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import numpy as np
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from scipy.sparse.linalg import expm
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from scipy.signal import medfilt
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from wafo.plotbackend import plotbackend as plt
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from wafo.sg_filter import (SavitzkyGolay, smoothn, Kalman, HodrickPrescott,
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HampelFilter)
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def demo_savitzky_on_noisy_chirp():
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"""
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Example
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-------
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>>> demo_savitzky_on_noisy_chirp()
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>>> plt.close()
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"""
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plt.figure(figsize=(7, 12))
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# generate chirp signal
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tvec = np.arange(0, 6.28, .02)
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true_signal = np.sin(tvec * (2.0 + tvec))
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true_d_signal = (2+tvec) * np.cos(tvec * (2.0 + tvec))
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# add noise to signal
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noise = np.random.normal(size=true_signal.shape)
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signal = true_signal + .15 * noise
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# plot signal
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plt.subplot(311)
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plt.plot(signal)
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plt.title('signal')
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# smooth and plot signal
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plt.subplot(312)
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savgol = SavitzkyGolay(n=8, degree=4)
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s_signal = savgol.smooth(signal)
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s2 = smoothn(signal, robust=True)
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plt.plot(s_signal)
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plt.plot(s2)
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plt.plot(true_signal, 'r--')
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plt.title('smoothed signal')
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# smooth derivative of signal and plot it
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plt.subplot(313)
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savgol1 = SavitzkyGolay(n=8, degree=1, diff_order=1)
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dt = tvec[1]-tvec[0]
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d_signal = savgol1.smooth(signal) / dt
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plt.plot(d_signal)
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plt.plot(true_d_signal, 'r--')
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plt.title('smoothed derivative of signal')
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def demo_kalman_voltimeter():
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"""
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Example
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-------
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>>> demo_kalman_voltimeter()
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>>> plt.close()
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"""
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V0 = 12
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h = np.atleast_2d(1) # voltimeter measure the voltage itself
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q = 1e-9 # variance of process noise as the car operates
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r = 0.05 ** 2 # variance of measurement error
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b = 0 # no system input
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u = 0 # no system input
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filt = Kalman(R=r, A=1, Q=q, H=h, B=b)
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# Generate random voltages and watch the filter operate.
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n = 50
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truth = np.random.randn(n) * np.sqrt(q) + V0
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z = truth + np.random.randn(n) * np.sqrt(r) # measurement
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x = np.zeros(n)
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for i, zi in enumerate(z):
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x[i] = filt(zi, u) # perform a Kalman filter iteration
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_hz = plt.plot(z, 'r.', label='observations')
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# a-posteriori state estimates:
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_hx = plt.plot(x, 'b-', label='Kalman output')
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_ht = plt.plot(truth, 'g-', label='true voltage')
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plt.legend()
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plt.title('Automobile Voltimeter Example')
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def lti_disc(F, L=None, Q=None, dt=1):
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"""LTI_DISC Discretize LTI ODE with Gaussian Noise.
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Syntax:
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[A,Q] = lti_disc(F,L,Qc,dt)
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In:
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F - NxN Feedback matrix
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L - NxL Noise effect matrix (optional, default identity)
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Qc - LxL Diagonal Spectral Density (optional, default zeros)
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dt - Time Step (optional, default 1)
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Out:
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A - Transition matrix
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Q - Discrete Process Covariance
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Description:
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Discretize LTI ODE with Gaussian Noise. The original
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ODE model is in form
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dx/dt = F x + L w, w ~ N(0,Qc)
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Result of discretization is the model
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x[k] = A x[k-1] + q, q ~ N(0,Q)
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Which can be used for integrating the model
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exactly over time steps, which are multiples
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of dt.
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"""
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n = np.shape(F)[0]
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if L is None:
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L = np.eye(n)
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if Q is None:
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Q = np.zeros((n, n))
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# Closed form integration of transition matrix
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A = expm(F * dt)
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# Closed form integration of covariance
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# by matrix fraction decomposition
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Phi = np.vstack((np.hstack((F, np.dot(np.dot(L, Q), L.T))),
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np.hstack((np.zeros((n, n)), -F.T))))
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AB = np.dot(expm(Phi * dt), np.vstack((np.zeros((n, n)), np.eye(n))))
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# Q = AB[:n, :] / AB[n:(2 * n), :]
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Q = np.linalg.solve(AB[n:(2 * n), :].T, AB[:n, :].T)
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return A, Q
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def demo_kalman_sine():
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"""Kalman Filter demonstration with sine signal.
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Example
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-------
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>>> demo_kalman_sine()
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>>> plt.close()
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"""
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sd = 0.5
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dt = 0.1
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w = 1
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T = np.arange(0, 30 + dt / 2, dt)
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n = len(T)
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X = 3*np.sin(w * T)
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Y = X + sd * np.random.randn(n)
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''' Initialize KF to values
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x = 0
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dx/dt = 0
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with great uncertainty in derivative
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'''
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M = np.zeros((2, 1))
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P = np.diag([0.1, 2])
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R = sd ** 2
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H = np.atleast_2d([1, 0])
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q = 0.1
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F = np.atleast_2d([[0, 1],
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[0, 0]])
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A, Q = lti_disc(F, L=None, Q=np.diag([0, q]), dt=dt)
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# Track and animate
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m = M.shape[0]
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_MM = np.zeros((m, n))
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_PP = np.zeros((m, m, n))
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'''In this demonstration we estimate a stationary sine signal from noisy
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measurements by using the classical Kalman filter.'
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'''
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filt = Kalman(R=R, x=M, P=P, A=A, Q=Q, H=H, B=0)
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# Generate random voltages and watch the filter operate.
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# n = 50
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# truth = np.random.randn(n) * np.sqrt(q) + V0
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# z = truth + np.random.randn(n) * np.sqrt(r) # measurement
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truth = X
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z = Y
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x = np.zeros((n, m))
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for i, zi in enumerate(z):
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x[i] = np.ravel(filt(zi, u=0))
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_hz = plt.plot(z, 'r.', label='observations')
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# a-posteriori state estimates:
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_hx = plt.plot(x[:, 0], 'b-', label='Kalman output')
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_ht = plt.plot(truth, 'g-', label='true voltage')
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plt.legend()
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plt.title('Automobile Voltimeter Example')
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# for k in range(m):
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# [M,P] = kf_predict(M,P,A,Q);
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# [M,P] = kf_update(M,P,Y(k),H,R);
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#
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# MM(:,k) = M;
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# PP(:,:,k) = P;
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#
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# %
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# % Animate
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# %
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# if rem(k,10)==1
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# plot(T,X,'b--',...
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# T,Y,'ro',...
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# T(k),M(1),'k*',...
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# T(1:k),MM(1,1:k),'k-');
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# legend('Real signal','Measurements','Latest estimate',
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# 'Filtered estimate')
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# title('Estimating a noisy sine signal with Kalman filter.');
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# drawnow;
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#
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# pause;
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# end
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# end
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#
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# clc;
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# disp('In this demonstration we estimate a stationary sine signal '
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# 'from noisy measurements by using the classical Kalman filter.');
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# disp(' ');
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# disp('The filtering results are now displayed sequantially for 10 time '
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# 'step at a time.');
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# disp(' ');
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# disp('<push any key to see the filtered and smoothed results together>')
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# pause;
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# %
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# % Apply Kalman smoother
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# %
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# SM = rts_smooth(MM,PP,A,Q);
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# plot(T,X,'b--',...
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# T,MM(1,:),'k-',...
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# T,SM(1,:),'r-');
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# legend('Real signal','Filtered estimate','Smoothed estimate')
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# title('Filtered and smoothed estimate of the original signal');
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#
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# clc;
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# disp('The filtered and smoothed estimates of the signal are now '
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# 'displayed.')
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# disp(' ');
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# disp('RMS errors:');
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# %
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# % Errors
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# %
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# fprintf('KF = %.3f\nRTS = %.3f\n',...
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# sqrt(mean((MM(1,:)-X(1,:)).^2)),...
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# sqrt(mean((SM(1,:)-X(1,:)).^2)));
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def demo_hampel():
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"""
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Example
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-------
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>>> demo_hampel()
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>>> plt.close()
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"""
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randint = np.random.randint
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Y = 5000 + np.random.randn(1000)
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outliers = randint(0, 1000, size=(10,))
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Y[outliers] = Y[outliers] + randint(1000, size=(10,))
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YY, res = HampelFilter(dx=3, t=3, fulloutput=True)(Y)
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YY1, res1 = HampelFilter(dx=1, t=3, adaptive=0.1, fulloutput=True)(Y)
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YY2, res2 = HampelFilter(dx=3, t=0, fulloutput=True)(Y) # median
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plt.figure(1)
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plot_hampel(Y, YY, res)
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plt.title('Standard HampelFilter')
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plt.figure(2)
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plot_hampel(Y, YY1, res1)
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plt.title('Adaptive HampelFilter')
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plt.figure(3)
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plot_hampel(Y, YY2, res2)
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plt.title('Median filter')
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def plot_hampel(Y, YY, res):
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X = np.arange(len(YY))
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plt.plot(X, Y, 'b.') # Original Data
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plt.plot(X, YY, 'r') # Hampel Filtered Data
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plt.plot(X, res['Y0'], 'b--') # Nominal Data
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plt.plot(X, res['LB'], 'r--') # Lower Bounds on Hampel Filter
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plt.plot(X, res['UB'], 'r--') # Upper Bounds on Hampel Filter
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i = res['outliers']
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plt.plot(X[i], Y[i], 'ks') # Identified Outliers
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def demo_tide_filter():
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"""
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Example
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-------
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>>> demo_tide_filter()
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>>> plt.close()
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"""
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# import statsmodels.api as sa
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import wafo.spectrum.models as sm
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sd = 10
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Sj = sm.Jonswap(Hm0=4.*sd)
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S = Sj.tospecdata()
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q = (0.1 * sd) ** 2 # variance of process noise s the car operates
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r = (100 * sd) ** 2 # variance of measurement error
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b = 0 # no system input
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u = 0 # no system input
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from scipy.signal import butter, filtfilt, lfilter_zi # lfilter,
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freq_tide = 1. / (12 * 60 * 60)
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freq_wave = 1. / 10
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freq_filt = freq_wave / 10
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dt = 1.
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freq = 1. / dt
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fn = (freq / 2)
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P = 10 * np.diag([1, 0.01])
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R = r
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H = np.atleast_2d([1, 0])
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F = np.atleast_2d([[0, 1],
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[0, 0]])
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A, Q = lti_disc(F, L=None, Q=np.diag([0, q]), dt=dt)
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t = np.arange(0, 60 * 12, 1. / freq)
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w = 2 * np.pi * freq # 1 Hz
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tide = 100 * np.sin(freq_tide * w * t + 2 * np.pi / 4) + 100
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y = tide + S.sim(len(t), dt=1. / freq)[:, 1].ravel()
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# lowess = sa.nonparametric.lowess
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# y2 = lowess(y, t, frac=0.5)[:,1]
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filt = Kalman(R=R, x=np.array([[tide[0]], [0]]), P=P, A=A, Q=Q, H=H, B=b)
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filt2 = Kalman(R=R, x=np.array([[tide[0]], [0]]), P=P, A=A, Q=Q, H=H, B=b)
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# y = tide + 0.5 * np.sin(freq_wave * w * t)
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# Butterworth filter
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b, a = butter(9, (freq_filt / fn), btype='low')
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# y2 = [lowess(y[max(i-60,0):i + 1], t[max(i-60,0):i + 1], frac=.3)[-1,1]
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# for i in range(len(y))]
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# y2 = [lfilter(b, a, y[:i + 1])[i] for i in range(len(y))]
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# y3 = filtfilt(b, a, y[:16]).tolist() + [filtfilt(b, a, y[:i + 1])[i]
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# for i in range(16, len(y))]
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# y0 = medfilt(y, 41)
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_zi = lfilter_zi(b, a)
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# y2 = lfilter(b, a, y)#, zi=y[0]*zi) # standard filter
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y3 = filtfilt(b, a, y) # filter with phase shift correction
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y4 = []
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y5 = []
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for _i, j in enumerate(y):
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tmp = np.ravel(filt(j, u=u))
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tmp = np.ravel(filt2(tmp[0], u=u))
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# if i==0:
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# print(filt.x)
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# print(filt2.x)
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y4.append(tmp[0])
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y5.append(tmp[1])
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_y0 = medfilt(y4, 41)
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# print(filt.P)
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# plot
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plt.plot(t, y, 'r.-', linewidth=2, label='raw data')
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# plt.plot(t, y2, 'b.-', linewidth=2, label='lowess @ %g Hz' % freq_filt)
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# plt.plot(t, y2, 'b.-', linewidth=2, label='filter @ %g Hz' % freq_filt)
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plt.plot(t, y3, 'g.-', linewidth=2, label='filtfilt @ %g Hz' % freq_filt)
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plt.plot(t, y4, 'k.-', linewidth=2, label='kalman')
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# plt.plot(t, y5, 'k.', linewidth=2, label='kalman2')
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plt.plot(t, tide, 'y-', linewidth=2, label='True tide')
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plt.legend(frameon=False, fontsize=14)
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plt.xlabel("Time [s]")
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plt.ylabel("Amplitude")
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def demo_savitzky_on_exponential():
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"""
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|
Example
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-------
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>>> demo_savitzky_on_exponential()
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>>> plt.close()
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"""
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t = np.linspace(-4, 4, 500)
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y = np.exp(-t ** 2) + np.random.normal(0, 0.05, np.shape(t))
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n = 11
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ysg = SavitzkyGolay(n, degree=1, diff_order=0)(y)
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plt.plot(t, y, t, ysg, '--')
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def demo_smoothn_on_1d_cos():
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|
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|
"""
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|
Example
|
|
|
|
-------
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|
>>> demo_smoothn_on_1d_cos()
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>>> plt.close()
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|
"""
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x = np.linspace(0, 100, 2 ** 8)
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y = np.cos(x / 10) + (x / 50) ** 2 + np.random.randn(np.size(x)) / 10
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y[np.r_[70, 75, 80]] = np.array([5.5, 5, 6])
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z = smoothn(y) # Regular smoothing
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zr = smoothn(y, robust=True) # Robust smoothing
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|
_h0 = plt.subplot(121),
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|
_h = plt.plot(x, y, 'r.', x, z, 'k', linewidth=2)
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|
plt.title('Regular smoothing')
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|
plt.subplot(122)
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|
plt.plot(x, y, 'r.', x, zr, 'k', linewidth=2)
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|
plt.title('Robust smoothing')
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|
|
|
|
def demo_smoothn_on_2d_exp_sin():
|
|
|
|
"""
|
|
|
|
Example
|
|
|
|
-------
|
|
|
|
>>> demo_smoothn_on_2d_exp_sin()
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|
|
|
|
|
|
>>> plt.close()
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|
|
|
"""
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|
xp = np.arange(0, 1, 0.02) # np.r_[0:1:0.02]
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|
[x, y] = np.meshgrid(xp, xp)
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|
|
f = np.exp(x + y) + np.sin((x - 2 * y) * 3)
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|
|
fn = f + np.random.randn(*f.shape) * 0.5
|
|
|
|
_fs, s = smoothn(fn, fulloutput=True)
|
|
|
|
fs2 = smoothn(fn, s=2 * s)
|
|
|
|
_h = plt.subplot(131),
|
|
|
|
_h = plt.contourf(xp, xp, fn)
|
|
|
|
_h = plt.subplot(132),
|
|
|
|
_h = plt.contourf(xp, xp, fs2)
|
|
|
|
_h = plt.subplot(133),
|
|
|
|
_h = plt.contourf(xp, xp, f)
|
|
|
|
|
|
|
|
|
|
|
|
def _cardioid(n=1000):
|
|
|
|
t = np.linspace(0, 2 * np.pi, n)
|
|
|
|
x0 = 2 * np.cos(t) * (1 - np.cos(t))
|
|
|
|
y0 = 2 * np.sin(t) * (1 - np.cos(t))
|
|
|
|
x = x0 + np.random.randn(x0.size) * 0.1
|
|
|
|
y = y0 + np.random.randn(y0.size) * 0.1
|
|
|
|
return x, y, x0, y0
|
|
|
|
|
|
|
|
|
|
|
|
def demo_smoothn_on_cardioid():
|
|
|
|
"""
|
|
|
|
Example
|
|
|
|
-------
|
|
|
|
>>> demo_smoothn_on_cardioid()
|
|
|
|
|
|
|
|
>>> plt.close()
|
|
|
|
"""
|
|
|
|
x, y, x0, y0 = _cardioid()
|
|
|
|
z = smoothn(x + 1j * y, robust=False)
|
|
|
|
plt.plot(x0, y0, 'y',
|
|
|
|
x, y, 'r.',
|
|
|
|
np.real(z), np.imag(z), 'k', linewidth=2)
|
|
|
|
|
|
|
|
|
|
|
|
def demo_hodrick_on_cardioid():
|
|
|
|
"""
|
|
|
|
Example
|
|
|
|
-------
|
|
|
|
>>> demo_hodrick_on_cardioid()
|
|
|
|
|
|
|
|
>>> plt.close()
|
|
|
|
"""
|
|
|
|
x, y, x0, y0 = _cardioid()
|
|
|
|
|
|
|
|
smooth = HodrickPrescott(w=20000)
|
|
|
|
# smooth = HampelFilter(adaptive=50)
|
|
|
|
xs, ys = smooth(x), smooth(y)
|
|
|
|
plt.plot(x0, y0, 'y',
|
|
|
|
x, y, 'r.',
|
|
|
|
xs, ys, 'k', linewidth=2)
|
|
|
|
|
|
|
|
if __name__ == '__main__':
|
|
|
|
from wafo.testing import test_docstrings
|
|
|
|
test_docstrings(__file__)
|
|
|
|
# demo_savitzky_on_noisy_chirp()
|
|
|
|
# plt.show('hold') # show plot
|
|
|
|
# demo_kalman_sine()
|
|
|
|
# demo_tide_filter()
|
|
|
|
# demo_hampel()
|
|
|
|
# demo_kalman_voltimeter()
|
|
|
|
# demo_savitzky_on_exponential()
|
|
|
|
# plt.figure(1)
|
|
|
|
# demo_hodrick_on_cardioid()
|
|
|
|
# plt.figure(2)
|
|
|
|
# # demo_smoothn_on_1d_cos()
|
|
|
|
# demo_smoothn_on_cardioid()
|
|
|
|
# plt.show('hold')
|