Module « scipy.signal »
Signature de la fonction iirdesign
def iirdesign(wp, ws, gpass, gstop, analog=False, ftype='ellip', output='ba', fs=None)
Description
iirdesign.__doc__
Complete IIR digital and analog filter design.
Given passband and stopband frequencies and gains, construct an analog or
digital IIR filter of minimum order for a given basic type. Return the
output in numerator, denominator ('ba'), pole-zero ('zpk') or second order
sections ('sos') form.
Parameters
----------
wp, ws : float or array like, shape (2,)
Passband and stopband edge frequencies. Possible values are scalars
(for lowpass and highpass filters) or ranges (for bandpass and bandstop
filters).
For digital filters, these are in the same units as `fs`. By default,
`fs` is 2 half-cycles/sample, so these are normalized from 0 to 1,
where 1 is the Nyquist frequency. For example:
- Lowpass: wp = 0.2, ws = 0.3
- Highpass: wp = 0.3, ws = 0.2
- Bandpass: wp = [0.2, 0.5], ws = [0.1, 0.6]
- Bandstop: wp = [0.1, 0.6], ws = [0.2, 0.5]
For analog filters, `wp` and `ws` are angular frequencies (e.g., rad/s).
Note, that for bandpass and bandstop filters passband must lie strictly
inside stopband or vice versa.
gpass : float
The maximum loss in the passband (dB).
gstop : float
The minimum attenuation in the stopband (dB).
analog : bool, optional
When True, return an analog filter, otherwise a digital filter is
returned.
ftype : str, optional
The type of IIR filter to design:
- Butterworth : 'butter'
- Chebyshev I : 'cheby1'
- Chebyshev II : 'cheby2'
- Cauer/elliptic: 'ellip'
- Bessel/Thomson: 'bessel'
output : {'ba', 'zpk', 'sos'}, optional
Filter form of the output:
- second-order sections (recommended): 'sos'
- numerator/denominator (default) : 'ba'
- pole-zero : 'zpk'
In general the second-order sections ('sos') form is
recommended because inferring the coefficients for the
numerator/denominator form ('ba') suffers from numerical
instabilities. For reasons of backward compatibility the default
form is the numerator/denominator form ('ba'), where the 'b'
and the 'a' in 'ba' refer to the commonly used names of the
coefficients used.
Note: Using the second-order sections form ('sos') is sometimes
associated with additional computational costs: for
data-intense use cases it is therefore recommended to also
investigate the numerator/denominator form ('ba').
fs : float, optional
The sampling frequency of the digital system.
.. versionadded:: 1.2.0
Returns
-------
b, a : ndarray, ndarray
Numerator (`b`) and denominator (`a`) polynomials of the IIR filter.
Only returned if ``output='ba'``.
z, p, k : ndarray, ndarray, float
Zeros, poles, and system gain of the IIR filter transfer
function. Only returned if ``output='zpk'``.
sos : ndarray
Second-order sections representation of the IIR filter.
Only returned if ``output=='sos'``.
See Also
--------
butter : Filter design using order and critical points
cheby1, cheby2, ellip, bessel
buttord : Find order and critical points from passband and stopband spec
cheb1ord, cheb2ord, ellipord
iirfilter : General filter design using order and critical frequencies
Notes
-----
The ``'sos'`` output parameter was added in 0.16.0.
Examples
--------
>>> from scipy import signal
>>> import matplotlib.pyplot as plt
>>> import matplotlib.ticker
>>> wp = 0.2
>>> ws = 0.3
>>> gpass = 1
>>> gstop = 40
>>> system = signal.iirdesign(wp, ws, gpass, gstop)
>>> w, h = signal.freqz(*system)
>>> fig, ax1 = plt.subplots()
>>> ax1.set_title('Digital filter frequency response')
>>> ax1.plot(w, 20 * np.log10(abs(h)), 'b')
>>> ax1.set_ylabel('Amplitude [dB]', color='b')
>>> ax1.set_xlabel('Frequency [rad/sample]')
>>> ax1.grid()
>>> ax1.set_ylim([-120, 20])
>>> ax2 = ax1.twinx()
>>> angles = np.unwrap(np.angle(h))
>>> ax2.plot(w, angles, 'g')
>>> ax2.set_ylabel('Angle (radians)', color='g')
>>> ax2.grid()
>>> ax2.axis('tight')
>>> ax2.set_ylim([-6, 1])
>>> nticks = 8
>>> ax1.yaxis.set_major_locator(matplotlib.ticker.LinearLocator(nticks))
>>> ax2.yaxis.set_major_locator(matplotlib.ticker.LinearLocator(nticks))
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