Differential Equations and Linear Algebra (4th Edition)

Published by Pearson
ISBN 10: 0-32196-467-5
ISBN 13: 978-0-32196-467-0

Chapter 9 - Systems of Differential Equations - 9.4 Vector Differential Equations: Nondefective Coefficient Matrix - Problems - Page 607: 13

Answer

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Work Step by Step

Given: $\begin{bmatrix} 1 & 1 & -1\\ 1& 1 & 1\\ -1 & 1 & 1 \end{bmatrix}$ A straightforward calculation yields $\det (A-\lambda I)=\begin{vmatrix} 1-\lambda & 1 & -1\\ 1 & 1-\lambda & 1\\ -1 & 1 & 1-\lambda \end{vmatrix}=(2-\lambda)(\lambda+1)(\lambda-2)$ so that A has eigenvalues $\lambda_1=2\\ \lambda_2=2\\ \lambda_3=-1$ Eigenvalue $λ_1 =2$: In this case, the system $(A − \lambda I)v = 0$ is $v_1=v_2-v_3\\ v_3=0\\ v_2=1\\ \rightarrow v_1=1$ The solution is $v = r(1,1,0)$. Therefore, $v_1=e^{2t} \begin{bmatrix} 1\\ 1 \\ 0 \end{bmatrix}$ Eigenvalue $\lambda_2 =2$: In this case, the system $(A − \lambda I)v = 0$ is $v_1=v_2-v_3\\ v_3=1\\ v_2=0\\ \rightarrow v_1=-1$ The solution is $v = r(-1, 0,1)$. Therefore, $v_2=e^{2t} \begin{bmatrix} -1\\ 0\\ 1 \end{bmatrix}$ Eigenvalue $\lambda_3 =-1$: In this case, the system $(A − \lambda I)v = 0$ is $v_1=0\\ v_2=1\\ v_3=-v_2=-1$ The solution is $v = r(0,1,-1)$. Therefore, $v_3=e^{-t} \begin{bmatrix} 0\\ 1\\ -1 \end{bmatrix}$ Hence, the general solution to the given equation is $x(t)=c_1v_1+c_2v_2+c_3v_3=c_1e^{2t}\begin{bmatrix} 1\\ 1\\ 0 \end{bmatrix}+c_2e^{2t}\begin{bmatrix} -1\\ 0\\ 1 \end{bmatrix}+c_3e^{-t}\begin{bmatrix} 0\\ 1\\ -1 \end{bmatrix}=\begin{bmatrix} c_2e^{2t}-c_2e^{2t}\\ c_1e^{2t}+c_3e^{-t}\\ c_2e^{2t}-c_3e^{-t} \end{bmatrix}$
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