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Lattice Filter Structures 243<br />

FIGURE 6.19<br />

form<br />

FIR filter structures in Example 6.8: (a) direct form (b) lattice<br />

Hence<br />

K 0 =2,K 1 = 1 4 ,K2 = 1 2 ,K3 = 1 3<br />

The direct form and the lattice form structures are shown in Figure 6.19. To<br />

check that our lattice structure is correct, let us compute the impulse response<br />

of the filter using both forms.<br />

>> [x,n] = impseq(0,0,3]; format long hdirect=filter(b,1,delta)<br />

hdirect =<br />

2.00000000000000 1.08333333333333 1.25000000000000 0.66666666666667<br />

>> hlattice=latcfilt(K,delta)<br />

hlattice =<br />

2.00000000000000 1.08333333333333 1.25000000000000 0.66666666666667<br />

□<br />

6.4.3 ALL-POLE LATTICE FILTERS<br />

A lattice structure for an IIR filter is restricted to an all-pole system<br />

function. It can be developed from an FIR lattice structure. Let an allpole<br />

system function be given by<br />

H(z) =<br />

1+<br />

1<br />

(6.22)<br />

N∑<br />

a N (m)z −m<br />

m=1<br />

which from (6.19) is equal to H(z) =1/A N (z). Clearly, it is an inverse system<br />

to the FIR lattice of Figure 6.18 (except for factor b 0 ). This IIR filter<br />

of order N has a lattice structure with N stages, as shown in Figure 6.20.<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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