lp2bs(b, a, wo=1.0, bw=1.0)
Return an analog band-stop filter with center frequency :None:None:`wo`
and bandwidth :None:None:`bw`
from an analog low-pass filter prototype with unity cutoff frequency, in transfer function ('ba') representation.
This is derived from the s-plane substitution
$$s \rightarrow \frac{s \cdot \mathrm{BW}}{s^2 + {\omega_0}^2}$$This is the "wideband" transformation, producing a stopband with geometric (log frequency) symmetry about :None:None:`wo`
.
Numerator polynomial coefficients.
Denominator polynomial coefficients.
Desired stopband center, as angular frequency (e.g., rad/s). Defaults to no change.
Desired stopband width, as angular frequency (e.g., rad/s). Defaults to 1.
Numerator polynomial coefficients of the transformed band-stop filter.
Denominator polynomial coefficients of the transformed band-stop filter.
Transform a lowpass filter prototype to a bandstop filter.
>>> from scipy import signal
... import matplotlib.pyplot as plt
>>> lp = signal.lti([1.0], [1.0, 1.5])See :
... bs = signal.lti(*signal.lp2bs(lp.num, lp.den))
... w, mag_lp, p_lp = lp.bode()
... w, mag_bs, p_bs = bs.bode(w)
... plt.plot(w, mag_lp, label='Lowpass')
... plt.plot(w, mag_bs, label='Bandstop')
... plt.semilogx()
... plt.grid()
... plt.xlabel('Frequency [rad/s]')
... plt.ylabel('Magnitude [dB]')
... plt.legend()
The following pages refer to to this document either explicitly or contain code examples using this.
scipy.signal._filter_design.lp2hp
scipy.signal._filter_design.lp2lp
scipy.signal._filter_design.lp2bs
scipy.signal._filter_design.lp2bs_zpk
scipy.signal._filter_design.lp2bp
scipy.signal._filter_design.bilinear
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