Pole locations and transfer function The poles of the Chebyshev I filter are laid to those of the Butterworth filter of the similar order and are shown on an ellipse in the s-plane. If N is odd there shall be a pole on the negative real axis. In order to search the pole locations and hence the transfer function we start the parameter β
The poles of H(s), sk = ζk + jΩk, k = 0, 1, ... , (N-1), are provided by
Note that if the sinh β and cosh β terms were not shown we could have the pole situation of the normalized Butterworth filter (on the unit circle), that is,
with σ2k + Ω2k = 1 which is the unit circle. Thus, the hyperbolic sine and cosine terms are scale factors which, when applied to the Butterworth pole coordinates, provide the pole coordinates of a Chebyshev I filter of the similar order. The Chebyshev poles are situated on an ellipse in the s- plane defined by
The major axis of the ellipse is on the imaginary (jΩ) axis and the minor axis is on the real axis and the foci are at Ω = ±1. The 3 dB cut-off frequency happens at the point where the ellipse collides the jΩ axis, that is, at Ω = cosh β. In taking together the transfer function, H(s), we laid on the symmetry of pole positions and create use of the left half plane poles only. Finally, the pole positions are measure by the actual "cut-off frequency" Ω1. That last step amounts to s→ s/Ω1 (in the case of the Butterworth design this was s→ s/Ωc).
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