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@ -212,55 +212,7 @@ def romberg(fun, a, b, releps=1e-3, abseps=1e-3):
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return res, abserr
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def h_roots(n, method='newton'):
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'''
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Returns the roots (x) of the nth order Hermite polynomial,
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H_n(x), and weights (w) to use in Gaussian Quadrature over
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[-inf,inf] with weighting function exp(-x**2).
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Parameters
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----------
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n : integer
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number of roots
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method : 'newton' or 'eigenvalue'
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uses Newton Raphson to find zeros of the Hermite polynomial (Fast)
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or eigenvalue of the jacobi matrix (Slow) to obtain the nodes and
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weights, respectively.
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Returns
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-------
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x : ndarray
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roots
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w : ndarray
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weights
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Example
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-------
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>>> import numpy as np
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>>> x, w = h_roots(10)
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>>> np.allclose(np.sum(x*w), -5.2516042729766621e-19)
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True
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See also
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|
|
--------
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|
qrule, gaussq
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|
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References
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|
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|
----------
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[1] Golub, G. H. and Welsch, J. H. (1969)
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'Calculation of Gaussian Quadrature Rules'
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Mathematics of Computation, vol 23,page 221-230,
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[2]. Stroud and Secrest (1966), 'gaussian quadrature formulas',
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prentice-hall, Englewood cliffs, n.j.
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'''
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if not method.startswith('n'):
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return ort.h_roots(n)
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else:
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sqrt = np.sqrt
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max_iter = 10
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releps = 3e-14
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def _h_roots_newton(n, releps=3e-14, max_iter=10):
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C = [9.084064e-01, 5.214976e-02, 2.579930e-03, 3.986126e-03]
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# PIM4=0.7511255444649425
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PIM4 = np.pi ** (-1. / 4)
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@ -309,28 +261,27 @@ def h_roots(n, method='newton'):
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break
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else:
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warnings.warn('too many iterations!')
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w = 2. / pp ** 2
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return _expand_roots(z, w, n, m)
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# x = np.empty(n)
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# w = np.empty(n)
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# x[0:m] = z # Store the root
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# x[n - 1:n - m - 1:-1] = -z # and its symmetric counterpart.
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# w[0:m] = 2. / pp ** 2 # Compute the weight
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# w[n - 1:n - m - 1:-1] = w[0:m] # and its symmetric counterpart.
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# return x, w
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x = np.empty(n)
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w = np.empty(n)
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x[0:m] = z # Store the root
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x[n - 1:n - m - 1:-1] = -z # and its symmetric counterpart.
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w[0:m] = 2. / pp ** 2 # Compute the weight
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w[n - 1:n - m - 1:-1] = w[0:m] # and its symmetric counterpart.
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return x, w
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|
|
def j_roots(n, alpha, beta, method='newton'):
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|
|
def h_roots(n, method='newton'):
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|
|
'''
|
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|
|
Returns the roots of the nth order Jacobi polynomial, P^(alpha,beta)_n(x)
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|
|
and weights (w) to use in Gaussian Quadrature over [-1,1] with weighting
|
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|
|
function (1-x)**alpha (1+x)**beta with alpha,beta > -1.
|
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|
|
Returns the roots (x) of the nth order Hermite polynomial,
|
|
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|
|
H_n(x), and weights (w) to use in Gaussian Quadrature over
|
|
|
|
|
[-inf,inf] with weighting function exp(-x**2).
|
|
|
|
|
|
|
|
|
|
Parameters
|
|
|
|
|
----------
|
|
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|
|
n : integer
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|
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|
|
number of roots
|
|
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|
|
alpha,beta : scalars
|
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|
|
|
defining shape of Jacobi polynomial
|
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|
|
|
method : 'newton' or 'eigenvalue'
|
|
|
|
|
uses Newton Raphson to find zeros of the Hermite polynomial (Fast)
|
|
|
|
|
or eigenvalue of the jacobi matrix (Slow) to obtain the nodes and
|
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|
|
@ -343,20 +294,19 @@ def j_roots(n, alpha, beta, method='newton'):
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w : ndarray
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|
|
weights
|
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|
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|
|
Example
|
|
|
|
|
--------
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|
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|
|
>>> [x,w]= j_roots(10,0,0)
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|
|
>>> sum(x*w)
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|
|
2.7755575615628914e-16
|
|
|
|
|
-------
|
|
|
|
|
>>> import numpy as np
|
|
|
|
|
>>> x, w = h_roots(10)
|
|
|
|
|
>>> np.allclose(np.sum(x*w), -5.2516042729766621e-19)
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|
|
|
|
True
|
|
|
|
|
|
|
|
|
|
See also
|
|
|
|
|
--------
|
|
|
|
|
qrule, gaussq
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
Reference
|
|
|
|
|
---------
|
|
|
|
|
References
|
|
|
|
|
----------
|
|
|
|
|
[1] Golub, G. H. and Welsch, J. H. (1969)
|
|
|
|
|
'Calculation of Gaussian Quadrature Rules'
|
|
|
|
|
Mathematics of Computation, vol 23,page 221-230,
|
|
|
|
@ -366,11 +316,11 @@ def j_roots(n, alpha, beta, method='newton'):
|
|
|
|
|
'''
|
|
|
|
|
|
|
|
|
|
if not method.startswith('n'):
|
|
|
|
|
[x, w] = ort.j_roots(n, alpha, beta)
|
|
|
|
|
else:
|
|
|
|
|
max_iter = 10
|
|
|
|
|
releps = 3e-14
|
|
|
|
|
return ort.h_roots(n)
|
|
|
|
|
return _h_roots_newton(n)
|
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|
|
|
|
|
|
|
|
|
|
|
|
|
def _j_roots_newton(n, alpha, beta, releps=3e-14, max_iter=10):
|
|
|
|
|
# Initial approximations to the roots go into z.
|
|
|
|
|
alfbet = alpha + beta
|
|
|
|
|
|
|
|
|
@ -415,14 +365,64 @@ def j_roots(n, alpha, beta, method='newton'):
|
|
|
|
|
else:
|
|
|
|
|
warnings.warn('too many iterations in jrule')
|
|
|
|
|
|
|
|
|
|
x = z # %Store the root and the weight.
|
|
|
|
|
x = z # Store the root and the weight.
|
|
|
|
|
f = (sp.gammaln(alpha + n) + sp.gammaln(beta + n) -
|
|
|
|
|
sp.gammaln(n + 1) - sp.gammaln(alpha + beta + n + 1))
|
|
|
|
|
w = (np.exp(f) * tmp * 2 ** alfbet / (pp * L[k0, :]))
|
|
|
|
|
|
|
|
|
|
return x, w
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
def j_roots(n, alpha, beta, method='newton'):
|
|
|
|
|
'''
|
|
|
|
|
Returns the roots of the nth order Jacobi polynomial, P^(alpha,beta)_n(x)
|
|
|
|
|
and weights (w) to use in Gaussian Quadrature over [-1,1] with weighting
|
|
|
|
|
function (1-x)**alpha (1+x)**beta with alpha,beta > -1.
|
|
|
|
|
|
|
|
|
|
Parameters
|
|
|
|
|
----------
|
|
|
|
|
n : integer
|
|
|
|
|
number of roots
|
|
|
|
|
alpha,beta : scalars
|
|
|
|
|
defining shape of Jacobi polynomial
|
|
|
|
|
method : 'newton' or 'eigenvalue'
|
|
|
|
|
uses Newton Raphson to find zeros of the Hermite polynomial (Fast)
|
|
|
|
|
or eigenvalue of the jacobi matrix (Slow) to obtain the nodes and
|
|
|
|
|
weights, respectively.
|
|
|
|
|
|
|
|
|
|
Returns
|
|
|
|
|
-------
|
|
|
|
|
x : ndarray
|
|
|
|
|
roots
|
|
|
|
|
w : ndarray
|
|
|
|
|
weights
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
Example
|
|
|
|
|
--------
|
|
|
|
|
>>> [x,w]= j_roots(10,0,0)
|
|
|
|
|
>>> sum(x*w)
|
|
|
|
|
2.7755575615628914e-16
|
|
|
|
|
|
|
|
|
|
See also
|
|
|
|
|
--------
|
|
|
|
|
qrule, gaussq
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
Reference
|
|
|
|
|
---------
|
|
|
|
|
[1] Golub, G. H. and Welsch, J. H. (1969)
|
|
|
|
|
'Calculation of Gaussian Quadrature Rules'
|
|
|
|
|
Mathematics of Computation, vol 23,page 221-230,
|
|
|
|
|
|
|
|
|
|
[2]. Stroud and Secrest (1966), 'gaussian quadrature formulas',
|
|
|
|
|
prentice-hall, Englewood cliffs, n.j.
|
|
|
|
|
'''
|
|
|
|
|
|
|
|
|
|
if not method.startswith('n'):
|
|
|
|
|
return ort.j_roots(n, alpha, beta)
|
|
|
|
|
return _j_roots_newton(n, alpha, beta)
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
def la_roots(n, alpha=0, method='newton'):
|
|
|
|
|
'''
|
|
|
|
|
Returns the roots (x) of the nth order generalized (associated) Laguerre
|
|
|
|
@ -471,9 +471,11 @@ def la_roots(n, alpha=0, method='newton'):
|
|
|
|
|
|
|
|
|
|
if not method.startswith('n'):
|
|
|
|
|
return ort.la_roots(n, alpha)
|
|
|
|
|
else:
|
|
|
|
|
max_iter = 10
|
|
|
|
|
releps = 3e-14
|
|
|
|
|
return _la_roots_newton(n, alpha)
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
def _la_roots_newton(n, alpha, releps=3e-14, max_iter=10):
|
|
|
|
|
|
|
|
|
|
C = [9.084064e-01, 5.214976e-02, 2.579930e-03, 3.986126e-03]
|
|
|
|
|
|
|
|
|
|
# Initial approximations to the roots go into z.
|
|
|
|
@ -527,68 +529,57 @@ def la_roots(n, alpha=0, method='newton'):
|
|
|
|
|
return x, w
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
def p_roots(n, method='newton', a=-1, b=1):
|
|
|
|
|
'''
|
|
|
|
|
Returns the roots (x) of the nth order Legendre polynomial, P_n(x),
|
|
|
|
|
and weights (w) to use in Gaussian Quadrature over [-1,1] with weighting
|
|
|
|
|
function 1.
|
|
|
|
|
|
|
|
|
|
Parameters
|
|
|
|
|
----------
|
|
|
|
|
n : integer
|
|
|
|
|
number of roots
|
|
|
|
|
method : 'newton' or 'eigenvalue'
|
|
|
|
|
uses Newton Raphson to find zeros of the Hermite polynomial (Fast)
|
|
|
|
|
or eigenvalue of the jacobi matrix (Slow) to obtain the nodes and
|
|
|
|
|
weights, respectively.
|
|
|
|
|
|
|
|
|
|
Returns
|
|
|
|
|
-------
|
|
|
|
|
x : ndarray
|
|
|
|
|
roots
|
|
|
|
|
w : ndarray
|
|
|
|
|
weights
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
Example
|
|
|
|
|
-------
|
|
|
|
|
Integral of exp(x) from a = 0 to b = 3 is: exp(3)-exp(0)=
|
|
|
|
|
>>> import numpy as np
|
|
|
|
|
>>> x, w = p_roots(11, a=0, b=3)
|
|
|
|
|
>>> np.allclose(np.sum(np.exp(x)*w), 19.085536923187668)
|
|
|
|
|
True
|
|
|
|
|
|
|
|
|
|
See also
|
|
|
|
|
--------
|
|
|
|
|
quadg.
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
References
|
|
|
|
|
----------
|
|
|
|
|
[1] Davis and Rabinowitz (1975) 'Methods of Numerical Integration',
|
|
|
|
|
page 365, Academic Press.
|
|
|
|
|
def _p_roots_newton_start(n):
|
|
|
|
|
m = int(np.fix((n + 1) / 2))
|
|
|
|
|
mm = 4 * m - 1
|
|
|
|
|
t = (np.pi / (4 * n + 2)) * np.arange(3, mm + 1, 4)
|
|
|
|
|
nn = 1 - (1 - 1 / n) / (8 * n * n)
|
|
|
|
|
xo = nn * np.cos(t)
|
|
|
|
|
return m, xo
|
|
|
|
|
|
|
|
|
|
[2] Golub, G. H. and Welsch, J. H. (1969)
|
|
|
|
|
'Calculation of Gaussian Quadrature Rules'
|
|
|
|
|
Mathematics of Computation, vol 23,page 221-230,
|
|
|
|
|
|
|
|
|
|
[3] Stroud and Secrest (1966), 'gaussian quadrature formulas',
|
|
|
|
|
prentice-hall, Englewood cliffs, n.j.
|
|
|
|
|
'''
|
|
|
|
|
def _p_roots_newton(n, ):
|
|
|
|
|
"""
|
|
|
|
|
Algorithm given by Davis and Rabinowitz in 'Methods
|
|
|
|
|
of Numerical Integration', page 365, Academic Press, 1975.
|
|
|
|
|
"""
|
|
|
|
|
m, xo = _p_roots_newton_start(n)
|
|
|
|
|
|
|
|
|
|
if not method.startswith('n'):
|
|
|
|
|
x, w = ort.p_roots(n)
|
|
|
|
|
else:
|
|
|
|
|
e1 = n * (n + 1)
|
|
|
|
|
for _j in range(2):
|
|
|
|
|
pkm1 = 1
|
|
|
|
|
pk = xo
|
|
|
|
|
for k in range(2, n + 1):
|
|
|
|
|
t1 = xo * pk
|
|
|
|
|
pkp1 = t1 - pkm1 - (t1 - pkm1) / k + t1
|
|
|
|
|
pkm1 = pk
|
|
|
|
|
pk = pkp1
|
|
|
|
|
|
|
|
|
|
m = int(np.fix((n + 1) / 2))
|
|
|
|
|
den = 1. - xo * xo
|
|
|
|
|
d1 = n * (pkm1 - xo * pk)
|
|
|
|
|
dpn = d1 / den
|
|
|
|
|
d2pn = (2. * xo * dpn - e1 * pk) / den
|
|
|
|
|
d3pn = (4. * xo * d2pn + (2 - e1) * dpn) / den
|
|
|
|
|
d4pn = (6. * xo * d3pn + (6 - e1) * d2pn) / den
|
|
|
|
|
u = pk / dpn
|
|
|
|
|
v = d2pn / dpn
|
|
|
|
|
h = -u * (1 + (.5 * u) * (v + u * (v * v - u * d3pn / (3 * dpn))))
|
|
|
|
|
p = pk + h * (dpn + (.5 * h) * (d2pn +
|
|
|
|
|
(h / 3) * (d3pn + .25 * h * d4pn)))
|
|
|
|
|
dp = dpn + h * (d2pn + (.5 * h) * (d3pn + h * d4pn / 3))
|
|
|
|
|
h = h - p / dp
|
|
|
|
|
xo = xo + h
|
|
|
|
|
|
|
|
|
|
mm = 4 * m - 1
|
|
|
|
|
t = (np.pi / (4 * n + 2)) * np.arange(3, mm + 1, 4)
|
|
|
|
|
nn = (1 - (1 - 1 / n) / (8 * n * n))
|
|
|
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xo = nn * np.cos(t)
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x = -xo - h
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fx = d1 - h * e1 * (pk + (h / 2) * (dpn + (h / 3) *
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(d2pn + (h / 4) *
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(d3pn + (.2 * h) * d4pn))))
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w = 2 * (1 - x ** 2) / (fx ** 2)
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return _expand_roots(x, w, n, m)
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if method.endswith('1'):
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def _p_roots_newton1(n, releps=1e-15, max_iter=100):
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m, xo = _p_roots_newton_start(n)
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# Compute the zeros of the N+1 Legendre Polynomial
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# using the recursion relation and the Newton-Raphson method
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@ -599,8 +590,6 @@ def p_roots(n, method='newton', a=-1, b=1):
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Lp = zeros((m,))
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dx = zeros((m,))
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releps = 1e-15
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max_iter = 100
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# Compute the zeros of the N+1 Legendre Polynomial
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# using the recursion relation and the Newton-Raphson method
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@ -632,51 +621,75 @@ def p_roots(n, method='newton', a=-1, b=1):
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x = -xo
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w = 2. / ((1 - x ** 2) * (Lp ** 2))
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else:
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# Algorithm given by Davis and Rabinowitz in 'Methods
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# of Numerical Integration', page 365, Academic Press, 1975.
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e1 = n * (n + 1)
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return _expand_roots(x, w, n, m)
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for _j in range(2):
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pkm1 = 1
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pk = xo
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for k in range(2, n + 1):
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t1 = xo * pk
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pkp1 = t1 - pkm1 - (t1 - pkm1) / k + t1
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pkm1 = pk
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pk = pkp1
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den = 1. - xo * xo
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d1 = n * (pkm1 - xo * pk)
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dpn = d1 / den
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d2pn = (2. * xo * dpn - e1 * pk) / den
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d3pn = (4. * xo * d2pn + (2 - e1) * dpn) / den
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d4pn = (6. * xo * d3pn + (6 - e1) * d2pn) / den
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u = pk / dpn
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v = d2pn / dpn
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h = (-u * (1 + (.5 * u) * (v + u *
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(v * v - u * d3pn / (3 * dpn)))))
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p = (pk + h * (dpn + (.5 * h) * (d2pn + (h / 3) *
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(d3pn + .25 * h * d4pn))))
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dp = dpn + h * (d2pn + (.5 * h) * (d3pn + h * d4pn / 3))
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h = h - p / dp
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xo = xo + h
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x = -xo - h
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fx = (d1 - h * e1 * (pk + (h / 2) *
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(dpn + (h / 3) * (d2pn + (h / 4) *
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(d3pn + (.2 * h) * d4pn)))))
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w = 2 * (1 - x ** 2) / (fx ** 2)
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def _expand_roots(x, w, n, m):
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if (m + m) > n:
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x[m - 1] = 0.0
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if not ((m + m) == n):
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m = m - 1
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x = np.hstack((x, -x[m - 1::-1]))
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w = np.hstack((w, w[m - 1::-1]))
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return x, w
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def p_roots(n, method='newton', a=-1, b=1):
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'''
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Returns the roots (x) of the nth order Legendre polynomial, P_n(x),
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and weights (w) to use in Gaussian Quadrature over [-1,1] with weighting
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|
function 1.
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Parameters
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|
----------
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|
|
n : integer
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|
number of roots
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|
method : 'newton' or 'eigenvalue'
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|
|
uses Newton Raphson to find zeros of the Hermite polynomial (Fast)
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|
|
or eigenvalue of the jacobi matrix (Slow) to obtain the nodes and
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|
|
weights, respectively.
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Returns
|
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|
-------
|
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|
|
x : ndarray
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|
roots
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|
w : ndarray
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|
weights
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|
Example
|
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|
|
-------
|
|
|
|
|
Integral of exp(x) from a = 0 to b = 3 is: exp(3)-exp(0)=
|
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|
|
>>> import numpy as np
|
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|
|
>>> x, w = p_roots(11, a=0, b=3)
|
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|
|
>>> np.allclose(np.sum(np.exp(x)*w), 19.085536923187668)
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|
|
True
|
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|
|
|
|
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|
See also
|
|
|
|
|
--------
|
|
|
|
|
quadg.
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
References
|
|
|
|
|
----------
|
|
|
|
|
[1] Davis and Rabinowitz (1975) 'Methods of Numerical Integration',
|
|
|
|
|
page 365, Academic Press.
|
|
|
|
|
|
|
|
|
|
[2] Golub, G. H. and Welsch, J. H. (1969)
|
|
|
|
|
'Calculation of Gaussian Quadrature Rules'
|
|
|
|
|
Mathematics of Computation, vol 23,page 221-230,
|
|
|
|
|
|
|
|
|
|
[3] Stroud and Secrest (1966), 'gaussian quadrature formulas',
|
|
|
|
|
prentice-hall, Englewood cliffs, n.j.
|
|
|
|
|
'''
|
|
|
|
|
|
|
|
|
|
if not method.startswith('n'):
|
|
|
|
|
x, w = ort.p_roots(n)
|
|
|
|
|
else:
|
|
|
|
|
if method.endswith('1'):
|
|
|
|
|
x, w = _p_roots_newton1(n)
|
|
|
|
|
else:
|
|
|
|
|
x, w = _p_roots_newton(n)
|
|
|
|
|
|
|
|
|
|
if (a != -1) | (b != 1):
|
|
|
|
|
# Linear map from[-1,1] to [a,b]
|
|
|
|
|