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Passive, active, and digital filters (3ed., CRC, 2009) - tiera.ru

Passive, active, and digital filters (3ed., CRC, 2009) - tiera.ru

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18-8 <strong>Passive</strong>, Active, <strong>and</strong> Digital FiltersH(e jv ) ¼ 12pð p pH 0 d (e ju )W r (e j(v u) )du (18:37)where W r (e ju ) is the spect<strong>ru</strong>m of the rectangular window.Since the two functions in the integral are periodic, a circular convolution results <strong>and</strong> the limits ofintegration are taken over one period. Thus the frequency response H(e jv ) will be a ‘‘smeared’’ version ofthe desired response H 0 d (e jv ) <strong>and</strong> the discontinuities in the desired frequency response become transitionb<strong>and</strong>s of H(e jv ). To underst<strong>and</strong> this, it is inst<strong>ru</strong>ctive to examine the frequency response for the causalrectangular window, that is,W r (e jvT ) ¼ XN 1e jvnTn¼0¼ e jv(N1)T=2 sin (vNT=2)sin (vT=2)(18:38)The spect<strong>ru</strong>m W r (e jvT ) for N ¼ 31 is shown in Figure 18.3. The spect<strong>ru</strong>m W r (e jvT ) has two features thatare worth noting, the mainlobe width <strong>and</strong> the sidelobe amplitude. The mainlobe width is defined asthe distance between the two points closest to v ¼ 0, where W r (e jvT ) is zero. For a rectangular window,the mainlobe width is equal to 4p=N. The maximum sidelobe amplitude for W r (e jvT ) is equal toapproximately 13 dB relative to the maximum value at v ¼ 0.Figure 18.4 shows the log–magnitude response of applying a 31-point rectangular window to approximatean ideal low-pass filter with a cutoff frequency equal to p=4. It can be seen that the sharp transitionin the ideal response at v ¼ v c has been converted into a gradual transition. Also, in the passb<strong>and</strong> a seriesof overshoots <strong>and</strong> undershoots occur, <strong>and</strong> in the stopb<strong>and</strong>, where the desired response is zero, the FIRfilter has a nonzero response. These are the results of the convolution between W r (e jvT ) <strong>and</strong> H d (e jvT ).The mainlobe of W r (e jvT ) causes the smearing of the desired response <strong>and</strong> the sidelobes of W r (e jvT )appear as overshoots <strong>and</strong> undershoots to the desired response. It is interesting to note that there will0–10Amplitude spect<strong>ru</strong>m (dB)–20–30–40–50–60–70–800 0.5 1 1.5 2 2.5 3 3.5Frequency (rad)FIGURE 18.3Fourier transform of the rectangular window.

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