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Linear Algebra Exercises-n-Answers.pdf

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<strong>Answers</strong> to <strong>Exercises</strong> 187<br />

leading to this eigenspace and eigenvector.<br />

( )<br />

−2b2 ∣∣<br />

{ b<br />

b 2 ∈ C}<br />

2<br />

For λ 2 = 1 the system is<br />

leading to this.<br />

Five.II.3.22<br />

2 · b 1 + 2 · b 2 = 0<br />

−1 · b 1 − 1 · b 2 = 0<br />

( )<br />

−b2 ∣∣<br />

{ b<br />

b 2 ∈ C}<br />

2<br />

( )<br />

−2<br />

1<br />

( )<br />

−1<br />

1<br />

The characteristic equation<br />

0 =<br />

∣ −2 − x −1<br />

5 2 − x∣ = x2 + 1<br />

has the complex roots λ 1 = i and λ 2 = −i. This system<br />

For λ 1 = i Gauss’ method gives this reduction.<br />

(−2 − x) · b 1 − 1 · b 2 = 0<br />

5 · b 1 (2 − x) · b 2 = 0<br />

(−2 − i) · b 1 − 1 · b 2 = 0 (−5/(−2−i))ρ 1+ρ 2 (−2 − i) · b −→ 1 − 1 · b 2 = 0<br />

5 · b 1 − (2 − i) · b 2 = 0<br />

0 = 0<br />

(For the calculation in the lower right get a common denominator<br />

5<br />

−2 − i − (2 − i) = 5<br />

−2 − i − −2 − i<br />

5 − (−5)<br />

· (2 − i) =<br />

−2 − i −2 − i<br />

to see that it gives a 0 = 0 equation.) These are the resulting eigenspace and eigenvector.<br />

( ) ( )<br />

(1/(−2 − i))b2 ∣∣ 1/(−2 − i)<br />

{<br />

b<br />

b 2 ∈ C}<br />

2 1<br />

For λ 2 = −i the system<br />

leads to this.<br />

Five.II.3.23<br />

(−2 + i) · b 1 − 1 · b 2 = 0 (−5/(−2+i))ρ 1 +ρ 2 (−2 + i) · b −→ 1 − 1 · b 2 = 0<br />

5 · b 1 − (2 + i) · b 2 = 0<br />

0 = 0<br />

( )<br />

(1/(−2 + i))b2 ∣∣<br />

{<br />

b2 ∈ C}<br />

b 2<br />

( )<br />

1/(−2 + i)<br />

The characteristic equation is<br />

1 − x 1 1<br />

0 =<br />

0 −x 1<br />

∣ 0 0 1 − x∣ = (1 − x)2 (−x)<br />

and so the eigenvalues are λ 1 = 1 (this is a repeated root of the equation) and λ 2 = 0. For the rest,<br />

consider this system.<br />

(1 − x) · b 1 + b 2 + b 3 = 0<br />

−x · b 2 + b 3 = 0<br />

(1 − x) · b 3 = 0<br />

When x = λ 1 = 1 then the solution set is this eigenspace.<br />

⎛ ⎞<br />

1<br />

{ ⎝b<br />

0 ⎠ ∣ b 1 ∈ C}<br />

0<br />

When x = λ 2 = 0 then the solution set is this eigenspace.<br />

⎛<br />

{ ⎝ −b ⎞<br />

2<br />

b 2<br />

⎠ ∣ b 2 ∈ C}<br />

0<br />

So these are eigenvectors associated with λ 1 = 1 and λ 2 = 0.<br />

⎛<br />

⎝ 1 ⎞ ⎛<br />

0⎠<br />

⎝ −1<br />

⎞<br />

1 ⎠<br />

0 0<br />

1

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