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@ -18,9 +18,13 @@ from numpy.ma.core import ones, zeros, prod, sin
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from numpy import diff, pi, inf #@UnresolvedImport
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from numpy import diff, pi, inf #@UnresolvedImport
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from numpy.lib.shape_base import vstack
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from numpy.lib.shape_base import vstack
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from numpy.lib.function_base import linspace
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from numpy.lib.function_base import linspace
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from scipy.interpolate import PiecewisePolynomial
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import polynomial as pl
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import polynomial as pl
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__all__ = ['PPform', 'savitzky_golay', 'savitzky_golay_piecewise', 'sgolay2d','SmoothSpline', 'stineman_interp']
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__all__ = ['PPform', 'savitzky_golay', 'savitzky_golay_piecewise', 'sgolay2d','SmoothSpline',
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'slopes','pchip_slopes','slopes2','stineman_interp', 'Pchip','StinemanInterp', 'CubicHermiteSpline']
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def savitzky_golay(y, window_size, order, deriv=0):
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def savitzky_golay(y, window_size, order, deriv=0):
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r"""Smooth (and optionally differentiate) data with a Savitzky-Golay filter.
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r"""Smooth (and optionally differentiate) data with a Savitzky-Golay filter.
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@ -531,13 +535,11 @@ class SmoothSpline(PPform):
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di = di.T
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di = di.T
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ci = ci.T
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ci = ci.T
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ai = ai.T
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ai = ai.T
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#end
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if not any(di):
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if not any(di):
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if not any(ci):
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if not any(ci):
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coefs = vstack([bi.ravel(), ai.ravel()])
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coefs = vstack([bi.ravel(), ai.ravel()])
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else:
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else:
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coefs = vstack([ci.ravel(), bi.ravel(), ai.ravel()])
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coefs = vstack([ci.ravel(), bi.ravel(), ai.ravel()])
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#end
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else:
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else:
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coefs = vstack([di.ravel(), ci.ravel(), bi.ravel(), ai.ravel()])
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coefs = vstack([di.ravel(), ci.ravel(), bi.ravel(), ai.ravel()])
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@ -566,9 +568,126 @@ class SmoothSpline(PPform):
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ddydx = diff(dydx, axis=0)
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ddydx = diff(dydx, axis=0)
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sp.linalg.use_solver(useUmfpack=True)
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sp.linalg.use_solver(useUmfpack=True)
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u = 2 * sp.linalg.spsolve((QQ + QQ.T), ddydx)
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u = 2 * sp.linalg.spsolve((QQ + QQ.T), ddydx)
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#faster than u=QQ\(Q' * yi);
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return u.reshape(n - 2, -1), p
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return u.reshape(n - 2, -1), p
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def _edge_case(m0, d1):
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return np.where((d1==0) | (m0==0), 0.0, 1.0/(1.0/m0+1.0/d1))
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def pchip_slopes(x, y):
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# Determine the derivatives at the points y_k, d_k, by using
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# PCHIP algorithm is:
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# We choose the derivatives at the point x_k by
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# Let m_k be the slope of the kth segment (between k and k+1)
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# If m_k=0 or m_{k-1}=0 or sgn(m_k) != sgn(m_{k-1}) then d_k == 0
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# else use weighted harmonic mean:
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# w_1 = 2h_k + h_{k-1}, w_2 = h_k + 2h_{k-1}
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# 1/d_k = 1/(w_1 + w_2)*(w_1 / m_k + w_2 / m_{k-1})
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# where h_k is the spacing between x_k and x_{k+1}
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hk = x[1:] - x[:-1]
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mk = (y[1:] - y[:-1]) / hk
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smk = np.sign(mk)
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condition = ((smk[1:] != smk[:-1]) | (mk[1:]==0) | (mk[:-1]==0))
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w1 = 2*hk[1:] + hk[:-1]
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w2 = hk[1:] + 2*hk[:-1]
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whmean = 1.0/(w1+w2)*(w1/mk[1:] + w2/mk[:-1])
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dk = np.zeros_like(y)
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dk[1:-1][condition] = 0.0
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dk[1:-1][~condition] = 1.0/whmean[~condition]
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# For end-points choose d_0 so that 1/d_0 = 1/m_0 + 1/d_1 unless
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# one of d_1 or m_0 is 0, then choose d_0 = 0
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dk[0] = _edge_case(mk[0],dk[1])
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dk[-1] = _edge_case(mk[-1],dk[-2])
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return dk
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def slopes2(x,y, method='parabola', tension=0, monotone=True):
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'''
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Return estimated slopes y'(x)
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Parameters
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----------
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x, y : array-like
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array containing the x- and y-data, respectively.
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x must be sorted low to high... (no repeats) while
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y can have repeated values.
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method : string
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defining method of estimation for yp. Valid options are:
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'Catmull-Rom' yp = (y[k+1]-y[k-1])/(x[k+1]-x[k-1])
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'Cardinal' yp = (1-tension) * (y[k+1]-y[k-1])/(x[k+1]-x[k-1])
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'parabola'
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'secant' average secants
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yp = 0.5*((y[k+1]-y[k])/(x[k+1]-x[k]) + (y[k]-y[k-1])/(x[k]-x[k-1]))
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tension : real scalar between 0 and 1.
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tension parameter used in Cardinal method
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monotone : bool
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If True modifies yp to preserve monoticity
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Returns
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-------
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yp : ndarray
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estimated slope
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References:
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-----------
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Wikipedia: Monotone cubic interpolation
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Cubic Hermite spline
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'''
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x = np.asarray(x, np.float_)
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y = np.asarray(y, np.float_)
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yp = np.zeros(y.shape, np.float_)
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dx = x[1:] - x[:-1]
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# Compute the slopes of the secant lines between successive points
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dydx = (y[1:] - y[:-1]) / dx
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method = method.lower()
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if method.startswith('parabola'):
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yp[1:-1] = (dydx[:-1] * dx[1:] + dydx[1:] * dx[:-1]) / (dx[1:] + dx[:-1])
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yp[0] = 2.0 * dydx[0] - yp[1]
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yp[-1] = 2.0 * dydx[-1] - yp[-2]
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else:
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# At the endpoints - use one-sided differences
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yp[0] = dydx[0]
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yp[-1] = dydx[-1]
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if method.startswith('secant'):
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# In the middle - use the average of the secants
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yp[1:-1] = (dydx[:-1] + dydx[1:]) / 2.0
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else: # Cardinal or Catmull-Rom method
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yp[1:-1] = (y[2:] - y[:-2]) / (x[2:] - x[:-2])
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if method.startswith('cardinal'):
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yp = (1-tension) * yp
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if monotone:
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# Special case: intervals where y[k] == y[k+1]
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# Setting these slopes to zero guarantees the spline connecting
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# these points will be flat which preserves monotonicity
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ii, = (dydx == 0.0).nonzero()
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yp[ii] = 0.0
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yp[ii+1] = 0.0
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alpha = yp[:-1]/dydx
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beta = yp[1:]/dydx
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dist = alpha**2 + beta**2
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tau = 3.0 / np.sqrt(dist)
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# To prevent overshoot or undershoot, restrict the position vector
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# (alpha, beta) to a circle of radius 3. If (alpha**2 + beta**2)>9,
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# then set m[k] = tau[k]alpha[k]delta[k] and m[k+1] = tau[k]beta[b]delta[k]
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# where tau = 3/sqrt(alpha**2 + beta**2).
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# Find the indices that need adjustment
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indices_to_fix, = (dist > 9.0).nonzero()
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for ii in indices_to_fix:
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yp[ii] = tau[ii] * alpha[ii] * dydx[ii]
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yp[ii+1] = tau[ii] * beta[ii] * dydx[ii]
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return yp
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def slopes(x, y):
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def slopes(x, y):
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"""
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"""
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@ -610,6 +729,117 @@ def slopes(x, y):
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yp[-1] = 2.0 * dy[-1] / dx[-1] - yp[-2]
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yp[-1] = 2.0 * dy[-1] / dx[-1] - yp[-2]
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return yp
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return yp
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class StinemanInterp(object):
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'''
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Returns the values of an interpolating function that runs through a set of points according to the algorithm of Stineman (1980).
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Parameters
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---------
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x,y : array-like
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coordinates of points defining the interpolating function.
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yp : array-like
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slopes of the interpolating function at x. Optional: only given if they are known, else the argument is not used.
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method : string
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method for computing the slope at the given points if the slope is not known. With method=
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"parabola" calculates the slopes from a parabola through every three points.
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Notes
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-----
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The interpolation method is described in an article by Russell W. Stineman (1980)
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According to Stineman, the interpolation procedure has "the following properties:
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If values of the ordinates of the specified points change monotonically, and the slopes of the line segments joining
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the points change monotonically, then the interpolating curve and its slope will change monotonically.
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If the slopes of the line segments joining the specified points change monotonically, then the slopes of the interpolating
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curve will change monotonically. Suppose that the conditions in (1) or (2) are satisfied by a set of points, but a small
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change in the ordinate or slope at one of the points will result conditions (1) or (2) being not longer satisfied. Then
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making this small change in the ordinate or slope at a point will cause no more than a small change in the interpolating
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curve." The method is based on rational interpolation with specially chosen rational functions to satisfy the above three
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conditions.
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Slopes computed at the given points with the methods provided by the `StinemanInterp' function satisfy Stineman's requirements.
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The original method suggested by Stineman (method="scaledstineman", the default, and "stineman") result in lower slopes near
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abrupt steps or spikes in the point sequence, and therefore a smaller tendency for overshooting. The method based on a second
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degree polynomial (method="parabola") provides better approximation to smooth functions, but it results in in higher slopes
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near abrupt steps or spikes and can lead to some overshooting where Stineman's method does not. Both methods lead to much
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less tendency for `spurious' oscillations than traditional interplation methods based on polynomials, such as splines
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(see the examples section).
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Stineman states that "The complete assurance that the procedure will never generate `wild' points makes it attractive as a
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general purpose procedure".
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This interpolation method has been implemented in Matlab and R in addition to Python.
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Examples
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--------
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>>> import wafo.interpolate as wi
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>>> x = linspace(0,2*pi,20)
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>>> y = sin(x); yp = cos(x)
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>>> xi = linspace(0,2*pi,40);
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>>> yi = wi.StinemanInterp(x,y)(xi)
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>>> yi1 = wi.CubicHermiteSpline(x,y, yp)(xi)
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>>> yi2 = wi.Pchip(x,y, method='parabola')(xi)
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>>> plt.subplot(211)
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>>> plt.plot(x,y,'o',xi,yi,'r', xi,yi1, 'g', xi,yi1, 'b')
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>>> plt.subplot(212)
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>>> plt.plot(xi,np.abs(sin(xi)-yi), 'r', xi, np.abs(sin(xi)-yi1), 'g', xi, np.abs(sin(xi)-yi2), 'b')
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References
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----------
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Stineman, R. W. A Consistently Well Behaved Method of Interpolation. Creative Computing (1980), volume 6, number 7, p. 54-57.
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See Also
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--------
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slopes, Pchip
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'''
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def __init__(self, x,y,yp=None,method='parabola'):
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if yp is None:
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yp = slopes2(x, y, method)
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self.x = np.asarray(x, np.float_)
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self.y = np.asarray(y, np.float_)
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self.yp = np.asarray(yp, np.float_)
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def __call__(self, xi):
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xi = np.asarray(xi, np.float_)
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x = self.x
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y = self.y
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yp = self.yp
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# calculate linear slopes
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dx = x[1:] - x[:-1]
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dy = y[1:] - y[:-1]
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s = dy / dx #note length of s is N-1 so last element is #N-2
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# find the segment each xi is in
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# this line actually is the key to the efficiency of this implementation
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idx = np.searchsorted(x[1:-1], xi)
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# now we have generally: x[idx[j]] <= xi[j] <= x[idx[j]+1]
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# except at the boundaries, where it may be that xi[j] < x[0] or xi[j] > x[-1]
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# the y-values that would come out from a linear interpolation:
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sidx = s.take(idx)
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xidx = x.take(idx)
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yidx = y.take(idx)
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xidxp1 = x.take(idx + 1)
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yo = yidx + sidx * (xi - xidx)
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# the difference that comes when using the slopes given in yp
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dy1 = (yp.take(idx) - sidx) * (xi - xidx) # using the yp slope of the left point
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dy2 = (yp.take(idx + 1) - sidx) * (xi - xidxp1) # using the yp slope of the right point
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dy1dy2 = dy1 * dy2
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# The following is optimized for Python. The solution actually
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# does more calculations than necessary but exploiting the power
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# of numpy, this is far more efficient than coding a loop by hand
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# in Python
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dy1mdy2 = np.where(dy1dy2,dy1-dy2,np.inf)
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dy1pdy2 = np.where(dy1dy2,dy1+dy2,np.inf)
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yi = yo + dy1dy2 * np.choose(np.array(np.sign(dy1dy2), np.int32) + 1,
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((2 * xi - xidx - xidxp1) / ((dy1mdy2) * (xidxp1 - xidx)),
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0.0,
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1 / (dy1pdy2)))
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return yi
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def stineman_interp(xi, x, y, yp=None):
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def stineman_interp(xi, x, y, yp=None):
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"""
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"""
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@ -703,6 +933,80 @@ def stineman_interp(xi, x, y, yp=None):
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1 / (dy1pdy2)))
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1 / (dy1pdy2)))
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return yi
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return yi
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class CubicHermiteSpline(PiecewisePolynomial):
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'''
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Piecewise Cubic Hermite Interpolation using Catmull-Rom
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method for computing the slopes.
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'''
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def __init__(self, x, y, yp=None, method='Catmull-Rom'):
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if yp is None:
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yp = slopes2(x, y, method, monotone=False)
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super(CubicHermiteSpline, self).__init__(x, zip(y,yp), orders=3)
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class Pchip(PiecewisePolynomial):
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"""PCHIP 1-d monotonic cubic interpolation
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Description
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-----------
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x and y are arrays of values used to approximate some function f:
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y = f(x)
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This class factory function returns a callable class whose __call__ method
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uses monotonic cubic, interpolation to find the value of new points.
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Parameters
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----------
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x : array
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A 1D array of monotonically increasing real values. x cannot
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include duplicate values (otherwise f is overspecified)
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y : array
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A 1-D array of real values. y's length along the interpolation
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axis must be equal to the length of x.
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Assumes x is sorted in monotonic order (e.g. x[1] > x[0])
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Example
|
|
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|
|
|
|
|
-------
|
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|
|
>>> import wafo.interpolate as wi
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|
# Create a step function (will demonstrate monotonicity)
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|
>>> x = np.arange(7.0) - 3.0
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>>> y = np.array([-1.0, -1,-1,0,1,1,1])
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# Interpolate using monotonic piecewise Hermite cubic spline
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>>> xvec = np.arange(599.)/100. - 3.0
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>>> yvec = wi.Pchip(x, y)(xvec)
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# Call the Scipy cubic spline interpolator
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>>> from scipy.interpolate import interpolate
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>>> function = interpolate.interp1d(x, y, kind='cubic')
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>>> yvec1 = function(xvec)
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# Non-montonic cubic Hermite spline interpolator using
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|
|
# Catmul-Rom method for computing slopes...
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>>> yvec2 = wi.CubicHermiteSpline(x,y)(xvec)
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>>> yvec3 = wi.StinemanInterp(x, y)(xvec)
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|
|
# Plot the results
|
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|
>>> plt.plot(x, y, 'ro')
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|
>>> plt.plot(xvec, yvec, 'b')
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>>> plt.plot(xvec, yvec1, 'k')
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>>> plt.plot(xvec, yvec2, 'g')
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>>> plt.plot(xvec, yvec3, 'm')
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|
>>> plt.title("pchip() step function test")
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>>> plt.xlabel("X")
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>>> plt.ylabel("Y")
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|
>>> plt.title("Comparing pypchip() vs. Scipy interp1d() vs. non-monotonic CHS")
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|
>>> legends = ["Data", "pypchip()", "interp1d","CHS", 'SI']
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|
>>> plt.legend(legends, loc="upper left")
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|
>>> plt.show()
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|
"""
|
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|
|
def __init__(self, x, y, yp=None, method='secant'):
|
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|
|
if yp is None:
|
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|
|
yp = slopes2(x, y, method=method, monotone=True)
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super(Pchip, self).__init__(x, zip(y,yp), orders=3)
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|
|
def test_smoothing_spline():
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|
|
def test_smoothing_spline():
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|
|
x = linspace(0, 2 * pi + pi / 4, 20)
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|
x = linspace(0, 2 * pi + pi / 4, 20)
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|
y = sin(x) #+ np.random.randn(x.size)
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y = sin(x) #+ np.random.randn(x.size)
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per.andreas.brodtkorb
13 years ago