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400 Chapter 8 IIR FILTER DESIGN<br />

with initial conditions y(−1) =0,y(−2) = −A sin ω 0 is exactly the same<br />

as the response of (8.38) to an impulse excitation. In fact, the homogeneous<br />

difference equation in (8.39) can be obtained directly from the<br />

trigonometric identity<br />

( ) ( )<br />

α + β α − β<br />

sin α + sin β =2sin cos<br />

(8.40)<br />

2<br />

2<br />

where, by definition, α =(n +1)ω 0 ,β=(n − 1)ω 0 , and y(n) =sin(n +<br />

1)ω 0 .<br />

In practical applications involving modulation of two sinusoidal carrier<br />

signals in phase quadrature, there is a need to generate the sinusoids<br />

A sin ω 0 n and A cos ω 0 n. These quadrature carrier signals can be generated<br />

by the so-called coupled-form oscillator, which can be obtained with<br />

the aid of the trigonometric formulas<br />

cos(α + β) =cos α cos β − sin α sin β (8.41)<br />

sin(α + β) =sin α cos β + cos α sin β (8.42)<br />

where by definition, α = nω 0 ,β= ω 0 ,y c (n) =cos(n +1)ω 0 , and y s (n) =<br />

sin(n +1)ω 0 .Thus, with substitution of these quantities into the two<br />

trigonometric identities, we obtain the two coupled difference equations.<br />

y c (n) =(cos ω 0 ) y c (n − 1) − (sin ω 0 ) y s (n − 1) (8.43)<br />

y s (n) =(sin ω 0 ) y c (n − 1) + (cos ω 0 ) y s (n − 1) (8.44)<br />

The structure for the realization of the coupled-form oscillator is illustrated<br />

in Figure 8.12. Note that this is a 2-output system that does<br />

not require any input excitation, but it does require setting the initial<br />

conditions y c (−1) = A cos ω 0 and y s (−1) = −A sin ω 0 in order to begin<br />

its self-sustaining oscillations.<br />

8.3 CHARACTERISTICS OF PROTOTYPE ANALOG FILTERS<br />

IIR filter design techniques rely on existing analog filters to obtain digital<br />

filters. We designate these analog filters as prototype filters. Three prototypes<br />

are widely used in practice. In this section we briefly summarize<br />

the characteristics of the lowpass versions of these prototypes: Butterworth<br />

lowpass, Chebyshev lowpass (Type I and II), and Elliptic lowpass.<br />

Although we will use MATLAB functions to design these filters, it is necessary<br />

to learn the characteristics of these filters so that we can use proper<br />

parameters in MATLAB functions to obtain correct results.<br />

Copyright 2010 Cengage Learning. All Rights Reserved. May not be copied, scanned, or duplicated, in whole or in part. Due to electronic rights, some third party content may be suppressed from the eBook and/or eChapter(s).<br />

Editorial review has deemed that any suppressed content does not materially affect the overall learning experience. Cengage Learning reserves the right to remove additional content at any time if subsequent rights restrictions require it.

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