scipy.signal.sweep_poly¶

scipy.signal.
sweep_poly
(t, poly, phi=0)[source]¶ Frequencyswept cosine generator, with a timedependent frequency.
This function generates a sinusoidal function whose instantaneous frequency varies with time. The frequency at time t is given by the polynomial poly.
Parameters:  t : ndarray
Times at which to evaluate the waveform.
 poly : 1D array_like or instance of numpy.poly1d
The desired frequency expressed as a polynomial. If poly is a list or ndarray of length n, then the elements of poly are the coefficients of the polynomial, and the instantaneous frequency is
f(t) = poly[0]*t**(n1) + poly[1]*t**(n2) + ... + poly[n1]
If poly is an instance of numpy.poly1d, then the instantaneous frequency is
f(t) = poly(t)
 phi : float, optional
Phase offset, in degrees, Default: 0.
Returns:  sweep_poly : ndarray
A numpy array containing the signal evaluated at t with the requested timevarying frequency. More precisely, the function returns
cos(phase + (pi/180)*phi)
, where phase is the integral (from 0 to t) of2 * pi * f(t)
;f(t)
is defined above.
See also
Notes
New in version 0.8.0.
If poly is a list or ndarray of length n, then the elements of poly are the coefficients of the polynomial, and the instantaneous frequency is:
f(t) = poly[0]*t**(n1) + poly[1]*t**(n2) + ... + poly[n1]
If poly is an instance of
numpy.poly1d
, then the instantaneous frequency is:f(t) = poly(t)
Finally, the output s is:
cos(phase + (pi/180)*phi)
where phase is the integral from 0 to t of
2 * pi * f(t)
,f(t)
as defined above.Examples
Compute the waveform with instantaneous frequency:
f(t) = 0.025*t**3  0.36*t**2 + 1.25*t + 2
over the interval 0 <= t <= 10.
>>> from scipy.signal import sweep_poly >>> p = np.poly1d([0.025, 0.36, 1.25, 2.0]) >>> t = np.linspace(0, 10, 5001) >>> w = sweep_poly(t, p)
Plot it:
>>> import matplotlib.pyplot as plt >>> plt.subplot(2, 1, 1) >>> plt.plot(t, w) >>> plt.title("Sweep Poly\nwith frequency " + ... "$f(t) = 0.025t^3  0.36t^2 + 1.25t + 2$") >>> plt.subplot(2, 1, 2) >>> plt.plot(t, p(t), 'r', label='f(t)') >>> plt.legend() >>> plt.xlabel('t') >>> plt.tight_layout() >>> plt.show()