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264 Chapter 3. Maps Between Spaces<br />

P ⊥ consists of the vectors that satisfy these two conditions.<br />

⎛<br />

⎝ 1<br />

⎞<br />

0⎠<br />

⎛<br />

⎝<br />

3<br />

v1<br />

⎞<br />

v2⎠<br />

=0<br />

⎛<br />

⎝ 0<br />

⎞<br />

1⎠<br />

⎛<br />

⎝<br />

2<br />

v1<br />

⎞<br />

v2⎠<br />

=0<br />

v3<br />

We can express those conditions more compactly as a linear system.<br />

P ⊥ ⎛<br />

= { ⎝ v1<br />

⎞<br />

v2⎠<br />

� �<br />

� 1<br />

0<br />

0<br />

1<br />

�<br />

3<br />

2<br />

⎛<br />

⎝ v1<br />

⎞<br />

� �<br />

v2⎠<br />

0<br />

= }<br />

0<br />

v3<br />

v3<br />

We are thus left with finding the nullspace of the map represented by the matrix,<br />

that is, with calculating the solution set of a homogeneous linear system.<br />

P ⊥ ⎛ ⎞<br />

v1<br />

= { ⎝v2⎠<br />

� � v1<br />

⎛ ⎞<br />

−3<br />

+3v3 =0<br />

} = {k ⎝−2⎠<br />

v2 +2v3 =0<br />

1<br />

� � k ∈ R}<br />

3.6 Example Where M is the xy-plane subspace of R 3 , what is M ⊥ ? A<br />

common first reaction is that M ⊥ is the yz-plane, but that’s not right. Some<br />

vectors from the yz-plane are not perpendicular to every vector in the xy-plane.<br />

� �<br />

1<br />

1 �⊥<br />

0<br />

� �<br />

0<br />

3<br />

2<br />

cos θ =<br />

v3<br />

v3<br />

1 · 0+1· 3+0· 2<br />

√ 1+1+0· √ 0+9+4 so θ ≈ 0.94 rad<br />

Instead M ⊥ is the z-axis, since proceeding as in the prior example and taking<br />

the natural basis for the xy-plane gives this.<br />

M ⊥ ⎛ ⎞<br />

x<br />

= { ⎝y⎠<br />

z<br />

� � �<br />

� 1 0 0<br />

0 1 0<br />

⎛ ⎞<br />

⎛ ⎞<br />

x � � x<br />

⎝y⎠<br />

0<br />

= } = { ⎝y⎠<br />

0<br />

z<br />

z<br />

� � x =0andy =0}<br />

The two examples that we’ve seen since Definition 3.4 illustrate the first<br />

sentence in that definition. The next result justifies the second sentence.<br />

3.7 Lemma Let M be a subspace of R n . The orthogonal complement of M is<br />

also a subspace. The space is the direct sum of the two R n = M ⊕ M ⊥ . And,<br />

for any �v ∈ R n , the vector �v − proj M (�v ) is perpendicular to every vector in M.<br />

Proof. First, the orthogonal complement M ⊥ is a subspace of R n because, as<br />

noted in the prior two examples, it is a nullspace.<br />

Next, we can start with any basis BM = 〈�µ1,...,�µk〉 for M and expand it to<br />

a basis for the entire space. Apply the Gram-Schmidt process to get an orthogonal<br />

basis K = 〈�κ1,...,�κn〉 for R n . This K is the concatenation of two bases<br />

〈�κ1,...,�κk〉 (with the same number of members as BM) and〈�κk+1,...,�κn〉.<br />

ThefirstisabasisforM, so if we show that the second is a basis for M ⊥ then<br />

we will have that the entire space is the direct sum of the two subspaces.

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