Differential Equations and Linear Algebra (4th Edition)

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

Chapter 7 - Eigenvalues and Eigenvectors - 7.3 Diagonalization - Problems - Page 460: 24

Answer

$x_1(t)=-C_1e^{-t}+C_3e^{2t}\\ x_2(t)=C_1e^{-t}+C_2e^{2t} \\ x_3(t)=-C_1e^{-t}+(C_2-C_3)e^{2t}$

Work Step by Step

The given system can be written as $x′ = Ax$, where $A=\begin{bmatrix} 1 & 1 & -1\\ 1 & 1 & 1\\ -1 & 1 & 1 \end{bmatrix}$ The transformed system is $y′ = (S−1AS)y$ where $x = Sy$ To determine S, we need the eigenvalues and eigenvectors of A. The characteristic polynomial of A is $p(\lambda)=\begin{bmatrix} 1-\lambda & 1 & -1\\ 1 & 1-\lambda & 1\\ -1 & 1 & 1-\lambda \end{bmatrix}=-\lambda^3+3\lambda^2-4$ Hence, A is nondefective by Corollary 7.2.10. The eigenvectors are easily computed: \lambda_1=-1: v=r(-1,1,-1)$ \lambda_2=2: v=s(0,1,1)\\ \lambda_3=2: v=t(1,0,-1) \\ $ Set $S = \begin{bmatrix} -1 & 0 & 1\\ 1 & 1 & 0\\ -1 & 1 & -1 \end{bmatrix}$ then from Theorem 7.3.4, $S−1AS = diag(-1,2,2)$ so that the system becomes: $\begin{bmatrix} y_1'\\ y_2' \\ y_3' \end{bmatrix}=\begin{bmatrix} -1 & 0 & 0\\ 0 & 2 & 0\\ 0 & 0 & 2 \end{bmatrix}\begin{bmatrix} y_1\\ y_2 \\ y_3 \end{bmatrix}$ Hence, $y_1'=-y_1\\ y_2'=2y_2 \\ y_3'=2y_3$ Both of these equations can be integrated to obtain $y_1(t)=C_1e^{-t}\\ y_2(t)=C_2e^{2t}\\ y_3(t)=C_3e^{2t}$ Return to the original variables, we have: $x=Sy=\begin{bmatrix} -1 & & 1\\ 1 & 1 & 0\\ -1 & 1 & 1 \end{bmatrix}\begin{bmatrix} C_1e^{-t}\\ C_2e^{2t}\\ C_3e^{2t} \end{bmatrix} \\ \rightarrow x_1(t)=-C_1e^{-t}+C_3e^{2t}\\ x_2(t)=C_1e^{-t}+C_2e^{2t} \\ x_3(t)=-C_1e^{-t}+(C_2-C_3)e^{2t}$
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