FIELD: physics.
SUBSTANCE: analysed radio signal is transmitted to the electrical input of an acousto-optic deflector where it is converted to an acoustic signal and then to an optical signal which then undergoes Fourier transformation with recording of its intensity distribution using an N-element line of photodiodes. Further, video signals are generated at outputs of said photodiodes, after which frequency of the radio signal is calculated, which matches the abscissa of the axis of symmetry of intensity distribution of the light signal which is discretised by the photodiodes. A threshold is set in the top part of the linear section of the amplitude characteristic of the photodiodes and the level of signals lower than thresholds on four photodiodes with levels closest to the threshold is determined. Further, signal levels on these photodiodes are denoted yA, yB, yC and yD, and frequencies corresponding to these levels are denoted fA, fB, fC and fD in ascending order of the frequencies. It is then ascertained that frequencies fA and fB are lower than the frequency of the signal limiting section formed by the threshold, and frequencies fC and fD - are higher. Further, signals on photodiodes are compared and if yA>yC, frequency f0 is calculated using the formula f0=(fC+fA-Δf1)/2, where Δf1=ΔF(yA-yC)/(yA-yB), otherwise frequency f0 is calculated using the formula f0=(fC+fA+Δf2)/2, where Δf2 =ΔF(yC-yA)/(yC-yD) where ΔF if the frequency interval between photodiodes.
EFFECT: method increases accuracy of measuring frequency of radio signals in strong signal mode.
6 dwg
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Authors
Dates
2011-06-20—Published
2009-02-11—Filed