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506 Chapter 9 SAMPLING RATE CONVERSION<br />

X(ω x )<br />

We will allow filter to<br />

substantially change<br />

this band.<br />

ω x<br />

−π −ω −ωx,s x,p<br />

0<br />

ω x,p π<br />

ω x,s<br />

(a)<br />

V(ω y )<br />

−π<br />

− 2π<br />

I<br />

− π I<br />

0<br />

(b)<br />

π<br />

I<br />

ω x,p<br />

I<br />

ω x,s<br />

I<br />

2π<br />

I<br />

2π − ω x,s<br />

I<br />

π<br />

ω y<br />

FIGURE 9.22<br />

Frequency parameters: (a) signal, (b) filter<br />

be the passband and stopband edge frequencies, respectively, of the lowpass<br />

linear-phase FIR filter given by<br />

H(ω) =H r (ω)e jθ(ω) (9.51)<br />

where H r (ω) isthe real-valued amplitude response and θ(ω) isthe unwrapped<br />

phase response. Then we have the following filter design specifications:<br />

1<br />

I H r(ω) ≤ 1 ± δ 1 for |ω| ∈[0,ω p ]<br />

1<br />

I H r(ω) ≤±δ 2<br />

for |ω| ∈[ω s ,π]<br />

(9.52)<br />

where ω p and ω s are as given in (9.50) and δ 1 and δ 2 are the passband<br />

and stopband ripple parameters, respectively, of the lowpass FIR filter.<br />

Comment: Instead of beginning the stopband at π/I, wewere able to<br />

shift it to (2π − ω s ) /I. Ifω x,s ≪ π, then this will be an important consideration<br />

to lower filter order. However, in the worst-case scenario of<br />

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