Distortion radar signal modelling method under time-varying plasma sheath
A plasma sheath and radar signal technology, which is applied in the field of modeling of distorted radar signals under the ion sheath, can solve the problems that the description of the radar signal cannot be distorted, and it is difficult to reflect the influence of the time-varying plasma sheath on the modulation of the radar signal.
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Embodiment 1
[0026] At present, relevant research on radar signals without plasma sheaths and single-frequency signals under steady-state plasma sheaths already exists. The modulation effect of the radar is complicated, and the existing relevant research cannot accurately analyze the influence of the time-varying plasma sheath on the distorted radar signal. The present invention researches and discusses the modeling method of the distorted radar signal under the time-varying plasma sheath. The invention aims at theoretically modeling the distorted radar signal under the time-varying plasma sheath, and determines the modulation influence on the amplitude and phase of the distorted radar signal from the real part and the imaginary part of the transmission coefficient of the time-varying plasma sheath.
[0027] The present invention is a radar signal modeling method under a time-varying plasma sheath, see figure 1 , the radar signal modeling method under the time-varying plasma sheath include...
Embodiment 2
[0042] The modeling method of the distorted radar signal under the time-varying plasma sheath is the same as in Embodiment 1, and the calculation in step S2 obtains the time-varying plasma sheath transmission coefficient T dyn (t,f 0 ), including the following steps:
[0043] 2.1) Calculate the time-varying plasma characteristic frequency ω of the mth layer p (t,z m ): input electron mass m e , the time-varying plasma sheath electron density model Ne calculated by step S1 dyn (z,t), determine the time-varying plasma characteristic frequency ω of the mth layer p (t,z m ), the time-varying plasma characteristic frequency of the mth layer, specifically expressed as follows:
[0044]
[0045] 2.2) Calculate the time-varying plasma sheath complex permittivity ε(t,z m , f 0 ): Input the time-varying electron collision frequency v of the plasma sheath en , using the time-varying plasma sheath electron density model Ne dyn (z,t), from the time-varying plasma sheath charac...
Embodiment 3
[0056] The modeling method of the distorted radar signal under the time-varying plasma sheath is the same as in Embodiment 1-2, and the calculation of the distorted signal model formed by the radar signal passing through the time-varying plasma sheath described in step S3 includes the following steps:
[0057] 3.1) Input chirp radar signal S(t): input radar signal carrier frequency f 0 , radar signal amplitude A, radar signal modulation frequency k and radar signal pulse width T P , to determine the chirp signal radar model S(t):
[0058]
[0059] 3.2) Determine the distortion radar signal model R dyn (t): the amplitude of the transmission coefficient of the time-varying plasma sheath|T dyn (t,f 0 )| and phase φ(t,f 0 ) and the chirp signal radar model S(t), jointly determine the distorted radar signal R dyn (t), that is, the distortion radar signal model R dyn (t).
[0060] Based on the determination of the distorted radar signal, the present invention can find the ...
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