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Analog and Digital Filters 577


The Chebyshev polynomial coeffi cients Cn(x) oscillate between –1 and 1, and can be
generated by using the recursion equation given as follows:
Cn+ 1 (x) = 2 Cn(x) − Cn− 1 (x)
with C 0 (x) = 1 and C 1 (x) = x.
Table 6.4 shows the Chebyshev polynomials for n = 1, 2, 3, and 4.
Figure 6.14 displays the magnitude responses of an analog Chebyshev type-1 LPF
for n = 1, 2, 3, 4, and 10.
R.6.61 The Chebyshev type-2 fi lter is the complement of the Chebyshev type-1 fi lter, in the
sense that the magnitude response is smooth in the pass band and presents equal
ripple in the stop band.
Unlike the type-1 fi lter, which consists only of poles, the type-2 fi lters consist of
both poles and zeros.
The magnitude square of the response is given by

Hjw
Cww
Cww
Cww

a
ns
nsp
ns

()


()


()


()


2 2

2

2
1




























where ∈ defi nes the maximum stop-band deviation, wp denotes the pass-band
cutoff frequency, ws denotes the stop-band cutoff frequency, and Cn(x) are the
Chebyshev polynomials (defi ned in Table 6.4).
Figure 6.15 shows the magnitude responses of an analog Chebyshev type-2 fi lters
for n = 1, 2, 3, 4, and 10.
R.6.62 Elliptic fi lters, also known as Cauer fi lters, present ripples in the pass as well as in
the stop-band regions. The main characteristic of the elliptic fi lter is that the transi-
tion band is the narrowest with respect to the other two fi lter types, the Butterworth
and Chebyshev fi lters.
The square of the magnitude of the transfer function of the Cauer fi lters is
given by
Hjw
a Jwhn

()


(,)


2
2 2

1


1








where ε is the pass-band deviation, Jn(w, h) is the n-order Jacobian, and h indicates
the ripple’s height (in the pass- and stop-band regions).
Figure 6.16 shows the magnitude response of an elliptic fi lter for n = 1, 2, 3, 4,
and 10.
R.6.63 Butterworth, Chebyshev (types 1 and 2), and elliptic fi lters deal basically with the
magnitude response, with little concern about their phase response.

TABLE 6.4
Chebyshev Polynomials
nCn(w)
1 w
22 w^2 − 1
34 w^3 − 3 w
48 w^4 − 8 w^2 + 1
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