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Comparative study of the features of propagation of ordinary and extraordinary modes of short waves in the ionosphere
- Authors: Raubo K.V.1, Zakharov V.E.1
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Affiliations:
- Immanuel Kant Baltic Federal University
- Issue: Vol 69, No 6 (2024)
- Pages: 547-552
- Section: ЭЛЕКТРОДИНАМИКА И РАСПРОСТРАНЕНИЕ РАДИОВОЛН
- URL: https://ruspoj.com/0033-8494/article/view/650663
- DOI: https://doi.org/10.31857/S0033849424060061
- EDN: https://elibrary.ru/IJPCZH
- ID: 650663
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Abstract
The field parameters of ordinary and non-ordinary waves are compared each other while short waves propagate in the ionosphere.
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About the authors
K. V. Raubo
Immanuel Kant Baltic Federal University
Email: VEZakharov@kantiana.ru
Institute of High Technology
Russian Federation, Alexander Nevsky Str.14, Kaliningrad, 236041V. E. Zakharov
Immanuel Kant Baltic Federal University
Author for correspondence.
Email: VEZakharov@kantiana.ru
Institute of High Technology
Russian Federation, Alexander Nevsky Str.14, Kaliningrad, 236041References
- Лукин Д. С., Палкин Е. А., Ипатов Е. Б. и др. // Сб. докл. XXV Всерос. открытой науч. конф. «Распространение радиоволн». Томск. 4–9 июля 2016. Томск: Изд-во ТУСУР, 2016. Т. 1. С. 40.
- Крюковский А. С., Лукин Д. С., Кирьянова К. С. // РЭ. 2012. Т. 57. № 9. С. 1028.
- Bilitza D., Altadill D., Zhang Y. et al. / // J. Space Weather and Space Climate. 2014. V. 4. A07.
- Hedin A. E. // J. Geophys. Res. 1991. V. 96. № A1. P. 1159.
- Захаров В. Е. // РЭ. 2019. Т. 64. № 6. С. 525.
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Fig. 1. The modulus of the Cartesian projection |fx| (curve 1), |fy| (curve 2) and |fz| (curve 3) of the polarization vector of an ordinary wave at f = 5 (a), 10 (b) and 15 MHz (c).
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3.
Fig. 2. The module of the Cartesian projection |fx| (curve 1), |fy| (curve 2) and |fz| (curve 3) of the polarization vector of the extraordinary wave at f = 5 (a) and 10 MHz (b).
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4.
Fig. 3. Results of calculations of the attenuation factor of an ordinary wave at f = 5 (a), 10 (b) and 15 MHz (c): curve 1 is the contribution from absorption, curve 2 is the contribution from beam divergence, curve 3 is the total attenuation factor.
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5.
Fig. 4. Results of calculations of the attenuation factor of the extraordinary wave at f = 5 (a) and 15 MHz (b): curve 1 is the contribution from absorption, curve 2 is the contribution from the divergence of the rays, curve 3 is the total attenuation factor.
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