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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 63where M ≥ N. This is equivalent to evaluating the response at equally spaced rangesdefined byR k =Inserting equation (2.119) into (2.113) yields the DFTck k = 0,...,(M − 1) (2.120)2f MX (k) =N−1∑n=0(x (n) exp − j 2πk )M nM ≥ N (2.121)which is <strong>of</strong>ten implemented using an FFT for computational efficiency. For a point targetlocated at range R 0 , the compressed response is a sampled instantiation <strong>of</strong> the digital sincin (2.114) or|X (k)| =∣sin( Nsin2( ))2πM k − ω R 0 (( )/ )2πM k − ω R 02∣k = 0,...,(M − 1) (2.122)The DFT is a linear operator; thus, the range pr<strong>of</strong>ile associated with multiple scatterers issimply the superposition <strong>of</strong> the individual responses.Zero padding is <strong>of</strong>ten used in conjunction with a DFT to decrease the filter spacing,which reduces straddle loss. For M > N, the sequence is said to be zero padded withM − N zeros. For M = N, the filters or range bins are spaced by the nominal waveformresolution c/2Nf .2.5.4.3 Range Sidelobe SuppressionRange sidelobes associated with large RCS targets may mask the presence <strong>of</strong> smallertargets. As noted in Figure 2-24, sidelobes are suppressed by applying an amplitudeweighting to the complex samples collected at a range gate. When selecting an amplitudetaper, the associated reduction in resolution and loss in SNR should be taken intoaccount [36].2.5.5 Straddle Loss and Range AmbiguitiesThe range pr<strong>of</strong>ile generated by an SF waveform may exhibit undesired artifacts as a result<strong>of</strong> ambiguities and straddle loss. The following sections examine these issues and theimpact <strong>of</strong> waveform parameter selection on performance.2.5.5.1 Straddle LossStraddle loss is introduced at two points in the processing chain: (1) when sampling thepulse’s match filtered response; and (2) within the DFT. The loss associated with the DFTwas discussed in Section 2.5.4.2. The loss associated with sampling is examined in thissection. When sampling the return from a pulse, the resultant straddle loss is a function<strong>of</strong> the range gate spacing and the single-pulse bandwidth or range resolution. Severalexamples are provided to illustrate the loss.In a radar system, range gates are <strong>of</strong>ten spaced by the transmit pulse’s range resolution.A similar spacing may be applied to a stepped frequency waveform where the range gates

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