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14.4 Gram-Schmidt & Orthogonal Complements 261<br />

We can check that P T P = I by a lengthy computation, or more simply, notice<br />

that<br />

(P T P ) =<br />

=<br />

⎛<br />

⎝<br />

u T 1<br />

u T 2<br />

u T 3<br />

⎞<br />

⎠ ( u 1 u 2 u 3<br />

)<br />

⎛<br />

1 0<br />

⎞<br />

0<br />

⎝0 1 0⎠ .<br />

0 0 1<br />

Above we are using orthonormality of the u i and the fact that matrix multiplication<br />

amounts to taking dot products between rows and columns. It is also very important<br />

to realize that the columns of an orthogonal matrix are made from an orthonormal<br />

set of vectors.<br />

Orthonormal Change of Basis and Diagonal Matrices. Suppose D is a diagonal<br />

matrix and we are able to use an orthogonal matrix P to change to a new basis. Then<br />

the matrix M of D in the new basis is:<br />

Now we calculate the transpose of M.<br />

The matrix M = P DP T is symmetric!<br />

M = P DP −1 = P DP T .<br />

M T = (P DP T ) T<br />

= (P T ) T D T P T<br />

= P DP T<br />

= M<br />

14.4 Gram-Schmidt & Orthogonal Complements<br />

Given a vector v and some other vector u not in span {v} we can construct<br />

the new vector<br />

v ⊥ := v − u · v u · u u .<br />

261

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