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12.2 The Eigenvalue–Eigenvector Equation 235<br />

Example 128 Let L be the <strong>linear</strong> transformation L: R 3 → R 3 given by<br />

⎛ ⎞<br />

x<br />

⎛<br />

2x + y − z<br />

⎞<br />

L ⎝y⎠ = ⎝<br />

z<br />

x + 2y − z<br />

−x − y + 2z<br />

⎠ .<br />

In the standard basis the matrix M representing L has columns Le i for each i, so:<br />

⎛ ⎞ ⎛<br />

⎞ ⎛ ⎞<br />

x 2 1 −1 x<br />

⎝y⎠<br />

↦−→<br />

L ⎝ 1 2 −1⎠<br />

⎝y⎠ .<br />

z −1 −1 2 z<br />

Then the characteristic polynomial of L is 2<br />

⎛<br />

⎞<br />

λ − 2 −1 1<br />

P M (λ) = det ⎝ −1 λ − 2 1 ⎠<br />

1 1 λ − 2<br />

= (λ − 2)[(λ − 2) 2 − 1] + [−(λ − 2) − 1] + [−(λ − 2) − 1]<br />

= (λ − 1) 2 (λ − 4) .<br />

So L has eigenvalues λ 1 = 1 (with multiplicity 2), and λ 2 = 4 (with multiplicity 1).<br />

To find the eigenvectors associated to each eigenvalue, we solve the homogeneous<br />

system (M − λ i I)X = 0 for each i.<br />

λ = 4: We set up the augmented matrix for the <strong>linear</strong> system:<br />

⎛<br />

−2 1 −1<br />

⎞<br />

0<br />

⎝ 1 −2 −1 0⎠<br />

−1 −1 −2 0<br />

∼<br />

∼<br />

⎛<br />

1 −2 −1<br />

⎞<br />

0<br />

⎝0 −3 −3 0⎠<br />

0 −3 −3 0<br />

⎛ ⎞<br />

1 0 1 0<br />

⎝0 1 1 0⎠ .<br />

0 0 0 0<br />

⎛ ⎞<br />

−1<br />

Any vector of the form t ⎝−1⎠ is then an eigenvector with eigenvalue 4; thus L<br />

1<br />

leaves a line through the origin invariant.<br />

2 It is often easier (and equivalent) to solve det(M − λI) = 0.<br />

235

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