I am currently working with astronomical data among which I have comet images. I would like to remove the background sky gradient in these images due to the time of capture
If anyone is looking for fitting a polynomial of a specific order (rather than polynomials where the highest power is equal to order
, you can make this adjustment to the accepted answer's polyfit
and polyval
:
instead of:
ij = itertools.product(range(order+1), range(order+1))
which, for order=2
gives [(0, 0), (0, 1), (0, 2), (1, 0), (1, 1), (1, 2), (2, 0), (2, 1), (2, 2)]
(aka up to a 4th degree polynomial), you can use
def xy_powers(order):
powers = itertools.product(range(order + 1), range(order + 1))
return [tup for tup in powers if sum(tup) <= order]
This returns [(0, 0), (0, 1), (0, 2), (1, 0), (1, 1), (2, 0)]
for order=2
Griddata uses a spline fitting. A 3rd order spline is not the same thing as a 3rd order polynomial (instead, it's a different 3rd order polynomial at every point).
If you just want to fit a 2D, 3rd order polynomial to your data, then do something like the following to estimate the 16 coefficients using all of your data points.
import itertools
import numpy as np
import matplotlib.pyplot as plt
def main():
# Generate Data...
numdata = 100
x = np.random.random(numdata)
y = np.random.random(numdata)
z = x**2 + y**2 + 3*x**3 + y + np.random.random(numdata)
# Fit a 3rd order, 2d polynomial
m = polyfit2d(x,y,z)
# Evaluate it on a grid...
nx, ny = 20, 20
xx, yy = np.meshgrid(np.linspace(x.min(), x.max(), nx),
np.linspace(y.min(), y.max(), ny))
zz = polyval2d(xx, yy, m)
# Plot
plt.imshow(zz, extent=(x.min(), y.max(), x.max(), y.min()))
plt.scatter(x, y, c=z)
plt.show()
def polyfit2d(x, y, z, order=3):
ncols = (order + 1)**2
G = np.zeros((x.size, ncols))
ij = itertools.product(range(order+1), range(order+1))
for k, (i,j) in enumerate(ij):
G[:,k] = x**i * y**j
m, _, _, _ = np.linalg.lstsq(G, z)
return m
def polyval2d(x, y, m):
order = int(np.sqrt(len(m))) - 1
ij = itertools.product(range(order+1), range(order+1))
z = np.zeros_like(x)
for a, (i,j) in zip(m, ij):
z += a * x**i * y**j
return z
main()
The following implementation of polyfit2d
uses the available numpy methods numpy.polynomial.polynomial.polyvander2d
and numpy.polynomial.polynomial.polyval2d
#!/usr/bin/env python3
import unittest
def polyfit2d(x, y, f, deg):
from numpy.polynomial import polynomial
import numpy as np
x = np.asarray(x)
y = np.asarray(y)
f = np.asarray(f)
deg = np.asarray(deg)
vander = polynomial.polyvander2d(x, y, deg)
vander = vander.reshape((-1,vander.shape[-1]))
f = f.reshape((vander.shape[0],))
c = np.linalg.lstsq(vander, f)[0]
return c.reshape(deg+1)
class MyTest(unittest.TestCase):
def setUp(self):
return self
def test_1(self):
self._test_fit(
[-1,2,3],
[ 4,5,6],
[[1,2,3],[4,5,6],[7,8,9]],
[2,2])
def test_2(self):
self._test_fit(
[-1,2],
[ 4,5],
[[1,2],[4,5]],
[1,1])
def test_3(self):
self._test_fit(
[-1,2,3],
[ 4,5],
[[1,2],[4,5],[7,8]],
[2,1])
def test_4(self):
self._test_fit(
[-1,2,3],
[ 4,5],
[[1,2],[4,5],[0,0]],
[2,1])
def test_5(self):
self._test_fit(
[-1,2,3],
[ 4,5],
[[1,2],[4,5],[0,0]],
[1,1])
def _test_fit(self, x, y, c, deg):
from numpy.polynomial import polynomial
import numpy as np
X = np.array(np.meshgrid(x,y))
f = polynomial.polyval2d(X[0], X[1], c)
c1 = polyfit2d(X[0], X[1], f, deg)
np.testing.assert_allclose(c1,
np.asarray(c)[:deg[0]+1,:deg[1]+1],
atol=1e-12)
unittest.main()
According to the principle of Least squares, and imitate Kington's style, while move argument m to argument m_1 and argument m_2.
import numpy as np
import matplotlib.pyplot as plt
import itertools
# w = (Phi^T Phi)^{-1} Phi^T t
# where Phi_{k, j + i (m_2 + 1)} = x_k^i y_k^j,
# t_k = z_k,
# i = 0, 1, ..., m_1,
# j = 0, 1, ..., m_2,
# k = 0, 1, ..., n - 1
def polyfit2d(x, y, z, m_1, m_2):
# Generate Phi by setting Phi as x^i y^j
nrows = x.size
ncols = (m_1 + 1) * (m_2 + 1)
Phi = np.zeros((nrows, ncols))
ij = itertools.product(range(m_1 + 1), range(m_2 + 1))
for h, (i, j) in enumerate(ij):
Phi[:, h] = x ** i * y ** j
# Generate t by setting t as Z
t = z
# Generate w by solving (Phi^T Phi) w = Phi^T t
w = np.linalg.solve(Phi.T.dot(Phi), (Phi.T.dot(t)))
return w
# t' = Phi' w
# where Phi'_{k, j + i (m_2 + 1)} = x'_k^i y'_k^j
# t'_k = z'_k,
# i = 0, 1, ..., m_1,
# j = 0, 1, ..., m_2,
# k = 0, 1, ..., n' - 1
def polyval2d(x_, y_, w, m_1, m_2):
# Generate Phi' by setting Phi' as x'^i y'^j
nrows = x_.size
ncols = (m_1 + 1) * (m_2 + 1)
Phi_ = np.zeros((nrows, ncols))
ij = itertools.product(range(m_1 + 1), range(m_2 + 1))
for h, (i, j) in enumerate(ij):
Phi_[:, h] = x_ ** i * y_ ** j
# Generate t' by setting t' as Phi' w
t_ = Phi_.dot(w)
# Generate z_ by setting z_ as t_
z_ = t_
return z_
if __name__ == "__main__":
# Generate x, y, z
n = 100
x = np.random.random(n)
y = np.random.random(n)
z = x ** 2 + y ** 2 + 3 * x ** 3 + y + np.random.random(n)
# Generate w
w = polyfit2d(x, y, z, m_1=3, m_2=2)
# Generate x', y', z'
n_ = 1000
x_, y_ = np.meshgrid(np.linspace(x.min(), x.max(), n_),
np.linspace(y.min(), y.max(), n_))
z_ = np.zeros((n_, n_))
for i in range(n_):
z_[i, :] = polyval2d(x_[i, :], y_[i, :], w, m_1=3, m_2=2)
# Plot
plt.imshow(z_, extent=(x_.min(), y_.max(), x_.max(), y_.min()))
plt.scatter(x, y, c=z)
plt.show()