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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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2.5 Stepped Frequency Waveforms 61The first term to the right <strong>of</strong> the equal sign is a constant and is associated with the roundtripdelay and the initial transmit frequency. The second term is a complex phasor rotatingat a rate defined by the frequency step size and the range to the target. The phase rotationis similar to that observed when employing a pulsed Doppler waveform. To simply theexpressions, the amplitude <strong>of</strong> the return is set to unity.Fourier analysis is applied to the complex samples in equation (2.112) to extract thelocation <strong>of</strong> the return in range. Consider the DTFT defined byX (ω) =N−1∑n=0x (n) exp (− jωn) (2.113)where x (n) are the measured returns collected from N pulses, and ω is the digital frequencywith units <strong>of</strong> radians/sample. The DTFT represents a filter bank tuned over a continuum<strong>of</strong> frequencies (or rotation rates), which in this case correspond to different ranges.The samples are <strong>of</strong>ten viewed as being collected in the frequency domain, and thereturns are then transformed to the time (or range) domain. The frequency-domain interpretationis based on the assertion that each pulse is measuring the target’s response(amplitude and phase) at a different frequency. From this perspective, an inverse DTFTwould naturally be applied; however, it is the rotating phase induced by the change infrequency that is important. Either a forward or inverse DTFT may be applied as long asthe location <strong>of</strong> the scatterers (either up- or down-range) is correctly interpreted within thepr<strong>of</strong>ile, and the return is scaled to account for the DTFT integration gain.For a point target located at range R 0 , the output <strong>of</strong> the DTFT is a digital sinc definedby( N ( ) )sin ω − ωR0 |X (ω)| =2(( ))(2.114)ω − ωR0 ∣sin2 ∣where ω R0 = 2π 2R 0c f , ω = 2π 2R f , and R is a continuous variable representingcrange. Equation (2.114) represents the range compressed response. The term ω R0 centersthe response at a particular range or frequency. The shape <strong>of</strong> the compressed response isexamined by setting R 0 = 0or( )N sin|X (ω)| =2 ω ( )ω (2.115)∣ sin∣2A plot <strong>of</strong> the compressed response is shown in Figure 2-25. The response consists <strong>of</strong> a mainlobe and sidelobe structure with peak sidelobes 13.2 dB below the peak <strong>of</strong> the main lobe.The DTFT is periodic and repeats at multiples <strong>of</strong> 2π in ω; therefore, the range compressedresponse is also periodic with periodicities spaced by c/2f . An implication is that rangemeasured at the output <strong>of</strong> the DTFT is relative to the range gate and not absolute range.Absolute range is defined by the time delay to the range gate and the relative range <strong>of</strong>fsetwithin the pr<strong>of</strong>ile.

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