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Principles of Modern Radar - Volume 2 1891121537

Principles of Modern Radar - Volume 2 1891121537

Principles of Modern Radar - Volume 2 1891121537

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464 CHAPTER 10 Clutter Suppression Using Space-Time Adaptive ProcessingFIGURE 10-3Spatial beampatternfor uniform andTaylor weightedULAs, includinginfluence <strong>of</strong> arrayerrors.3020Antenna Illumination PatternTaylor WeightingUniform WeightingTaylor Weighting, 0.5 dB/3° errorsdB100−10−200 5 10 15 20 25 30 35 40Azimuth Angle (Degrees)where L array is the array length in meters (substitute the array width into (10.26) forelevation beamwidth). The 3 dB beamwidth isB 3−dB = a swλ oL arraydegrees (10.27)a sw is a beam-broadening factor; typical values are in the range <strong>of</strong> 58 ≤ a sw ≤ 70 [1].10.2.2 Temporal Sampling and Doppler ProcessingMTI radar systems transmit and receive a sequence <strong>of</strong> N pulses as a means <strong>of</strong> temporallysampling the signal environment in the slow-time or Doppler dimension. The analog-todigitalconverters (ADCs) sample in the fast time, or range, dimension. The radar signalprocessor coherently combines the N pulses in a manner very similar to spatial beamforming;this operation is commonly called Doppler processing or Doppler beamforming.Doppler beamforming separates the target signal from stationary ground clutter returns atthe same angle and also enables estimation <strong>of</strong> target radial velocity.Consider a length-N periodic pulse train, with a pulse repetition interval (PRI) <strong>of</strong> T .Further assume the presence <strong>of</strong> a point scatterer, initially at range r o from the antenna phasecenter reference point. Due to the relative motion between the scatterer and radar platform,an interpulse change in range <strong>of</strong> r is present. The coherent dwell is kept sufficiently shortto maintain a constant radial velocity between radar and scatterer, so the interpulse changein range is constant-valued. With this in mind, the corresponding fast-time delay resultingfrom the motion between platform and scatterer isτ n = 2r o + n2rc(10.28)

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