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Chebyshev filter : ウィキペディア英語版
Chebyshev filter

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.
== 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 \omega of the ''n''th-order low-pass filter is equal to the absolute value of the transfer function H_n(j \omega):
:G_n(\omega) = \left | H_n(j \omega) \right | = \frac\right)}}
where \varepsilon is the ripple factor, \omega_0 is the cutoff frequency and T_n is a Chebyshev polynomial of the nth order.
The passband exhibits equiripple behavior, with the ripple determined by the ripple factor \varepsilon. In the passband, the Chebyshev polynomial alternates between -1 and 1 so the filter gain alternate between maxima at ''G'' = 1 and minima at G=1/\sqrt. At the cutoff frequency \omega_0 the gain again has the value 1/\sqrt but continues to drop into the stop band 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 order of a Chebyshev filter is equal to the number of reactive components (for example, inductors) needed to realize the filter using analog electronics.
The ripple is often given in dB:
:Ripple in dB = 10 \log_(1+\varepsilon^2)
so that a ripple amplitude of 3 dB results from \varepsilon = 1.
An even steeper roll-off can be obtained if ripple is allowed in the stop band, by allowing zeroes on the j\omega-axis in the complex plane. However, this results in less suppression in the stop band. The result is called an elliptic filter, also known as Cauer filter.



抄文引用元・出典: フリー百科事典『 ウィキペディア(Wikipedia)
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