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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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10.2 Space-Time Signal Representation 465where n is the pulse index, and the factor <strong>of</strong> two accounts for two-way range; as in thespatial case, τ n is simply distance divided by the velocity <strong>of</strong> propagation.As a result <strong>of</strong> the time-varying change in range, a pulse-to-pulse phase rotation occursleading to a Doppler frequency <strong>of</strong>fset. The phase for the n-th pulse is[ ]ro + nrφ n = τ n ω c = 4πλ o(10.29)This expression neglects bandwidth-related dispersion. Since radian frequency is the timederivative <strong>of</strong> phase, the corresponding Doppler frequency isf d = 1 dφ n2π dt= 2rλ o t = 2v rλ o. (10.30)v r denotes the radial velocity component, sometimes also called line-<strong>of</strong>-sight velocity orrange rate. Equation (10.30) indicates that motion along a radial line between radar andtarget leads to the Doppler frequency <strong>of</strong>fset.The resulting temporal snapshot (temporal signal vector) corresponding to a pointscatterer with normalized Doppler ˜f d = f d T is x t = a t s t ( ˜f d ), where a t is the signalcomplex envelope (taken as perfectly correlated over the coherent dwell) ands t ( ˜f d ) = [ 1 e j2π ˜f de j2π(2 ˜f d )··· e j2π(N−1) ˜f d] T(10.31)s t ( ˜f d ) is known as the temporal steering vector. Comparing (10.31) and (10.19), we finda mathematical similarity between spatial and temporal responses after writing (10.19) ass s ( f sp ) = ā [ 1 e j2π f spe j2π(2 f sp)··· e j2π(M−2) f spe j2π(M−1) f sp ] T(10.32)where ā is a complex scalar. For this reason, the collection <strong>of</strong> N receive pulses is sometimescalled the temporal aperture.Based on this similarity between spatial and temporal responses, we find by analogyto our discussion <strong>of</strong> the spatial matched filter in Section 10.2.1 that the temporal matchedfilter requires the weight vector w t = s t ( ˜f d ). It is common to apply a real-valued weightingfunction to tailor the sidelobe response at the expense <strong>of</strong> broadened main lobe and loss <strong>of</strong>integration gain: w t = b t ⊙ s t ( ˜f d ), where b t is a real-valued function, such as a Hanningor Chebyshev weighting.Spatial or temporal matched filtering operations are coherent. The matched filteradjusts the phase <strong>of</strong> each sample and then sums the individual voltages. Referring to thecollection <strong>of</strong> N pulses as the coherent processing interval (CPI)—common in MTI radarparlance—emphasizes this notion.The temporal or spatial steering vectors in (10.31)–(10.32) assume a Vandermondestructure: each consecutive element <strong>of</strong> the vector is a multiple <strong>of</strong> the preceding term,increased by a single integer. This structure characterizes a linear phase ramp across thesampled aperture; the slope <strong>of</strong> the phase ramp corresponds to the particular frequency.Employing a fast Fourier transform (FFT) [9] enables the processor to efficiently testfor the various phase ramp slopes, thereby accomplishing matched filtering. A weightingfunction is directly applied to the data in this instance. Straddle loss—the loss in SNRdue to a mismatched filter response—occurs in practice since the precise target spatial orDoppler frequency is generally unknown. The difference between the precise linear phase

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