9 research outputs found

    Probability of erroneous reception of navigational radio signals under ionospheric disturbances

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    The work deals with the issues of the determination of the probability of frequency-selective fading (FSF) of navigational radio signals in satellite radio navigation systems under artificial ionosphere disturbances. The connection between the coherence band of the trans-ionospheric channel and the conditional size of ionospheric inhomogeneities is established. Based on the results of computer simulation, the threshold values of the Mean square deviation (MSD) of fluctuations of the total electron content in the inclined radio-line are determined, in which the probability of frequency-selective fading is hig

    The methodology for calculating the interval of the shortwave radio link frequency correlation with the sphericity and smallscale inhomogeneities of the ionosphere

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    The paper suggests the methodology for calculating the interval of the fading frequency correlation in the shortwave radio link with one discrete beam and its diffuse scattering. This methodology takes into account the effect of the sphericity and small-scale inhomogeneities of the ionosphere reflecting laye

    ΠœΠ΅Ρ‚ΠΎΠ΄ΠΈΠΊΠ° ΠΎΡ†Π΅Π½ΠΊΠΈ надСТности связи Π² ΠΊΠΎΡ€ΠΎΡ‚ΠΊΠΎΠ²ΠΎΠ»Π½ΠΎΠ²ΠΎΠΉ Ρ€Π°Π΄ΠΈΠΎΠ»ΠΈΠ½ΠΈΠΈ с райсовскими замираниями с ΡƒΡ‡Π΅Ρ‚ΠΎΠΌ диффузности ионосфСры

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    Introduction. There exists a technique for estimating the dependence of communication reliability in a shortwave radio-frequency transmission channel (SWRC) with a single discrete beam and diffuse wave scattering across small-scale ionospheric inhomogeneities on the selected operating frequency taking into account the given signal-to-noise ratio and ionospheric diffusivity. In this technique, the Nakagami m-distribution is used to describe interference fading of the received signal. However, in a single-beam SWRC, fading signal amplitudes are described by the Rician or generalized Rayleigh, rather than by Nakagami, distribution in 90 % of all cases. At the same time, the results obtained using the Nakagami distribution to approximate fading and to assess its effect on communication quality agrees well with those obtained by the Rician distribution only in two cases: the presence of Rayleigh distribution or the complete absence of fading.Aim. To develop a methodology for estimating communication reliability in a single-beam SWRC with Rician fading and to compare its results with that under Nakagami fading.Materials and methods. The effect of operating frequency and ionospheric diffusivity on fading distribution parameters in a single-beam SWRC was estimated by simulating transionospheric communication channels based on a radio-physical phase screen method. The effect of Rician fading parameters on communication reliability was simulated in the MatLab environment. The initial data on ionospheric parameters were obtained using the IRI-2016 model.Results. A three-stage methodology for estimating communication reliability in a single-beam SWRC with Rician fading was developed; its results were compared with that under Nakagami fading. Dependencies were obtained to describe communication reliability in a single-beam SWRC during the day and at night on the selected operating frequency relative to the maximum applicable frequency and on the level of ionospheric diffusivity during Rician and Nakagami fading.Conclusion. The conducted analysis showed that, at different levels of ionospheric diffusivity, communication reliability in a single-beam SWRC with Nakagami fading can be significantly overestimated (up to 12 %), compared to that under Rician fading.Π’Π²Π΅Π΄Π΅Π½ΠΈΠ΅. Π˜Π·Π²Π΅ΡΡ‚Π½Π° ΠΌΠ΅Ρ‚ΠΎΠ΄ΠΈΠΊΠ° ΠΎΡ†Π΅Π½ΠΊΠΈ зависимости надСТности связи Π² ΠΊΠΎΡ€ΠΎΡ‚ΠΊΠΎΠ²ΠΎΠ»Π½ΠΎΠ²ΠΎΠΉ (ΠšΠ’) Ρ€Π°Π΄ΠΈΠΎΠ»ΠΈΠ½ΠΈΠΈ с ΠΎΠ΄Π½ΠΈΠΌ дискрСтным Π»ΡƒΡ‡ΠΎΠΌ ΠΈ Π΄ΠΈΡ„Ρ„ΡƒΠ·Π½Ρ‹ΠΌ рассСяниСм Π²ΠΎΠ»Π½Ρ‹ Π½Π° ΠΌΠ΅Π»ΠΊΠΎΠΌΠ°ΡΡˆΡ‚Π°Π±Π½Ρ‹Ρ… нСоднородностях ионосфСры ΠΎΡ‚ Π²Ρ‹Π±ΠΎΡ€Π° Ρ€Π°Π±ΠΎΡ‡Π΅ΠΉ частоты с ΡƒΡ‡Π΅Ρ‚ΠΎΠΌ сигнально-ΠΏΠΎΠΌΠ΅Ρ…ΠΎΠ²ΠΎΠΉ обстановки ΠΈ уровня диффузности ионосфСры. Π’ Π΄Π°Π½Π½ΠΎΠΉ ΠΌΠ΅Ρ‚ΠΎΠ΄ΠΈΠΊΠ΅ для описания ΠΈΠ½Ρ‚Π΅Ρ€Ρ„Π΅Ρ€Π΅Π½Ρ†ΠΈΠΎΠ½Π½Ρ‹Ρ… Π·Π°ΠΌΠΈΡ€Π°Π½ΠΈΠΉ ΠΏΡ€ΠΈΠ½ΠΈΠΌΠ°Π΅ΠΌΠΎΠ³ΠΎ сигнала ΠΈΡΠΏΠΎΠ»ΡŒΠ·ΡƒΠ΅Ρ‚ΡΡ m-распрСдСлСниС Накагами. Однако Π² ΠšΠ’ ΠΎΠ΄Π½ΠΎΠ»ΡƒΡ‡Π΅Π²ΠΎΠΉ Ρ€Π°Π΄ΠΈΠΎΠ»ΠΈΠ½ΠΈΠΈ замирания Π°ΠΌΠΏΠ»ΠΈΡ‚ΡƒΠ΄Ρ‹ сигнала Π² 90 % всСх случаСв ΠΎΠΏΠΈΡΡ‹Π²Π°ΡŽΡ‚ΡΡ распрСдСлСниСм Π½Π΅ Накагами, Π° Райса, ΠΈΠ»ΠΈ ΠΎΠ±ΠΎΠ±Ρ‰Π΅Π½Π½Ρ‹ΠΌ распрСдСлСниСм РэлСя. ΠŸΡ€ΠΈ этом ΠΏΡ€ΠΈΠΌΠ΅Π½Π΅Π½ΠΈΠ΅ распрСдСлСния Накагами для аппроксимации Π·Π°ΠΌΠΈΡ€Π°Π½ΠΈΠΉ ΠΈ Π°Π½Π°Π»ΠΈΠ·Π° ΠΈΡ… влияния Π½Π° качСство связи Π΄Π°Π΅Ρ‚ Ρ…ΠΎΡ€ΠΎΡˆΠ΅Π΅ совпадСниС с распрСдСлСниСм Райса Ρ‚ΠΎΠ»ΡŒΠΊΠΎ Π² Π΄Π²ΡƒΡ… частных случаях: распрСдСлСния РэлСя ΠΈ ΠΏΠΎΠ»Π½ΠΎΠ³ΠΎ отсутствия Π·Π°ΠΌΠΈΡ€Π°Π½ΠΈΠΉ.ЦСль Ρ€Π°Π±ΠΎΡ‚Ρ‹. Π Π°Π·Ρ€Π°Π±ΠΎΡ‚Π°Ρ‚ΡŒ ΠΌΠ΅Ρ‚ΠΎΠ΄ΠΈΠΊΡƒ ΠΎΡ†Π΅Π½ΠΊΠΈ надСТности связи Π² ΠΎΠ΄Π½ΠΎΠ»ΡƒΡ‡Π΅Π²ΠΎΠΉ ΠΊΠΎΡ€ΠΎΡ‚ΠΊΠΎΠ²ΠΎΠ»Π½ΠΎΠ²ΠΎΠΉ Ρ€Π°Π΄ΠΈΠΎΠ»ΠΈΠ½ΠΈΠΈ с райсовскими замираниями ΠΈ ΡΡ€Π°Π²Π½ΠΈΡ‚ΡŒ Π΅Π΅ Ρ€Π΅Π·ΡƒΠ»ΡŒΡ‚Π°Ρ‚Ρ‹ с Π½Π°Π΄Π΅ΠΆΠ½ΠΎΡΡ‚ΡŒΡŽ связи ΠΏΡ€ΠΈ замираниях Накагами.ΠœΠ°Ρ‚Π΅Ρ€ΠΈΠ°Π»Ρ‹ ΠΈ ΠΌΠ΅Ρ‚ΠΎΠ΄Ρ‹. Для ΠΎΡ†Π΅Π½ΠΊΠΈ влияния Ρ€Π°Π±ΠΎΡ‡Π΅ΠΉ частоты ΠΈ диффузности ионосфСры Π½Π° ΠΏΠ°Ρ€Π°ΠΌΠ΅Ρ‚Ρ€Ρ‹ распрСдСлСния Π·Π°ΠΌΠΈΡ€Π°Π½ΠΈΠΉ Π² ΠΎΠ΄Π½ΠΎΠ»ΡƒΡ‡Π΅Π²ΠΎΠΉ ΠšΠ’-Ρ€Π°Π΄ΠΈΠΎΠ»ΠΈΠ½ΠΈΠΈ использовались ΠΌΠ΅Ρ‚ΠΎΠ΄Ρ‹ модСлирования трансионосфСрных ΠΊΠ°Π½Π°Π»ΠΎΠ² связи Π½Π° основС радиофизичСского ΠΌΠ΅Ρ‚ΠΎΠ΄Π° Ρ„Π°Π·ΠΎΠ²ΠΎΠ³ΠΎ экрана. Для ΠΎΡ†Π΅Π½ΠΊΠΈ влияния ΠΏΠ°Ρ€Π°ΠΌΠ΅Ρ‚Ρ€ΠΎΠ² Π·Π°ΠΌΠΈΡ€Π°Π½ΠΈΠΉ с распрСдСлСниСм Райса Π½Π° Π½Π°Π΄Π΅ΠΆΠ½ΠΎΡΡ‚ΡŒ ΠšΠ’-связи использовалась срСда MatLab. Π˜ΡΡ…ΠΎΠ΄Π½Ρ‹Π΅ Π΄Π°Π½Π½Ρ‹Π΅ ΠΎ ΠΏΠ°Ρ€Π°ΠΌΠ΅Ρ‚Ρ€Π°Ρ… ионосфСры ΠΏΠΎΠ»ΡƒΡ‡Π΅Π½Ρ‹ с использованиСм ΠΌΠΎΠ΄Π΅Π»ΠΈ IRI-2016.Π Π΅Π·ΡƒΠ»ΡŒΡ‚Π°Ρ‚Ρ‹. Π Π°Π·Ρ€Π°Π±ΠΎΡ‚Π°Π½Π° 3-этапная ΠΌΠ΅Ρ‚ΠΎΠ΄ΠΈΠΊΠ° ΠΎΡ†Π΅Π½ΠΊΠΈ надСТности связи Π² ΠΎΠ΄Π½ΠΎΠ»ΡƒΡ‡Π΅Π²ΠΎΠΉ ΠšΠ’-Ρ€Π°Π΄ΠΈΠΎΠ»ΠΈΠ½ΠΈΠΈ с райсовскими замираниями ΠΈ осущСствлСно сравнСниС Π΅Π΅ Ρ€Π΅Π·ΡƒΠ»ΡŒΡ‚Π°Ρ‚ΠΎΠ² с Π½Π°Π΄Π΅ΠΆΠ½ΠΎΡΡ‚ΡŒΡŽ связи ΠΏΡ€ΠΈ замираниях Накагами. ΠŸΠΎΠ»ΡƒΡ‡Π΅Π½Ρ‹ зависимости надСТности связи Π² ΠΎΠ΄Π½ΠΎΠ»ΡƒΡ‡Π΅Π²ΠΎΠΉ ΠšΠ’-Ρ€Π°Π΄ΠΈΠΎΠ»ΠΈΠ½ΠΈΠΈ Π½ΠΎΡ‡ΡŒΡŽ ΠΈ Π΄Π½Π΅ΠΌ ΠΎΡ‚ Π²Ρ‹Π±ΠΎΡ€Π° Ρ€Π°Π±ΠΎΡ‡Π΅ΠΉ частоты ΠΎΡ‚Π½ΠΎΡΠΈΡ‚Π΅Π»ΡŒΠ½ΠΎ максимально ΠΏΡ€ΠΈΠΌΠ΅Π½ΠΈΠΌΠΎΠΉ частоты ΠΈ ΠΎΡ‚ уровня диффузности ионосфСры ΠΏΡ€ΠΈ замираниях Райса ΠΈ Накагами.Π—Π°ΠΊΠ»ΡŽΡ‡Π΅Π½ΠΈΠ΅. Анализ ΠΏΠΎΠ»ΡƒΡ‡Π΅Π½Π½Ρ‹Ρ… Ρ€Π΅Π·ΡƒΠ»ΡŒΡ‚Π°Ρ‚ΠΎΠ² ΠΏΠΎΠΊΠ°Π·Ρ‹Π²Π°Π΅Ρ‚, Ρ‡Ρ‚ΠΎ ΠΏΡ€ΠΈ Ρ€Π°Π·Π»ΠΈΡ‡Π½ΠΎΠΌ ΡƒΡ€ΠΎΠ²Π½Π΅ диффузности ионосфСры Π½Π°Π΄Π΅ΠΆΠ½ΠΎΡΡ‚ΡŒ связи Π² ΠΎΠ΄Π½ΠΎΠ»ΡƒΡ‡Π΅Π²ΠΎΠΉ ΠšΠ’-Ρ€Π°Π΄ΠΈΠΎΠ»ΠΈΠ½ΠΈΠΈ с замираниями Накагами ΠΌΠΎΠΆΠ΅Ρ‚ Π±Ρ‹Ρ‚ΡŒ сущСствСнно Π·Π°Π²Ρ‹ΡˆΠ΅Π½Π° (Π΄ΠΎ 12 %) ΠΏΠΎ ΡΡ€Π°Π²Π½Π΅Π½ΠΈΡŽ с замираниями Райса

    Estimation of noise error when measuring virtual height during diffusivity of ionospheric F layer

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    It is shown that during diffusivity of ionosphere its bandwidth of coherence may shrink to hundreds of hertz. Frequency-selective fading appears in these cases and the noise error when measuring ionospheric virtual height increases by 1–2 orders if compared to the normal ionospheric conditions

    Estimation of noise error when measuring virtual height during diffusivity of ionospheric F layer

    No full text
    It is shown that during diffusivity of ionosphere its bandwidth of coherence may shrink to hundreds of hertz. Frequency-selective fading appears in these cases and the noise error when measuring ionospheric virtual height increases by 1–2 orders if compared to the normal ionospheric conditions
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