As before, we can easily extend this projection operator to cases where the measure of distance between $\mathbf{y}$ and the subspace $\mathbf{v}$ is weighted (i.e. non-uniform). We can accomodate these weighted distances by re-writing the projection operator as
$$ \mathbf{P}_{V} = \mathbf{V} ( \mathbf{V}^T \mathbf{Q V})^{-1} \mathbf{V}^T \mathbf{Q} $$where $\mathbf{Q}$ is positive definite matrix. Earlier, we started with a point $\mathbf{y}$ and inflated a sphere centered at $\mathbf{y}$ until it just touched the plane defined by $\mathbf{v}_i$ and this point was closest point on the subspace to $\mathbf{y}$. In the general case with a weighted distance except now we inflate an ellipsoid, not a sphere, until the ellipsoid touches the line.
The code and figure below illustrate what happens using the weighted $ \mathbf{P}_v $. It is basically the same code we used above. You can download the IPython notebook corresponding to this post and try different values on the diagonal of $\mathbf{Q}$.
x = np.linspace(0,2,50)
y = x + x**2 + np.random.randn(len(x))
V = matrix(np.vstack([ones(x.shape),x,x**2]).T)
Q = np.matrix(np.eye(V.shape[0]))
i,j =np.diag_indices_from(Q)
Q[i[:20],j[:20]]=100
R = np.matrix(np.diag([1,1,13]))*0
Pv = V*inv(V.T*Q*V+R)*V.T*Q
p=np.polyfit(x,y,2)
fig, ax = subplots()
fig.set_size_inches(5,5)
ax.plot(x,y,'o',label='data',alpha=0.3)
ax.plot(x,np.dot(Pv,y).flat,label='projection')
ax.plot(x,np.polyval(p,x),'-',label='polyfit',alpha=0.3)
ax.grid()
ax.legend(loc=0)
x = np.random.rand(50)*2
x.sort() # sort for plotting
y = x + x**2 + np.random.randn(len(x))
V = matrix(np.vstack([ones(x.shape),x,x**2]).T)
Pv = V*inv(V.T*V+eye(3)*4)*V.T
p=np.polyfit(x,y,2)
fig, ax = subplots()
fig.set_size_inches(5,5)
ax.plot(x,y,'o',label='data',alpha=0.3)
ax.plot(x,np.dot(Pv,y).flat,'-s',label='projection')
#ax.plot(x,np.polyval(p,x),'s',label='polyfit')
ax.grid()
ax.legend(loc=0);
import numpy as np
import matplotlib.pyplot as plt
from matplotlib.widgets import Slider
fig, ax = plt.subplots()
fig.set_size_inches(5,5)
plt.subplots_adjust(left=0.25, bottom=0.30,right=1)
x = np.linspace(0,2,50)
y = x + x**2 + np.sin(2*np.pi*x) + np.random.randn(len(x))
V = np.matrix(np.vstack([np.ones(x.shape),x,x**2]).T)
Q = np.matrix(np.eye(V.shape[0]))
i,j =np.diag_indices_from(Q)
#Q[i[:20],j[:20]]=100
R = np.matrix(np.diag([1,1,1]))*0
Pv = V*np.linalg.inv(V.T*Q*V+R)*V.T*Q
p=np.polyfit(x,y,2)
ax.plot(x,y,'o',label='data',alpha=0.3)
ax.set_title('err^2=%3.2f'%(np.linalg.norm(y)**2 - np.linalg.norm(np.dot(Pv,y))**2 ))
ls_line,=ax.plot(x,np.dot(Pv,y).flat,label='projection')
ax.plot(x,np.polyval(p,x),'-',label='polyfit',alpha=0.3)
ax.legend(loc=0)
ax.grid()
axw0 = plt.axes([0.25, 0.2, 0.65, 0.03] )
sw0 = Slider(axw0, 'w0', 0.1, 30.0, valinit = 1)
axw1 = plt.axes([0.25, 0.15, 0.65, 0.03] )
sw1 = Slider(axw1, 'w1', 0.1, 30.0, valinit = 1)
axw2 = plt.axes([0.25, 0.10, 0.65, 0.03] )
sw2 = Slider(axw2, 'w2', 0.1, 30.0, valinit = 1)
def update_w0(val):
w = sw0.val
R[0,0]=w
Pv = V*np.linalg.inv(V.T*Q*V+R)*V.T*Q
ls_line.set_ydata(np.dot(Pv,y).flat)
ax.set_title('err=%3.2f'%(np.linalg.norm(y)**2 - np.linalg.norm(np.dot(Pv,y))**2 ))
plt.draw()
sw0.on_changed(update_w0)
def update_w1(val):
w = sw1.val
R[1,1]=w
Pv = V*np.linalg.inv(V.T*Q*V+R)*V.T*Q
ls_line.set_ydata(np.dot(Pv,y).flat)
ax.set_title('err=%3.2f'%(np.linalg.norm(y)**2 - np.linalg.norm(np.dot(Pv,y))**2 ))
plt.draw()
sw1.on_changed(update_w1)
def update_w2(val):
w = sw2.val
R[2,2]=w
Pv = V*np.linalg.inv(V.T*Q*V+R)*V.T*Q
ls_line.set_ydata(np.dot(Pv,y).flat)
ax.set_title('err=%3.2f'%(np.linalg.norm(y)**2 - np.linalg.norm(np.dot(Pv,y))**2 ))
plt.draw()
sw2.on_changed(update_w2)
plt.show()
This post was created using the nbconvert utility from the source IPython Notebook which is available for download from the main github site for this blog. The projection concept is masterfully discussed in the classic Strang, G. (2003). Introduction to linear algebra. Wellesley Cambridge Pr. Also, some of Dr. Strang's excellent lectures are available on MIT Courseware. I highly recommend these as well as the book.