Module « scipy.signal »
Signature de la fonction firls
def firls(numtaps, bands, desired, weight=None, nyq=None, fs=None)
Description
firls.__doc__
FIR filter design using least-squares error minimization.
Calculate the filter coefficients for the linear-phase finite
impulse response (FIR) filter which has the best approximation
to the desired frequency response described by `bands` and
`desired` in the least squares sense (i.e., the integral of the
weighted mean-squared error within the specified bands is
minimized).
Parameters
----------
numtaps : int
The number of taps in the FIR filter. `numtaps` must be odd.
bands : array_like
A monotonic nondecreasing sequence containing the band edges in
Hz. All elements must be non-negative and less than or equal to
the Nyquist frequency given by `nyq`.
desired : array_like
A sequence the same size as `bands` containing the desired gain
at the start and end point of each band.
weight : array_like, optional
A relative weighting to give to each band region when solving
the least squares problem. `weight` has to be half the size of
`bands`.
nyq : float, optional
*Deprecated. Use `fs` instead.*
Nyquist frequency. Each frequency in `bands` must be between 0
and `nyq` (inclusive). Default is 1.
fs : float, optional
The sampling frequency of the signal. Each frequency in `bands`
must be between 0 and ``fs/2`` (inclusive). Default is 2.
Returns
-------
coeffs : ndarray
Coefficients of the optimal (in a least squares sense) FIR filter.
See also
--------
firwin
firwin2
minimum_phase
remez
Notes
-----
This implementation follows the algorithm given in [1]_.
As noted there, least squares design has multiple advantages:
1. Optimal in a least-squares sense.
2. Simple, non-iterative method.
3. The general solution can obtained by solving a linear
system of equations.
4. Allows the use of a frequency dependent weighting function.
This function constructs a Type I linear phase FIR filter, which
contains an odd number of `coeffs` satisfying for :math:`n < numtaps`:
.. math:: coeffs(n) = coeffs(numtaps - 1 - n)
The odd number of coefficients and filter symmetry avoid boundary
conditions that could otherwise occur at the Nyquist and 0 frequencies
(e.g., for Type II, III, or IV variants).
.. versionadded:: 0.18
References
----------
.. [1] Ivan Selesnick, Linear-Phase Fir Filter Design By Least Squares.
OpenStax CNX. Aug 9, 2005.
http://cnx.org/contents/eb1ecb35-03a9-4610-ba87-41cd771c95f2@7
Examples
--------
We want to construct a band-pass filter. Note that the behavior in the
frequency ranges between our stop bands and pass bands is unspecified,
and thus may overshoot depending on the parameters of our filter:
>>> from scipy import signal
>>> import matplotlib.pyplot as plt
>>> fig, axs = plt.subplots(2)
>>> fs = 10.0 # Hz
>>> desired = (0, 0, 1, 1, 0, 0)
>>> for bi, bands in enumerate(((0, 1, 2, 3, 4, 5), (0, 1, 2, 4, 4.5, 5))):
... fir_firls = signal.firls(73, bands, desired, fs=fs)
... fir_remez = signal.remez(73, bands, desired[::2], fs=fs)
... fir_firwin2 = signal.firwin2(73, bands, desired, fs=fs)
... hs = list()
... ax = axs[bi]
... for fir in (fir_firls, fir_remez, fir_firwin2):
... freq, response = signal.freqz(fir)
... hs.append(ax.semilogy(0.5*fs*freq/np.pi, np.abs(response))[0])
... for band, gains in zip(zip(bands[::2], bands[1::2]),
... zip(desired[::2], desired[1::2])):
... ax.semilogy(band, np.maximum(gains, 1e-7), 'k--', linewidth=2)
... if bi == 0:
... ax.legend(hs, ('firls', 'remez', 'firwin2'),
... loc='lower center', frameon=False)
... else:
... ax.set_xlabel('Frequency (Hz)')
... ax.grid(True)
... ax.set(title='Band-pass %d-%d Hz' % bands[2:4], ylabel='Magnitude')
...
>>> fig.tight_layout()
>>> plt.show()
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