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G.13 Orthonormal Bases and Complements 427<br />

(d) Construct an orthonormal basis for R 3 from u and v.<br />

If you did part (c) you can probably find 3 orthogonal vectors to make<br />

a orthogonal basis. All you need to do to turn this into an orthonormal<br />

basis is make these into unit vectors.<br />

(e) Test your abstract formulae starting with<br />

u = ( 1 2 0 ) and v = ( 0 1 1 ) .<br />

Try it out, and if you get stuck try drawing a sketch of the vectors you<br />

have.<br />

Hint for Review Problem 10<br />

This video shows you a way to solve problem 10 that’s different to the method<br />

described in the Lecture. The first thing is to think of<br />

⎛<br />

1 0<br />

⎞<br />

2<br />

M = ⎝−1 2 0⎠<br />

−1 2 2<br />

as a set of 3 vectors<br />

⎛ ⎞<br />

⎛ ⎞<br />

⎛ ⎞<br />

0<br />

0<br />

2<br />

v 1 = ⎝−1⎠ , v 2 = ⎝ 2⎠ , v 3 = ⎝0⎠ .<br />

−1<br />

−2<br />

2<br />

Then you need to remember that we are searching for a decomposition<br />

M = QR<br />

where Q is an orthogonal matrix. Thus the upper triangular matrix R = Q T M<br />

and Q T Q = I. Moreover, orthogonal matrices perform rotations. To see this<br />

compare the inner product u v = u T v of vectors u and v with that of Qu and<br />

Qv:<br />

(Qu) (Qv) = (Qu) T (Qv) = u T Q T Qv = u T v = u v .<br />

Since the dot product doesn’t change, we learn that Q does not change angles<br />

or lengths of vectors.<br />

Now, here’s an interesting procedure: rotate v 1 , v 2 and v 3 such that v 1 is<br />

along the x-axis, v 2 is in the xy-plane. Then if you put these in a matrix you<br />

get something of the form<br />

⎛ ⎞<br />

a b c<br />

⎝0 d e⎠<br />

0 0 f<br />

which is exactly what we want for R!<br />

427

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