9 research outputs found
Probability of erroneous reception of navigational radio signals under ionospheric disturbances
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
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
ΠΠ΅ΡΠΎΠ΄ΠΈΠΊΠ° ΠΎΡΠ΅Π½ΠΊΠΈ Π½Π°Π΄Π΅ΠΆΠ½ΠΎΡΡΠΈ ΡΠ²ΡΠ·ΠΈ Π² ΠΊΠΎΡΠΎΡΠΊΠΎΠ²ΠΎΠ»Π½ΠΎΠ²ΠΎΠΉ ΡΠ°Π΄ΠΈΠΎΠ»ΠΈΠ½ΠΈΠΈ Ρ ΡΠ°ΠΉΡΠΎΠ²ΡΠΊΠΈΠΌΠΈ Π·Π°ΠΌΠΈΡΠ°Π½ΠΈΡΠΌΠΈ Ρ ΡΡΠ΅ΡΠΎΠΌ Π΄ΠΈΡΡΡΠ·Π½ΠΎΡΡΠΈ ΠΈΠΎΠ½ΠΎΡΡΠ΅ΡΡ
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.ΠΠ²Π΅Π΄Π΅Π½ΠΈΠ΅. ΠΠ·Π²Π΅ΡΡΠ½Π° ΠΌΠ΅ΡΠΎΠ΄ΠΈΠΊΠ° ΠΎΡΠ΅Π½ΠΊΠΈ Π·Π°Π²ΠΈΡΠΈΠΌΠΎΡΡΠΈ Π½Π°Π΄Π΅ΠΆΠ½ΠΎΡΡΠΈ ΡΠ²ΡΠ·ΠΈ Π² ΠΊΠΎΡΠΎΡΠΊΠΎΠ²ΠΎΠ»Π½ΠΎΠ²ΠΎΠΉ (ΠΠ) ΡΠ°Π΄ΠΈΠΎΠ»ΠΈΠ½ΠΈΠΈ Ρ ΠΎΠ΄Π½ΠΈΠΌ Π΄ΠΈΡΠΊΡΠ΅ΡΠ½ΡΠΌ Π»ΡΡΠΎΠΌ ΠΈ Π΄ΠΈΡΡΡΠ·Π½ΡΠΌ ΡΠ°ΡΡΠ΅ΡΠ½ΠΈΠ΅ΠΌ Π²ΠΎΠ»Π½Ρ Π½Π° ΠΌΠ΅Π»ΠΊΠΎΠΌΠ°ΡΡΡΠ°Π±Π½ΡΡ
Π½Π΅ΠΎΠ΄Π½ΠΎΡΠΎΠ΄Π½ΠΎΡΡΡΡ
ΠΈΠΎΠ½ΠΎΡΡΠ΅ΡΡ ΠΎΡ Π²ΡΠ±ΠΎΡΠ° ΡΠ°Π±ΠΎΡΠ΅ΠΉ ΡΠ°ΡΡΠΎΡΡ Ρ ΡΡΠ΅ΡΠΎΠΌ ΡΠΈΠ³Π½Π°Π»ΡΠ½ΠΎ-ΠΏΠΎΠΌΠ΅Ρ
ΠΎΠ²ΠΎΠΉ ΠΎΠ±ΡΡΠ°Π½ΠΎΠ²ΠΊΠΈ ΠΈ ΡΡΠΎΠ²Π½Ρ Π΄ΠΈΡΡΡΠ·Π½ΠΎΡΡΠΈ ΠΈΠΎΠ½ΠΎΡΡΠ΅ΡΡ. Π Π΄Π°Π½Π½ΠΎΠΉ ΠΌΠ΅ΡΠΎΠ΄ΠΈΠΊΠ΅ Π΄Π»Ρ ΠΎΠΏΠΈΡΠ°Π½ΠΈΡ ΠΈΠ½ΡΠ΅ΡΡΠ΅ΡΠ΅Π½ΡΠΈΠΎΠ½Π½ΡΡ
Π·Π°ΠΌΠΈΡΠ°Π½ΠΈΠΉ ΠΏΡΠΈΠ½ΠΈΠΌΠ°Π΅ΠΌΠΎΠ³ΠΎ ΡΠΈΠ³Π½Π°Π»Π° ΠΈΡΠΏΠΎΠ»ΡΠ·ΡΠ΅ΡΡΡ m-ΡΠ°ΡΠΏΡΠ΅Π΄Π΅Π»Π΅Π½ΠΈΠ΅ ΠΠ°ΠΊΠ°Π³Π°ΠΌΠΈ. ΠΠ΄Π½Π°ΠΊΠΎ Π² ΠΠ ΠΎΠ΄Π½ΠΎΠ»ΡΡΠ΅Π²ΠΎΠΉ ΡΠ°Π΄ΠΈΠΎΠ»ΠΈΠ½ΠΈΠΈ Π·Π°ΠΌΠΈΡΠ°Π½ΠΈΡ Π°ΠΌΠΏΠ»ΠΈΡΡΠ΄Ρ ΡΠΈΠ³Π½Π°Π»Π° Π² 90 % Π²ΡΠ΅Ρ
ΡΠ»ΡΡΠ°Π΅Π² ΠΎΠΏΠΈΡΡΠ²Π°ΡΡΡΡ ΡΠ°ΡΠΏΡΠ΅Π΄Π΅Π»Π΅Π½ΠΈΠ΅ΠΌ Π½Π΅ ΠΠ°ΠΊΠ°Π³Π°ΠΌΠΈ, Π° Π Π°ΠΉΡΠ°, ΠΈΠ»ΠΈ ΠΎΠ±ΠΎΠ±ΡΠ΅Π½Π½ΡΠΌ ΡΠ°ΡΠΏΡΠ΅Π΄Π΅Π»Π΅Π½ΠΈΠ΅ΠΌ Π ΡΠ»Π΅Ρ. ΠΡΠΈ ΡΡΠΎΠΌ ΠΏΡΠΈΠΌΠ΅Π½Π΅Π½ΠΈΠ΅ ΡΠ°ΡΠΏΡΠ΅Π΄Π΅Π»Π΅Π½ΠΈΡ ΠΠ°ΠΊΠ°Π³Π°ΠΌΠΈ Π΄Π»Ρ Π°ΠΏΠΏΡΠΎΠΊΡΠΈΠΌΠ°ΡΠΈΠΈ Π·Π°ΠΌΠΈΡΠ°Π½ΠΈΠΉ ΠΈ Π°Π½Π°Π»ΠΈΠ·Π° ΠΈΡ
Π²Π»ΠΈΡΠ½ΠΈΡ Π½Π° ΠΊΠ°ΡΠ΅ΡΡΠ²ΠΎ ΡΠ²ΡΠ·ΠΈ Π΄Π°Π΅Ρ Ρ
ΠΎΡΠΎΡΠ΅Π΅ ΡΠΎΠ²ΠΏΠ°Π΄Π΅Π½ΠΈΠ΅ Ρ ΡΠ°ΡΠΏΡΠ΅Π΄Π΅Π»Π΅Π½ΠΈΠ΅ΠΌ Π Π°ΠΉΡΠ° ΡΠΎΠ»ΡΠΊΠΎ Π² Π΄Π²ΡΡ
ΡΠ°ΡΡΠ½ΡΡ
ΡΠ»ΡΡΠ°ΡΡ
: ΡΠ°ΡΠΏΡΠ΅Π΄Π΅Π»Π΅Π½ΠΈΡ Π ΡΠ»Π΅Ρ ΠΈ ΠΏΠΎΠ»Π½ΠΎΠ³ΠΎ ΠΎΡΡΡΡΡΡΠ²ΠΈΡ Π·Π°ΠΌΠΈΡΠ°Π½ΠΈΠΉ.Π¦Π΅Π»Ρ ΡΠ°Π±ΠΎΡΡ. Π Π°Π·ΡΠ°Π±ΠΎΡΠ°ΡΡ ΠΌΠ΅ΡΠΎΠ΄ΠΈΠΊΡ ΠΎΡΠ΅Π½ΠΊΠΈ Π½Π°Π΄Π΅ΠΆΠ½ΠΎΡΡΠΈ ΡΠ²ΡΠ·ΠΈ Π² ΠΎΠ΄Π½ΠΎΠ»ΡΡΠ΅Π²ΠΎΠΉ ΠΊΠΎΡΠΎΡΠΊΠΎΠ²ΠΎΠ»Π½ΠΎΠ²ΠΎΠΉ ΡΠ°Π΄ΠΈΠΎΠ»ΠΈΠ½ΠΈΠΈ Ρ ΡΠ°ΠΉΡΠΎΠ²ΡΠΊΠΈΠΌΠΈ Π·Π°ΠΌΠΈΡΠ°Π½ΠΈΡΠΌΠΈ ΠΈ ΡΡΠ°Π²Π½ΠΈΡΡ Π΅Π΅ ΡΠ΅Π·ΡΠ»ΡΡΠ°ΡΡ Ρ Π½Π°Π΄Π΅ΠΆΠ½ΠΎΡΡΡΡ ΡΠ²ΡΠ·ΠΈ ΠΏΡΠΈ Π·Π°ΠΌΠΈΡΠ°Π½ΠΈΡΡ
ΠΠ°ΠΊΠ°Π³Π°ΠΌΠΈ.ΠΠ°ΡΠ΅ΡΠΈΠ°Π»Ρ ΠΈ ΠΌΠ΅ΡΠΎΠ΄Ρ. ΠΠ»Ρ ΠΎΡΠ΅Π½ΠΊΠΈ Π²Π»ΠΈΡΠ½ΠΈΡ ΡΠ°Π±ΠΎΡΠ΅ΠΉ ΡΠ°ΡΡΠΎΡΡ ΠΈ Π΄ΠΈΡΡΡΠ·Π½ΠΎΡΡΠΈ ΠΈΠΎΠ½ΠΎΡΡΠ΅ΡΡ Π½Π° ΠΏΠ°ΡΠ°ΠΌΠ΅ΡΡΡ ΡΠ°ΡΠΏΡΠ΅Π΄Π΅Π»Π΅Π½ΠΈΡ Π·Π°ΠΌΠΈΡΠ°Π½ΠΈΠΉ Π² ΠΎΠ΄Π½ΠΎΠ»ΡΡΠ΅Π²ΠΎΠΉ ΠΠ-ΡΠ°Π΄ΠΈΠΎΠ»ΠΈΠ½ΠΈΠΈ ΠΈΡΠΏΠΎΠ»ΡΠ·ΠΎΠ²Π°Π»ΠΈΡΡ ΠΌΠ΅ΡΠΎΠ΄Ρ ΠΌΠΎΠ΄Π΅Π»ΠΈΡΠΎΠ²Π°Π½ΠΈΡ ΡΡΠ°Π½ΡΠΈΠΎΠ½ΠΎΡΡΠ΅ΡΠ½ΡΡ
ΠΊΠ°Π½Π°Π»ΠΎΠ² ΡΠ²ΡΠ·ΠΈ Π½Π° ΠΎΡΠ½ΠΎΠ²Π΅ ΡΠ°Π΄ΠΈΠΎΡΠΈΠ·ΠΈΡΠ΅ΡΠΊΠΎΠ³ΠΎ ΠΌΠ΅ΡΠΎΠ΄Π° ΡΠ°Π·ΠΎΠ²ΠΎΠ³ΠΎ ΡΠΊΡΠ°Π½Π°. ΠΠ»Ρ ΠΎΡΠ΅Π½ΠΊΠΈ Π²Π»ΠΈΡΠ½ΠΈΡ ΠΏΠ°ΡΠ°ΠΌΠ΅ΡΡΠΎΠ² Π·Π°ΠΌΠΈΡΠ°Π½ΠΈΠΉ Ρ ΡΠ°ΡΠΏΡΠ΅Π΄Π΅Π»Π΅Π½ΠΈΠ΅ΠΌ Π Π°ΠΉΡΠ° Π½Π° Π½Π°Π΄Π΅ΠΆΠ½ΠΎΡΡΡ ΠΠ-ΡΠ²ΡΠ·ΠΈ ΠΈΡΠΏΠΎΠ»ΡΠ·ΠΎΠ²Π°Π»Π°ΡΡ ΡΡΠ΅Π΄Π° MatLab. ΠΡΡ
ΠΎΠ΄Π½ΡΠ΅ Π΄Π°Π½Π½ΡΠ΅ ΠΎ ΠΏΠ°ΡΠ°ΠΌΠ΅ΡΡΠ°Ρ
ΠΈΠΎΠ½ΠΎΡΡΠ΅ΡΡ ΠΏΠΎΠ»ΡΡΠ΅Π½Ρ Ρ ΠΈΡΠΏΠΎΠ»ΡΠ·ΠΎΠ²Π°Π½ΠΈΠ΅ΠΌ ΠΌΠΎΠ΄Π΅Π»ΠΈ IRI-2016.Π Π΅Π·ΡΠ»ΡΡΠ°ΡΡ. Π Π°Π·ΡΠ°Π±ΠΎΡΠ°Π½Π° 3-ΡΡΠ°ΠΏΠ½Π°Ρ ΠΌΠ΅ΡΠΎΠ΄ΠΈΠΊΠ° ΠΎΡΠ΅Π½ΠΊΠΈ Π½Π°Π΄Π΅ΠΆΠ½ΠΎΡΡΠΈ ΡΠ²ΡΠ·ΠΈ Π² ΠΎΠ΄Π½ΠΎΠ»ΡΡΠ΅Π²ΠΎΠΉ ΠΠ-ΡΠ°Π΄ΠΈΠΎΠ»ΠΈΠ½ΠΈΠΈ Ρ ΡΠ°ΠΉΡΠΎΠ²ΡΠΊΠΈΠΌΠΈ Π·Π°ΠΌΠΈΡΠ°Π½ΠΈΡΠΌΠΈ ΠΈ ΠΎΡΡΡΠ΅ΡΡΠ²Π»Π΅Π½ΠΎ ΡΡΠ°Π²Π½Π΅Π½ΠΈΠ΅ Π΅Π΅ ΡΠ΅Π·ΡΠ»ΡΡΠ°ΡΠΎΠ² Ρ Π½Π°Π΄Π΅ΠΆΠ½ΠΎΡΡΡΡ ΡΠ²ΡΠ·ΠΈ ΠΏΡΠΈ Π·Π°ΠΌΠΈΡΠ°Π½ΠΈΡΡ
ΠΠ°ΠΊΠ°Π³Π°ΠΌΠΈ. ΠΠΎΠ»ΡΡΠ΅Π½Ρ Π·Π°Π²ΠΈΡΠΈΠΌΠΎΡΡΠΈ Π½Π°Π΄Π΅ΠΆΠ½ΠΎΡΡΠΈ ΡΠ²ΡΠ·ΠΈ Π² ΠΎΠ΄Π½ΠΎΠ»ΡΡΠ΅Π²ΠΎΠΉ ΠΠ-ΡΠ°Π΄ΠΈΠΎΠ»ΠΈΠ½ΠΈΠΈ Π½ΠΎΡΡΡ ΠΈ Π΄Π½Π΅ΠΌ ΠΎΡ Π²ΡΠ±ΠΎΡΠ° ΡΠ°Π±ΠΎΡΠ΅ΠΉ ΡΠ°ΡΡΠΎΡΡ ΠΎΡΠ½ΠΎΡΠΈΡΠ΅Π»ΡΠ½ΠΎ ΠΌΠ°ΠΊΡΠΈΠΌΠ°Π»ΡΠ½ΠΎ ΠΏΡΠΈΠΌΠ΅Π½ΠΈΠΌΠΎΠΉ ΡΠ°ΡΡΠΎΡΡ ΠΈ ΠΎΡ ΡΡΠΎΠ²Π½Ρ Π΄ΠΈΡΡΡΠ·Π½ΠΎΡΡΠΈ ΠΈΠΎΠ½ΠΎΡΡΠ΅ΡΡ ΠΏΡΠΈ Π·Π°ΠΌΠΈΡΠ°Π½ΠΈΡΡ
Π Π°ΠΉΡΠ° ΠΈ ΠΠ°ΠΊΠ°Π³Π°ΠΌΠΈ.ΠΠ°ΠΊΠ»ΡΡΠ΅Π½ΠΈΠ΅. ΠΠ½Π°Π»ΠΈΠ· ΠΏΠΎΠ»ΡΡΠ΅Π½Π½ΡΡ
ΡΠ΅Π·ΡΠ»ΡΡΠ°ΡΠΎΠ² ΠΏΠΎΠΊΠ°Π·ΡΠ²Π°Π΅Ρ, ΡΡΠΎ ΠΏΡΠΈ ΡΠ°Π·Π»ΠΈΡΠ½ΠΎΠΌ ΡΡΠΎΠ²Π½Π΅ Π΄ΠΈΡΡΡΠ·Π½ΠΎΡΡΠΈ ΠΈΠΎΠ½ΠΎΡΡΠ΅ΡΡ Π½Π°Π΄Π΅ΠΆΠ½ΠΎΡΡΡ ΡΠ²ΡΠ·ΠΈ Π² ΠΎΠ΄Π½ΠΎΠ»ΡΡΠ΅Π²ΠΎΠΉ ΠΠ-ΡΠ°Π΄ΠΈΠΎΠ»ΠΈΠ½ΠΈΠΈ Ρ Π·Π°ΠΌΠΈΡΠ°Π½ΠΈΡΠΌΠΈ ΠΠ°ΠΊΠ°Π³Π°ΠΌΠΈ ΠΌΠΎΠΆΠ΅Ρ Π±ΡΡΡ ΡΡΡΠ΅ΡΡΠ²Π΅Π½Π½ΠΎ Π·Π°Π²ΡΡΠ΅Π½Π° (Π΄ΠΎ 12 %) ΠΏΠΎ ΡΡΠ°Π²Π½Π΅Π½ΠΈΡ Ρ Π·Π°ΠΌΠΈΡΠ°Π½ΠΈΡΠΌΠΈ Π Π°ΠΉΡΠ°
Estimation of noise error when measuring virtual height during diffusivity of ionospheric F layer
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 1β2 orders if compared to the normal ionospheric conditions
Estimation of noise error when measuring virtual height during diffusivity of ionospheric F layer
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 1β2 orders if compared to the normal ionospheric conditions