current (SYM-H), solar activity factor (F10.7P), and vertical E×B drift, all of which are thought to influence irregularity occurrence, though with different percentage contributions. Of these inputs, Hr, doy, and F10.7P constituted the primary input parameters (PIP). We investigated the contribution of each input to the ROTI changes by developing seven models adding an input to the PIP at each time. The greatest contributor to the modelling results was SYM-H with a percentage contribution of ≈2% (8%) for the model with both quiet and disturbed (only disturbed) conditions. The accuracy of the overall model during both geomagnetically quiet and disturbed (only disturbed) conditions was 0.1479 (0.1494) TECU/min with a correlation coefficient of 0.72 (0.65). The diurnal variability of ROTI was observed with higher values of ROTI existing between 1600 UT (1900 LT) and 2300 UT (0200 LT) than during other UT hours of the day. The ROTI values exhibited the semi-annual/seasonal variability with higher values during the March equinox than during the September equinox, and lower values during the solstice months. We further confirmed that irregularities depend on the solar activity. They are strong during high solar activity and minimal/weak during low/minimum solar activity periods.
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