Model results for the ionospheric lower transition height over mid-latitude

Theoretical calculations of the ionospheric lower transition height (LTH), a level of equal O<sup>+</sup> and molecular ion densities, were performed and compared with empirical models by Zhang et al.&nbsp;(1996). This paper represents a substantial extension of the prior work by...

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Main Authors: J. Lei, L. Liu, W. Wan, S.-R. Zhang
Format: Article
Language:English
Published: Copernicus Publications 2004-06-01
Series:Annales Geophysicae
Online Access:https://www.ann-geophys.net/22/2037/2004/angeo-22-2037-2004.pdf
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spelling doaj-1bf97c1585e34d329bc8ea5c5ec021d02020-11-25T00:39:14ZengCopernicus PublicationsAnnales Geophysicae0992-76891432-05762004-06-01222037204510.5194/angeo-22-2037-2004Model results for the ionospheric lower transition height over mid-latitudeJ. Lei0J. Lei1L. Liu2W. Wan3S.-R. Zhang4Institute of Geology and Geophysics, Chinese Academy of Sciences, Beijing 100029, ChinaWuhan Ionospheric Observatory, Wuhan Institute of Physics and Mathematics, Chinese Academy of Sciences, Wuhan 430071, ChinaInstitute of Geology and Geophysics, Chinese Academy of Sciences, Beijing 100029, ChinaInstitute of Geology and Geophysics, Chinese Academy of Sciences, Beijing 100029, ChinaHaystack Observatory, Massachusetts Institute of Technology, Westford, Massachusetts, USATheoretical calculations of the ionospheric lower transition height (LTH), a level of equal O<sup>+</sup> and molecular ion densities, were performed and compared with empirical models by Zhang et al.&nbsp;(1996). This paper represents a substantial extension of the prior work by including the AE-C data of ion composition analysis and by detailed quantitative studies of the LTH simulation, and by creating a new LTH empirical model based on our simulations. Results show that: (1) the calculated LTH, in general, is lowest near 11-13LT and reaches the diurnal maximum after midnight (about 01~02LT). The local time asymmetry becomes more evident in summer, when the time of minimum shifts to 16LT. (2) The simulated LTH presents a dominant, semiannual variation during nighttime, and a pronounced annual variation during daytime. (3) The simulated LTH increases with solar activity at night and decreases by day, while the standard IRI option has an opposite tendency at night in summer and equinox. Therefore, the day-night difference of simulated LTH significantly increases with solar activity. (4) Both daytime and nighttime LTHs, tend to increase with the increasing geomagnetic activity <i>A<sub>p</sub></i> index, with a mean slope about 0.1455km per <i>A<sub>p</sub></i> unit. (5) The diurnal variation of LTH is found to be more than 20 km, which is much larger than the seasonal variation under F107=100 and <i>A<sub>p</sub></i>=10. Thus, the diurnal and solar activity variations of LTH are more pronounced than its seasonal and magnetic activity variations.https://www.ann-geophys.net/22/2037/2004/angeo-22-2037-2004.pdf
collection DOAJ
language English
format Article
sources DOAJ
author J. Lei
J. Lei
L. Liu
W. Wan
S.-R. Zhang
spellingShingle J. Lei
J. Lei
L. Liu
W. Wan
S.-R. Zhang
Model results for the ionospheric lower transition height over mid-latitude
Annales Geophysicae
author_facet J. Lei
J. Lei
L. Liu
W. Wan
S.-R. Zhang
author_sort J. Lei
title Model results for the ionospheric lower transition height over mid-latitude
title_short Model results for the ionospheric lower transition height over mid-latitude
title_full Model results for the ionospheric lower transition height over mid-latitude
title_fullStr Model results for the ionospheric lower transition height over mid-latitude
title_full_unstemmed Model results for the ionospheric lower transition height over mid-latitude
title_sort model results for the ionospheric lower transition height over mid-latitude
publisher Copernicus Publications
series Annales Geophysicae
issn 0992-7689
1432-0576
publishDate 2004-06-01
description Theoretical calculations of the ionospheric lower transition height (LTH), a level of equal O<sup>+</sup> and molecular ion densities, were performed and compared with empirical models by Zhang et al.&nbsp;(1996). This paper represents a substantial extension of the prior work by including the AE-C data of ion composition analysis and by detailed quantitative studies of the LTH simulation, and by creating a new LTH empirical model based on our simulations. Results show that: (1) the calculated LTH, in general, is lowest near 11-13LT and reaches the diurnal maximum after midnight (about 01~02LT). The local time asymmetry becomes more evident in summer, when the time of minimum shifts to 16LT. (2) The simulated LTH presents a dominant, semiannual variation during nighttime, and a pronounced annual variation during daytime. (3) The simulated LTH increases with solar activity at night and decreases by day, while the standard IRI option has an opposite tendency at night in summer and equinox. Therefore, the day-night difference of simulated LTH significantly increases with solar activity. (4) Both daytime and nighttime LTHs, tend to increase with the increasing geomagnetic activity <i>A<sub>p</sub></i> index, with a mean slope about 0.1455km per <i>A<sub>p</sub></i> unit. (5) The diurnal variation of LTH is found to be more than 20 km, which is much larger than the seasonal variation under F107=100 and <i>A<sub>p</sub></i>=10. Thus, the diurnal and solar activity variations of LTH are more pronounced than its seasonal and magnetic activity variations.
url https://www.ann-geophys.net/22/2037/2004/angeo-22-2037-2004.pdf
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