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-rw-r--r--numpy/polynomial/chebyshev.py241
1 files changed, 158 insertions, 83 deletions
diff --git a/numpy/polynomial/chebyshev.py b/numpy/polynomial/chebyshev.py
index a81085921..d66ec5ef3 100644
--- a/numpy/polynomial/chebyshev.py
+++ b/numpy/polynomial/chebyshev.py
@@ -669,6 +669,7 @@ def chebmulx(c):
Notes
-----
+
.. versionadded:: 1.5.0
"""
@@ -883,6 +884,8 @@ def chebder(c, m=1, scl=1, axis=0) :
axis : int, optional
Axis over which the derivative is taken. (Default: 0).
+ .. versionadded:: 1.7.0
+
Returns
-------
der : ndarray
@@ -990,6 +993,8 @@ def chebint(c, m=1, k=[], lbnd=0, scl=1, axis=0):
axis : int, optional
Axis over which the derivative is taken. (Default: 0).
+ .. versionadded:: 1.7.0
+
Returns
-------
S : ndarray
@@ -1185,8 +1190,6 @@ def chebval2d(x, y, c):
If `c` is a 1-D array a one is implicitly appended to its shape to make
it 2-D. The shape of the result will be c.shape[2:] + x.shape.
- .. versionadded::1.7.0
-
Parameters
----------
x, y : array_like, compatible objects
@@ -1210,6 +1213,11 @@ def chebval2d(x, y, c):
--------
chebval, chebgrid2d, chebval3d, chebgrid3d
+ Notes
+ -----
+
+ .. versionadded::1.7.0
+
"""
try:
x, y = np.array((x, y), copy=0)
@@ -1242,8 +1250,6 @@ def chebgrid2d(x, y, c):
its shape to make it 2-D. The shape of the result will be c.shape[2:] +
x.shape + y.shape.
- .. versionadded:: 1.7.0
-
Parameters
----------
x, y : array_like, compatible objects
@@ -1267,6 +1273,11 @@ def chebgrid2d(x, y, c):
--------
chebval, chebval2d, chebval3d, chebgrid3d
+ Notes
+ -----
+
+ .. versionadded::1.7.0
+
"""
c = chebval(x, c)
c = chebval(y, c)
@@ -1291,8 +1302,6 @@ def chebval3d(x, y, z, c):
shape to make it 3-D. The shape of the result will be c.shape[3:] +
x.shape.
- .. versionadded::1.7.0
-
Parameters
----------
x, y, z : array_like, compatible object
@@ -1317,6 +1326,11 @@ def chebval3d(x, y, z, c):
--------
chebval, chebval2d, chebgrid2d, chebgrid3d
+ Notes
+ -----
+
+ .. versionadded::1.7.0
+
"""
try:
x, y, z = np.array((x, y, z), copy=0)
@@ -1352,8 +1366,6 @@ def chebgrid3d(x, y, z, c):
its shape to make it 3-D. The shape of the result will be c.shape[3:] +
x.shape + yshape + z.shape.
- .. versionadded:: 1.7.0
-
Parameters
----------
x, y, z : array_like, compatible objects
@@ -1378,6 +1390,11 @@ def chebgrid3d(x, y, z, c):
--------
chebval, chebval2d, chebgrid2d, chebval3d
+ Notes
+ -----
+
+ .. versionadded::1.7.0
+
"""
c = chebval(x, c)
c = chebval(y, c)
@@ -1386,28 +1403,38 @@ def chebgrid3d(x, y, z, c):
def chebvander(x, deg) :
- """Vandermonde matrix of given degree.
+ """Pseudo-Vandermonde matrix of given degree.
+
+ Returns the pseudo-Vandermonde matrix of degree `deg` and sample points
+ `x`. The pseudo-Vandermonde matrix is defined by
+
+ .. math:: V[..., i] = T_i(x),
- Returns the Vandermonde matrix of degree `deg` and sample points `x`.
- This isn't a true Vandermonde matrix because `x` can be an arbitrary
- ndarray and the Chebyshev polynomials aren't powers. If ``V`` is the
- returned matrix and `x` is a 2d array, then the elements of ``V`` are
- ``V[i,j,k] = T_k(x[i,j])``, where ``T_k`` is the Chebyshev polynomial
- of degree ``k``.
+ where `0 <= i <= deg`. The leading indices of `V` index the elements of
+ `x` and the last index is the degree of the Chebyshev polynomial.
+
+ If `c` is a 1-D array of coefficients of length `n + 1` and `V` is the
+ matrix ``V = chebvander(x, n)``, then ``np.dot(V, c)`` and
+ ``chebval(x, c)`` are the same up to roundoff. This equivalence is
+ useful both for least squares fitting and for the evaluation of a large
+ number of Chebyshev series of the same degree and sample points.
Parameters
----------
x : array_like
- Array of points. The values are converted to double or complex
- doubles. If x is scalar it is converted to a 1D array.
- deg : integer
+ Array of points. The dtype is converted to float64 or complex128
+ depending on whether any of the elements are complex. If `x` is
+ scalar it is converted to a 1-D array.
+ deg : int
Degree of the resulting matrix.
Returns
-------
- vander : Vandermonde matrix.
- The shape of the returned matrix is ``x.shape + (deg+1,)``. The last
- index is the degree.
+ vander: ndarray
+ The pseudo Vandermonde matrix. The shape of the returned matrix is
+ ``x.shape + (deg + 1,)``, where The last index is the degree of the
+ corresponding Chebyshev polynomial. The dtype will be the same as
+ the converted `x`.
"""
ideg = int(deg)
@@ -1429,36 +1456,50 @@ def chebvander(x, deg) :
def chebvander2d(x, y, deg) :
- """Pseudo Vandermonde matrix of given degree.
-
- Returns the pseudo Vandermonde matrix for 2D Chebyshev series in `x`
- and `y`. The sample point coordinates must all have the same shape
- after conversion to arrays and the dtype will be converted to either
- float64 or complex128 depending on whether any of `x` or 'y' are
- complex. The maximum degrees of the 2D Chebyshev series in each
- variable are specified in the list `deg` in the form ``[xdeg, ydeg]``.
- The return array has the shape ``x.shape + (order,)`` if `x`, and `y`
- are arrays or ``(1, order) if they are scalars. Here order is the
- number of elements in a flattened coefficient array of original shape
- ``(xdeg + 1, ydeg + 1)``. The flattening is done so that the resulting
- pseudo Vandermonde array can be easily used in least squares fits.
+ """Pseudo-Vandermonde matrix of given degrees.
+
+ Returns the pseudo-Vandermonde matrix of degrees `deg` and sample
+ points `(x, y)`. The pseudo-Vandermonde matrix is defined by
+
+ .. math:: V[..., deg[1]*i + j] = T_i(x) * T_j(y),
+
+ where `0 <= i <= deg[0]` and `0 <= j <= deg[1]`. The leading indices of
+ `V` index the points `(x, y)` and the last index encodes the degrees of
+ the Chebyshev polynomials.
+
+ If `c` is a 2-D array of coefficients of shape `(m + 1, n + 1)` and `V`
+ is the matrix ``V = chebvander2d(x, y, [m, n])``, then
+ ``np.dot(V, c.flat)`` and ``chebval2d(x, y, c)`` are the same up to
+ roundoff. This equivalence is useful both for least squares fitting and
+ for the evaluation of a large number of 2-D Chebyshev series of the
+ same degrees and sample points.
Parameters
----------
- x,y : array_like
- Arrays of point coordinates, each of the same shape.
- deg : list
+ x, y : array_like
+ Arrays of point coordinates, all of the same shape. The dtypes
+ will be converted to either float64 or complex128 depending on
+ whether any of the elements are complex. Scalars are converted to
+ 1-D arrays.
+ deg : list of ints
List of maximum degrees of the form [x_deg, y_deg].
Returns
-------
vander2d : ndarray
- The shape of the returned matrix is described above.
+ The shape of the returned matrix is ``x.shape + (order,)``, where
+ :math:`order = (deg[0]+1)*(deg([1]+1)`. The dtype will be the same
+ as the converted `x` and `y`.
See Also
--------
chebvander, chebvander3d. chebval2d, chebval3d
+ Notes
+ -----
+
+ .. versionadded::1.7.0
+
"""
ideg = [int(d) for d in deg]
is_valid = [id == d and id >= 0 for id, d in zip(ideg, deg)]
@@ -1474,37 +1515,51 @@ def chebvander2d(x, y, deg) :
def chebvander3d(x, y, z, deg) :
- """Pseudo Vandermonde matrix of given degree.
-
- Returns the pseudo Vandermonde matrix for 3D Chebyshev series in `x`,
- `y`, or `z`. The sample point coordinates must all have the same shape
- after conversion to arrays and the dtype will be converted to either
- float64 or complex128 depending on whether any of `x`, `y`, or 'z' are
- complex. The maximum degrees of the 3D Chebeshev series in each
- variable are specified in the list `deg` in the form ``[xdeg, ydeg,
- zdeg]``. The return array has the shape ``x.shape + (order,)`` if `x`,
- `y`, and `z` are arrays or ``(1, order) if they are scalars. Here order
- is the number of elements in a flattened coefficient array of original
- shape ``(xdeg + 1, ydeg + 1, zdeg + 1)``. The flattening is done so
- that the resulting pseudo Vandermonde array can be easily used in least
- squares fits.
+ """Pseudo-Vandermonde matrix of given degrees.
+
+ Returns the pseudo-Vandermonde matrix of degrees `deg` and sample
+ points `(x, y, z)`. If `l, m, n` are the given degrees in `x, y, z`,
+ then The pseudo-Vandermonde matrix is defined by
+
+ .. math:: V[..., (m+1)(n+1)i + (n+1)j + k] = T_i(x)*T_j(y)*T_k(z),
+
+ where `0 <= i <= l`, `0 <= j <= m`, and `0 <= j <= n`. The leading
+ indices of `V` index the points `(x, y, z)` and the last index encodes
+ the degrees of the Chebyshev polynomials.
+
+ If `c` is a 3-D array of coefficients of shape `(l + 1, m + 1, n + 1)`
+ and `V` is the matrix ``V = chebvander3d(x, y, z, [l, m, n])``, then
+ ``np.dot(V, c.flat)`` and ``chebval3d(x, y, z, c)`` are the same up to
+ roundoff. This equivalence is useful both for least squares fitting and
+ for the evaluation of a large number of 3-D Chebyshev series of the
+ same degrees and sample points.
Parameters
----------
- x,y,z : array_like
- Arrays of point coordinates, each of the same shape.
- deg : list
+ x, y, z : array_like
+ Arrays of point coordinates, all of the same shape. The dtypes will
+ be converted to either float64 or complex128 depending on whether
+ any of the elements are complex. Scalars are converted to 1-D
+ arrays.
+ deg : list of ints
List of maximum degrees of the form [x_deg, y_deg, z_deg].
Returns
-------
vander3d : ndarray
- The shape of the returned matrix is described above.
+ The shape of the returned matrix is ``x.shape + (order,)``, where
+ :math:`order = (deg[0]+1)*(deg([1]+1)*(deg[2]+1)`. The dtype will
+ be the same as the converted `x`, `y`, and `z`.
See Also
--------
chebvander, chebvander3d. chebval2d, chebval3d
+ Notes
+ -----
+
+ .. versionadded::1.7.0
+
"""
ideg = [int(d) for d in deg]
is_valid = [id == d and id >= 0 for id, d in zip(ideg, deg)]
@@ -1688,15 +1743,15 @@ def chebcompanion(c):
"""Return the scaled companion matrix of c.
The basis polynomials are scaled so that the companion matrix is
- symmetric when `c` represents a single Chebyshev polynomial. This
- provides better eigenvalue estimates than the unscaled case and in the
- single polynomial case the eigenvalues are guaranteed to be real if
- np.eigvalsh is used to obtain them.
+ symmetric when `c` is aa Chebyshev basis polynomial. This provides
+ better eigenvalue estimates than the unscaled case and for basis
+ polynomials the eigenvalues are guaranteed to be real if
+ `numpy.linalg.eigvalsh` is used to obtain them.
Parameters
----------
c : array_like
- 1-d array of Legendre series coefficients ordered from low to high
+ 1-d array of Chebyshev series coefficients ordered from low to high
degree.
Returns
@@ -1704,6 +1759,11 @@ def chebcompanion(c):
mat : ndarray
Scaled companion matrix of dimensions (deg, deg).
+ Notes
+ -----
+
+ .. versionadded::1.7.0
+
"""
# c is a trimmed copy
[c] = pu.as_series([c])
@@ -1781,12 +1841,13 @@ def chebroots(c):
def chebgauss(deg):
- """Gauss Chebyshev quadrature.
+ """
+ Gauss-Chebyshev quadrature.
Computes the sample points and weights for Gauss-Chebyshev quadrature.
These sample points and weights will correctly integrate polynomials of
- degree ``2*deg - 1`` or less over the interval ``[-1, 1]`` with the
- weight function ``f(x) = 1/sqrt(1 - x**2)``.
+ degree :math:`2*deg - 1` or less over the interval :math:`[-1, 1]` with
+ the weight function :math:`f(x) = 1/\sqrt{1 - x^2}`.
Parameters
----------
@@ -1802,16 +1863,16 @@ def chebgauss(deg):
Notes
-----
- The results have only been tested up to degree 100. Higher degrees may
- be problematic. There are closed form solutions for the sample points
- and weights. If ``n = deg``, then
- ``x_i = cos(pi*(2*i - 1)/(2*n))``
- ``w_i = pi/n``
+ .. versionadded:: 1.7.0
+
+ The results have only been tested up to degree 100, higher degrees may
+ be problematic. For Gauss-Chebyshev there are closed form solutions for
+ the sample points and weights. If n = `deg`, then
+
+ .. math:: x_i = \cos(\pi (2 i - 1) / (2 n))
- where ``c`` is a constant independent of ``k`` and ``x_k`` is the k'th
- root of ``L_n``, and then scaling the results to get the right value
- when integrating 1.
+ .. math:: w_i = \pi / n
"""
ideg = int(deg)
@@ -1825,11 +1886,12 @@ def chebgauss(deg):
def chebweight(x):
- """Weight function of the Chebyshev polynomials.
+ """
+ The weight function of the Chebyshev polynomials.
- The weight function for which the Chebyshev polynomials are orthogonal.
- In this case the weight function is ``1/(1 - x**2)``. Note that the
- Chebyshev polynomials are not normalized.
+ The weight function is :math:`1/\sqrt{1 - x^2}` and the interval of
+ integration is :math:`[-1, 1]`. The Chebyshev polynomials are orthogonal, but
+ not normalized, with respect to this weight function.
Parameters
----------
@@ -1841,16 +1903,22 @@ def chebweight(x):
w : ndarray
The weight function at `x`.
+ Notes
+ -----
+
+ .. versionadded:: 1.7.0
+
"""
w = 1./(np.sqrt(1. + x) * np.sqrt(1. - x))
return w
def chebpts1(npts):
- """Chebyshev points of the first kind.
+ """
+ Chebyshev points of the first kind.
- Chebyshev points of the first kind are the set ``{cos(x_k)}``,
- where ``x_k = pi*(k + .5)/npts`` for k in ``range(npts}``.
+ The Chebyshev points of the first kind are the points ``cos(x)``,
+ where ``x = [pi*(k + .5)/npts for k in range(npts)]``.
Parameters
----------
@@ -1860,10 +1928,15 @@ def chebpts1(npts):
Returns
-------
pts : ndarray
- The Chebyshev points of the second kind.
+ The Chebyshev points of the first kind.
+
+ See Also
+ --------
+ chebpts2
Notes
-----
+
.. versionadded:: 1.5.0
"""
@@ -1878,10 +1951,11 @@ def chebpts1(npts):
def chebpts2(npts):
- """Chebyshev points of the second kind.
+ """
+ Chebyshev points of the second kind.
- Chebyshev points of the second kind are the set ``{cos(x_k)}``,
- where ``x_k = pi*/(npts - 1)`` for k in ``range(npts}``.
+ The Chebyshev points of the second kind are the points ``cos(x)``,
+ where ``x = [pi*k/(npts - 1) for k in range(npts)]``.
Parameters
----------
@@ -1895,6 +1969,7 @@ def chebpts2(npts):
Notes
-----
+
.. versionadded:: 1.5.0
"""