Let find eigen values. For that we need the next formula:
det ( A − λ I ) = 0 \det (A - \lambda I) = 0 det ( A − λ I ) = 0
Where I I I is the identity matrix
∣ 2 − λ 1 1 2 3 − λ 2 − 2 1 2 − λ ∣ = ( 2 − λ ) 2 ( 3 − λ ) − 4 + 2 + 2 ( 3 − λ ) − 2 ( 2 − λ ) − 2 ( 2 − λ ) \left| \begin{array}{ccc}
2 - \lambda & 1 & 1 \\
2 & 3 - \lambda & 2 \\
-2 & 1 & 2 - \lambda
\end{array} \right| = (2 - \lambda)^2 (3 - \lambda) - 4 + 2 + 2(3 - \lambda) - 2(2 - \lambda) - 2(2 - \lambda) ∣ ∣ 2 − λ 2 − 2 1 3 − λ 1 1 2 2 − λ ∣ ∣ = ( 2 − λ ) 2 ( 3 − λ ) − 4 + 2 + 2 ( 3 − λ ) − 2 ( 2 − λ ) − 2 ( 2 − λ ) = − λ 3 + 7 λ 2 − 14 λ + 8 = -\lambda^3 + 7\lambda^2 - 14\lambda + 8 = − λ 3 + 7 λ 2 − 14 λ + 8 − λ 3 + 7 λ 2 − 14 λ + 8 = 0 - \lambda^3 + 7\lambda^2 - 14\lambda + 8 = 0 − λ 3 + 7 λ 2 − 14 λ + 8 = 0 λ 3 − 7 λ 2 + 14 λ − 8 = 0 \lambda^3 - 7\lambda^2 + 14\lambda - 8 = 0 λ 3 − 7 λ 2 + 14 λ − 8 = 0 ( λ − 1 ) ( λ − 2 ) ( λ − 4 ) = 0 (\lambda - 1)(\lambda - 2)(\lambda - 4) = 0 ( λ − 1 ) ( λ − 2 ) ( λ − 4 ) = 0 ∣ λ − 1 = 0 λ − 2 = 0 ⇒ ∣ λ 1 = 1 λ 2 = 2 λ 3 = 4 \left| \begin{array}{l}
\lambda - 1 = 0 \\
\lambda - 2 = 0 \Rightarrow
\end{array} \right| \begin{array}{l}
\lambda_1 = 1 \\
\lambda_2 = 2 \\
\lambda_3 = 4
\end{array} ∣ ∣ λ − 1 = 0 λ − 2 = 0 ⇒ ∣ ∣ λ 1 = 1 λ 2 = 2 λ 3 = 4
Now we will find the eigen vectors corresponding to each eigen value
1. For λ 1 = 1 \lambda_1 = 1 λ 1 = 1
( A − λ 1 α = 0 1 1 1 2 2 2 − 2 1 1 ) ∣ α 1 α 2 α 3 ∣ = 0 \left( \begin{array}{ccc}
A - \lambda_1 & \alpha = 0 \\
1 & 1 & 1 \\
2 & 2 & 2 \\
-2 & 1 & 1
\end{array} \right) \left| \begin{array}{l}
\alpha_1 \\
\alpha_2 \\
\alpha_3
\end{array} \right| = 0 ⎝ ⎛ A − λ 1 1 2 − 2 α = 0 1 2 1 1 2 1 ⎠ ⎞ ∣ ∣ α 1 α 2 α 3 ∣ ∣ = 0
Having the system of three equations
{ α 1 + α 2 + α 3 = 0 2 α 1 + 2 α 2 + 2 α 3 = 0 − 2 α 1 + α 2 + α 3 = 0 \left\{ \begin{array}{l}
\alpha_1 + \alpha_2 + \alpha_3 = 0 \\
2\alpha_1 + 2\alpha_2 + 2\alpha_3 = 0 \\
-2\alpha_1 + \alpha_2 + \alpha_3 = 0
\end{array} \right. ⎩ ⎨ ⎧ α 1 + α 2 + α 3 = 0 2 α 1 + 2 α 2 + 2 α 3 = 0 − 2 α 1 + α 2 + α 3 = 0
Solve the system by the Gauss method
( 1 1 1 2 2 2 − 2 1 1 ) ∼ ( 1 1 1 1 1 1 − 2 1 1 ) ∼ ( 1 1 1 − 2 1 1 0 0 0 ) ∼ ( 1 1 1 0 1 1 0 0 0 ) ∼ ( 1 1 1 0 0 0 ) \left( \begin{array}{ccc}
1 & 1 & 1 \\
2 & 2 & 2 \\
-2 & 1 & 1
\end{array} \right)
\sim
\left( \begin{array}{ccc}
1 & 1 & 1 \\
1 & 1 & 1 \\
-2 & 1 & 1
\end{array} \right)
\sim
\left( \begin{array}{ccc}
1 & 1 & 1 \\
-2 & 1 & 1 \\
0 & 0 & 0
\end{array} \right)
\sim
\left( \begin{array}{ccc}
1 & 1 & 1 \\
0 & 1 & 1 \\
0 & 0 & 0
\end{array} \right)
\sim
\left( \begin{array}{ccc}
1 & 1 & 1 \\
0 & 0 & 0
\end{array} \right) ⎝ ⎛ 1 2 − 2 1 2 1 1 2 1 ⎠ ⎞ ∼ ⎝ ⎛ 1 1 − 2 1 1 1 1 1 1 ⎠ ⎞ ∼ ⎝ ⎛ 1 − 2 0 1 1 0 1 1 0 ⎠ ⎞ ∼ ⎝ ⎛ 1 0 0 1 1 0 1 1 0 ⎠ ⎞ ∼ ( 1 0 1 0 1 0 )
Having the next equations
{ α 1 + α 2 + α 3 = 0 α 2 + α 3 = 0 \left\{ \begin{array}{l}
\alpha_1 + \alpha_2 + \alpha_3 = 0 \\
\alpha_2 + \alpha_3 = 0
\end{array} \right. { α 1 + α 2 + α 3 = 0 α 2 + α 3 = 0 { α 1 + α 2 = − α 3 α 2 = − α 3 \left\{ \begin{array}{l}
\alpha_1 + \alpha_2 = -\alpha_3 \\
\alpha_2 = -\alpha_3
\end{array} \right. { α 1 + α 2 = − α 3 α 2 = − α 3
Let α 3 = t \alpha_3 = t α 3 = t , then α 2 = − t \alpha_2 = -t α 2 = − t and α 1 = 0 \alpha_1 = 0 α 1 = 0 . That means that our eigen vector has the following form:
α = ( 0 − t t ) or α = ( 0 − 1 1 ) \alpha = \left( \begin{array}{c}
0 \\
-t \\
t
\end{array} \right) \text{ or } \alpha = \left( \begin{array}{c}
0 \\
-1 \\
1
\end{array} \right) α = ⎝ ⎛ 0 − t t ⎠ ⎞ or α = ⎝ ⎛ 0 − 1 1 ⎠ ⎞
2. For λ 2 = 2 \lambda_2 = 2 λ 2 = 2
Similar to the previous
[ 0 1 1 2 1 2 − 2 1 0 ] [ β 1 β 2 β 3 ] = 0 \left[ \begin{array}{ccc}
0 & 1 & 1 \\
2 & 1 & 2 \\
-2 & 1 & 0
\end{array} \right]
\left[ \begin{array}{c}
\beta_1 \\
\beta_2 \\
\beta_3
\end{array} \right] = 0 ⎣ ⎡ 0 2 − 2 1 1 1 1 2 0 ⎦ ⎤ ⎣ ⎡ β 1 β 2 β 3 ⎦ ⎤ = 0 ( 0 1 1 0 2 1 2 0 − 2 1 0 0 ) ∼ ( 0 1 1 0 2 1 2 0 0 2 2 0 ) ∼ ( 2 1 2 0 0 1 1 0 0 0 0 0 ) ∼ ( 1 1 / 2 1 0 0 1 1 0 0 0 0 0 ) { β 1 + 1 2 β 2 + β 3 = 0 β 2 + β 3 = 0 { β 1 + 1 2 β 2 = − β 3 β 2 = − β 3 \begin{array}{l}
\left( \begin{array}{cccc}
0 & 1 & 1 & 0 \\
2 & 1 & 2 & 0 \\
-2 & 1 & 0 & 0
\end{array} \right)
\sim
\left( \begin{array}{cccc}
0 & 1 & 1 & 0 \\
2 & 1 & 2 & 0 \\
0 & 2 & 2 & 0
\end{array} \right)
\sim
\left( \begin{array}{cccc}
2 & 1 & 2 & 0 \\
0 & 1 & 1 & 0 \\
0 & 0 & 0 & 0
\end{array} \right)
\sim
\left( \begin{array}{cccc}
1 & 1/2 & 1 & 0 \\
0 & 1 & 1 & 0 \\
0 & 0 & 0 & 0
\end{array} \right) \\
\left\{
\begin{array}{l}
\beta_1 + \frac{1}{2} \beta_2 + \beta_3 = 0 \\
\beta_2 + \beta_3 = 0
\end{array}
\right. \\
\left\{
\begin{array}{l}
\beta_1 + \frac{1}{2} \beta_2 = -\beta_3 \\
\beta_2 = -\beta_3
\end{array}
\right. \\
\end{array} ⎝ ⎛ 0 2 − 2 1 1 1 1 2 0 0 0 0 ⎠ ⎞ ∼ ⎝ ⎛ 0 2 0 1 1 2 1 2 2 0 0 0 ⎠ ⎞ ∼ ⎝ ⎛ 2 0 0 1 1 0 2 1 0 0 0 0 ⎠ ⎞ ∼ ⎝ ⎛ 1 0 0 1/2 1 0 1 1 0 0 0 0 ⎠ ⎞ { β 1 + 2 1 β 2 + β 3 = 0 β 2 + β 3 = 0 { β 1 + 2 1 β 2 = − β 3 β 2 = − β 3
Let β 3 = t ⇒ β 2 = − t ⇒ β 1 = − 1 2 t ⇒ β = ( − 1 2 t − t t ) \beta_3 = t \Rightarrow \beta_2 = -t \Rightarrow \beta_1 = -\frac{1}{2} t \Rightarrow \beta = \begin{pmatrix} -\frac{1}{2} t \\ -t \\ t \end{pmatrix} β 3 = t ⇒ β 2 = − t ⇒ β 1 = − 2 1 t ⇒ β = ⎝ ⎛ − 2 1 t − t t ⎠ ⎞ or β = ( 1 2 − 2 ) \beta = \begin{pmatrix} 1 \\ 2 \\ -2 \end{pmatrix} β = ⎝ ⎛ 1 2 − 2 ⎠ ⎞
3. For λ 3 = 4 \lambda_3 = 4 λ 3 = 4
Similar to the previous
[ − 2 1 1 2 − 1 2 − 2 1 − 2 ] ∗ [ γ 1 γ 2 γ 3 ] = 0 ( − 2 1 1 0 2 − 1 2 0 − 2 1 − 2 0 ) ∼ ( 0 0 3 0 2 − 1 2 0 0 0 0 0 ) ∼ ( 1 − 1 2 1 0 0 0 1 0 0 0 0 0 ) { γ 1 − 1 2 γ 2 + γ 3 = 0 γ 3 = 0 { γ 1 = 1 2 γ 2 γ 3 = 0 \begin{array}{l}
\left[ \begin{array}{ccc}
-2 & 1 & 1 \\
2 & -1 & 2 \\
-2 & 1 & -2
\end{array} \right]
* \left[ \begin{array}{c}
\gamma_1 \\
\gamma_2 \\
\gamma_3
\end{array} \right] = 0 \\
\left( \begin{array}{cccc}
-2 & 1 & 1 & 0 \\
2 & -1 & 2 & 0 \\
-2 & 1 & -2 & 0
\end{array} \right)
\sim
\left( \begin{array}{cccc}
0 & 0 & 3 & 0 \\
2 & -1 & 2 & 0 \\
0 & 0 & 0 & 0
\end{array} \right)
\sim
\left( \begin{array}{cccc}
1 & -\frac{1}{2} & 1 & 0 \\
0 & 0 & 1 & 0 \\
0 & 0 & 0 & 0
\end{array} \right) \\
\left\{
\begin{array}{l}
\gamma_1 - \frac{1}{2} \gamma_2 + \gamma_3 = 0 \\
\gamma_3 = 0
\end{array}
\right. \\
\left\{
\begin{array}{l}
\gamma_1 = \frac{1}{2} \gamma_2 \\
\gamma_3 = 0
\end{array}
\right. \\
\end{array} ⎣ ⎡ − 2 2 − 2 1 − 1 1 1 2 − 2 ⎦ ⎤ ∗ ⎣ ⎡ γ 1 γ 2 γ 3 ⎦ ⎤ = 0 ⎝ ⎛ − 2 2 − 2 1 − 1 1 1 2 − 2 0 0 0 ⎠ ⎞ ∼ ⎝ ⎛ 0 2 0 0 − 1 0 3 2 0 0 0 0 ⎠ ⎞ ∼ ⎝ ⎛ 1 0 0 − 2 1 0 0 1 1 0 0 0 0 ⎠ ⎞ { γ 1 − 2 1 γ 2 + γ 3 = 0 γ 3 = 0 { γ 1 = 2 1 γ 2 γ 3 = 0
Let γ 2 = t ⇒ γ 1 = 1 2 t ⇒ γ = ( 1 2 t t 0 ) \gamma_2 = t \Rightarrow \gamma_1 = \frac{1}{2} t \Rightarrow \gamma = \begin{pmatrix} \frac{1}{2} t \\ t \\ 0 \end{pmatrix} γ 2 = t ⇒ γ 1 = 2 1 t ⇒ γ = ⎝ ⎛ 2 1 t t 0 ⎠ ⎞ or γ = ( 1 2 0 ) \gamma = \begin{pmatrix} 1 \\ 2 \\ 0 \end{pmatrix} γ = ⎝ ⎛ 1 2 0 ⎠ ⎞
Answer:
1) λ 1 = 1 \lambda_1 = 1 λ 1 = 1 ; α = ( 0 − 1 1 ) \alpha = \begin{pmatrix} 0 \\ -1 \\ 1 \end{pmatrix} α = ⎝ ⎛ 0 − 1 1 ⎠ ⎞
2) λ 2 = 2 \lambda_2 = 2 λ 2 = 2 ; β = ( 1 2 − 2 ) \beta = \begin{pmatrix} 1 \\ 2 \\ -2 \end{pmatrix} β = ⎝ ⎛ 1 2 − 2 ⎠ ⎞
3) λ 3 = 4 \lambda_3 = 4 λ 3 = 4 ; γ = ( 1 2 0 ) \gamma = \begin{pmatrix} 1 \\ 2 \\ 0 \end{pmatrix} γ = ⎝ ⎛ 1 2 0 ⎠ ⎞
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