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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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216 CHAPTER 6 Spotlight Synthetic Aperture <strong>Radar</strong>TABLE 6-1 Properties <strong>of</strong> the Fourier Transform Commonly Used in SAR Imaging. The double arrowsymbol ⇔ is used to indicate that two functions are related via the Fourier transform.Property Description Application to SARLinearity af(t) + bg(t) ⇔ aF(ω) + bG(ω), Superposition <strong>of</strong> scatterers in an imagewhere a and b are constantsTime scaling f (at) ⇔ |a| 1 a )Deramp scaling <strong>of</strong> range axisTime shifting f (t − t 0 ) ⇔ F(ω)e − jωt 0Displacement <strong>of</strong> scatterer from scene centerFrequency shifting e jω0t f (t) ⇔ F(ω − ω 0 ) Modulation and basebandingArea under F(ω) f (0) = ∫ +∞−∞ F(ω)dωPeak value <strong>of</strong> point scatterer responseMultiplication/convolution f (t) ∗ g(t) ⇔ F(ω)G(ω) Spectral windowing; phase error effecton point scatterer responseCorrelation f (t)⋆g(t) ⇔ F(ω)G ∗ (ω) Matched filtering, or pulse compressionIn this case, the Fourier transform integral is easy to write, as the rect function simplyalters the limits <strong>of</strong> integration <strong>of</strong> (6.1), where f (t) = 1:F(ω) =∫ T/2−T/2Next, we carry out the integral and evaluate it at the limits:∫ T/2e − jωt jωtT/2e− dt = − jω ∣−T/2=−T/2(cos ω T 2)− j sin( ) ωsin2 T = T ω2 T( ) T= T sinc2π ωe − jωt dt (6.5)(ω T ) (− cos ω T ) (− j sin ω T )222− jω(6.6)The last line <strong>of</strong> this expression is the sinc function, which is defined as sinc(x) =sin(π x)/π x. The word sinc is a contraction <strong>of</strong> the Latin term sinus cardinalis, or cardinalsine. The derivation above begins with a rect function in the time domain and obtains asinc function in the frequency domain. These domains are commonly reversed in radarengineering. The rect function is <strong>of</strong>ten used to represent the constant-amplitude spectrum<strong>of</strong> a transmitted signal. After pulse compression (see the correlation property in Table 6-1as well as Chapter 2), the spectrum is real-valued. Thus, the signal in the time domain isthe sinc function determined by the relationship:( ) ωrect ⇔ 2π Bsinc(Bt) (6.7)2π Bwhere B is the bandwidth <strong>of</strong> the transmitted signal (in Hz, not rad/s).Figure 6-1 plots the sinc function for several values <strong>of</strong> B, and we notice two things:First, the maximum value <strong>of</strong> the sinc function is equal to 2π B as implied by (6.7). This

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