Chebyshev filters are analog or digital filters having a steeper roll-off and more passband ripple (type I) or stopband ripple (type II) than Butterworth filters. Chebyshev filters have the property that they minimize the error between the idealized and the actual filter characteristic over the range of the filter, but with ripples in the passband. This type of filter is named after Pafnuty Chebyshev because its mathematical characteristics are derived from Chebyshev polynomials.
Because of the passband ripple inherent in Chebyshev filters, the ones that have a smoother response in the passband but a more irregular response in the stopband are preferred for some applications.
- 1 Type I Chebyshev filters
- 2 Type II Chebyshev filters
- 3 Implementation
- 4 Comparison with other linear filters
- 5 See also
- 6 Notes
- 7 References
Type I Chebyshev filters
Type I Chebyshev filters are the most common types of Chebyshev filters. The gain (or amplitude) response as a function of angular frequency of the nth-order low-pass filter is equal to the absolute value of the transfer function :
The passband exhibits equiripple behavior, with the ripple determined by the ripple factor . In the passband, the Chebyshev polynomial alternates between -1 and 1 so the filter gain alternate between maxima at G = 1 and minima at . At the cutoff frequency the gain again has the value but continues to drop into the stopband as the frequency increases. This behavior is shown in the diagram on the right. The common practice of defining the cutoff frequency at −3 dB is usually not applied to Chebyshev filters; instead the cutoff is taken as the point at which the gain falls to the value of the ripple for the final time.
The ripple is often given in dB:
- Ripple in dB =
so that a ripple amplitude of 3 dB results from
An even steeper roll-off can be obtained if ripple is allowed in the stopband, by allowing zeroes on the -axis in the complex plane. However, this results in less suppression in the stopband. The result is called an elliptic filter, also known as Cauer filter.
Poles and zeroes
For simplicity, it is assumed that the cutoff frequency is equal to unity. The poles of the gain function of the Chebyshev filter are the zeroes of the denominator of the gain function. Using the complex frequency s, these occur when:
Defining and using the trigonometric definition of the Chebyshev polynomials yields:
where the multiple values of the arc cosine function are made explicit using the integer index m. The poles of the Chebyshev gain function are then:
Using the properties of the trigonometric and hyperbolic functions, this may be written in explicitly complex form:
where m = 1, 2,..., n and
This may be viewed as an equation parametric in and it demonstrates that the poles lie on an ellipse in s-space centered at s = 0 with a real semi-axis of length and an imaginary semi-axis of length of
The transfer function
The above expression yields the poles of the gain G. For each complex pole, there is another which is the complex conjugate, and for each conjugate pair there are two more that are the negatives of the pair. The transfer function must be stable, so that its poles are those of the gain that have negative real parts and therefore lie in the left half plane of complex frequency space. The transfer function is then given by
where are only those poles with a negative sign in front of the real term in the above equation for the poles.
The group delay
The group delay is defined as the derivative of the phase with respect to angular frequency and is a measure of the distortion in the signal introduced by phase differences for different frequencies.
The gain and the group delay for a fifth-order type I Chebyshev filter with ε=0.5 are plotted in the graph on the left. It can be seen that there are ripples in the gain and the group delay in the passband but not in the stopband.
Type II Chebyshev filters
Also known as inverse Chebyshev filters, the Type II Chebyshev filter type is less common because it does not roll off as fast as Type I, and requires more components. It has no ripple in the passband, but does have equiripple in the stopband. The gain is:
In the stopband, the Chebyshev polynomial oscillates between -1 and 1 so that the gain will oscillate between zero and
For a stopband attenuation of 5 dB, ε = 0.6801; for an attenuation of 10 dB, ε = 0.3333. The frequency f0 = ω0/2π is the cutoff frequency. The 3 dB frequency fH is related to f0 by:
Poles and zeroes
Assuming that the cutoff frequency is equal to unity, the poles of the gain of the Chebyshev filter are the zeroes of the denominator of the gain:
The poles of gain of the type II Chebyshev filter are the inverse of the poles of the type I filter:
where m = 1, 2, ..., n . The zeroes of the type II Chebyshev filter are the zeroes of the numerator of the gain:
The zeroes of the type II Chebyshev filter are therefore the inverse of the zeroes of the Chebyshev polynomial.
for m = 1, 2, ..., n.
The transfer function
The transfer function is given by the poles in the left half plane of the gain function, and has the same zeroes but these zeroes are single rather than double zeroes.
The group delay
The gain and the group delay for a fifth-order type II Chebyshev filter with ε=0.1 are plotted in the graph on the left. It can be seen that there are ripples in the gain in the stopband but not in the pass band.
A passive LC Chebyshev low-pass filter may be realized using a Cauer topology. The inductor or capacitor values of a nth-order Chebyshev prototype filter may be calculated from the following equations:
G1, Gk are the capacitor or inductor element values. fH, the 3 dB frequency is calculated with:
The coefficients A, γ, β, Ak, and Bk may be calculated from the following equations:
where RdB is the passband ripple in decibels.
- C1 shunt = G1, L2 series = G2, ...
- L1 shunt = G1, C1 series = G2, ...
Note that when G1 is a shunt capacitor or series inductor, G0 corresponds to the input resistance or conductance, respectively. The same relationship holds for Gn+1 and Gn. The resulting circuit is a normalized low-pass filter. Using frequency transformations and impedance scaling, the normalized low-pass filter may be transformed into high-pass, band-pass, and band-stop filters of any desired cutoff frequency or bandwidth.
As with most analog filters, the Chebyshev may be converted to a digital (discrete-time) recursive form via the bilinear transform. However, as digital filters have a finite bandwidth, the response shape of the transformed Chebyshev is warped. Alternatively, the Matched Z-transform method may be used, which does not warp the response.
Comparison with other linear filters
The following illustration shows the Chebyshev filters next to other common filter types obtained with the same number of coefficients (fifth order):
- Matthaei et. al 1980, p.99
- Daniels, Richard W. (1974). Approximation Methods for Electronic Filter Design. New York: McGraw-Hill. ISBN 0-07-015308-6.
- Williams, Arthur B.; Taylors, Fred J. (1988). Electronic Filter Design Handbook. New York: McGraw-Hill. ISBN 0-07-070434-1.
- Matthaei, George L.; Young, Leo; Jones, E. M. T. (1980). Microwave Filters, Impedance-Matching Networks, and Coupling Structures. Norwood, MA: Artech House. ISBN 0-89-006099-1.