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FIR and IIR system realization
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2
wl) — oGz —osNt + yeFIR Filter Realization:
Structure of FIR filters
With cont
us filters that have diserete components, the filler structure isan electric schema that
includes condensers, coils and resistances,.9s well s other elements. These fillers are active if they
contain amplifiers.
Inthe ease of digital filters, the structure ofthe filter corresponds to the synoptic schema that
‘connects input and output, into whieh delay clements and weighting values are introduced. This is @
‘way of visualizing the flow of samplings when it undergoes delays or when itis weighted. This
structure is direetly deduced from the transfer function or the difference equation. It is very simple
andl for this reason is called a direct structure.
Direct form realization of FIR filter systen (transversal Structure)
pla) = Yack yx(n—k)
where y(n) and x(n) are output and input sequence respectivey. this equation is obtained by setting
bik) and a,=0, k=0,1,2,..Mel
Foran FIR filer characterized by equation (5.3) in Chapter 5, wit
obtain Figure 7.1.
put x and output y we
we)
Figure 7.1. Direct structure of an FIR fillerCascade form realization of FIR filter System
‘Asan alternative to the direct form, we factor the Fir transfer function H(z) asa product of
second order factor given by
H(z) =|] (Boe + BeFIR Lincar Phase
A linear phase FIR filter of length M is characterized by
h(n) = h(M ~1~n)
the symmetry property ofa linear phase FIR filter is used to reduce the multipliers required in
these realizations. using this condition, the Z-transform of the impulse response can be expressed
as
(2) = 21K 9] = Lated=*
x(n)
BY
|
h00) Att) (ey
nl
yo
Fig. 9.20 Direct Form Realisation Structure ofa Linear Phase FIR System when M is Even
pole: fe}
b
(0)
| 1 = fe
me mF may mee-ayer\7 n—ay2) V7
ok —— i oo
Fig.9.21 Direct Form Realisation Structure of a Linear Phase FIR System when M is OddCascade Realisation
HG) -()
‘This function is realised in FIR cascade form as shown in Fig. B9.13(0).
yeeoe
Obeain FAR tinearspha
gat
a
tere M= S and the realisation is shown in Fig, B9.14(@)-
Cascade Realisation
Ho(t+ Jette)
has a product of two sections which have te linear phase symm
mn in Fig. E9.14(b).
- fe 0
property The corresponding cascade
He
realisation is show?
ers
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Fig, £9.14(@) and (®)