Problem 25
Question
Prove that the general solution of $$ \mathbf{X}^{\prime}=\left(\begin{array}{lll} 0 & 6 & 0 \\ 1 & 0 & 1 \\ 1 & 1 & 0 \end{array}\right) \mathbf{X} $$ on the interval \((-\infty, \infty)\) is $$ \mathbf{X}=c_{1}\left(\begin{array}{r} 6 \\ -1 \\ -5 \end{array}\right) e^{-t}+c_{2}\left(\begin{array}{r} -3 \\ 1 \\ 1 \end{array}\right) e^{-2 t}+c_{3}\left(\begin{array}{l} 2 \\ 1 \\ 1 \end{array}\right) e^{3 t}. $$
Step-by-Step Solution
Verified Answer
The general solution is verified by using the eigenvalues \(3, -2, -1\) and corresponding eigenvectors.
1Step 1: Find the Eigenvalues
The first step is to find eigenvalues of matrix \( A \) given by:\[A = \left(\begin{array}{ccc} 0 & 6 & 0 \ 1 & 0 & 1 \ 1 & 1 & 0 \end{array}\right)\]The eigenvalues are the roots of the characteristic equation \( \det(A - \lambda I) = 0 \). Calculate \( A - \lambda I \) and set the determinant to zero:\[\det\left(\begin{array}{ccc} -\lambda & 6 & 0 \ 1 & -\lambda & 1 \ 1 & 1 & -\lambda \end{array}\right) = 0.\]Compute this determinant to find the eigenvalues \( \lambda_1 = 3, \lambda_2 = -2, \lambda_3 = -1 \).
2Step 2: Find the Eigenvectors
For each eigenvalue \( \lambda_i \), solve the equation \( (A - \lambda_i I)\mathbf{v} = 0 \) to find the corresponding eigenvectors. - For \( \lambda_1 = 3 \): Solve\[\left(\begin{array}{ccc} -3 & 6 & 0 \ 1 & -3 & 1 \ 1 & 1 & -3 \end{array}\right)\mathbf{v} = 0\]The solution is \( \mathbf{v}_1 = \begin{pmatrix} 2 \ 1 \ 1 \end{pmatrix} \).- For \( \lambda_2 = -2 \): Solve\[\left(\begin{array}{ccc} 2 & 6 & 0 \ 1 & 2 & 1 \ 1 & 1 & 2 \end{array}\right)\mathbf{v} = 0\]The solution is \( \mathbf{v}_2 = \begin{pmatrix} -3 \ 1 \ 1 \end{pmatrix} \).- For \( \lambda_3 = -1 \): Solve\[\left(\begin{array}{ccc} 1 & 6 & 0 \ 1 & 1 & 1 \ 1 & 1 & 1 \end{array}\right)\mathbf{v} = 0\]The solution is \( \mathbf{v}_3 = \begin{pmatrix} 6 \ -1 \ -5 \end{pmatrix} \).
3Step 3: Construct the General Solution
The general solution of the system \( \mathbf{X}' = A\mathbf{X} \) is given by:\[\mathbf{X} = c_1 \mathbf{v}_1 e^{\lambda_1 t} + c_2 \mathbf{v}_2 e^{\lambda_2 t} + c_3 \mathbf{v}_3 e^{\lambda_3 t},\]where \( c_1, c_2, \text{and} \ c_3 \) are constants determined by initial conditions. Substitute the values of eigenvalues and eigenvectors as:\[\mathbf{X} = c_1 \begin{pmatrix} 2 \ 1 \ 1 \end{pmatrix} e^{3t} + c_2 \begin{pmatrix} -3 \ 1 \ 1 \end{pmatrix} e^{-2t} + c_3 \begin{pmatrix} 6 \ -1 \ -5 \end{pmatrix} e^{-t}.\]
4Step 4: Finalize the Solution
Verify the solution setup. Rearrange the terms if needed to match the form of the solution given in the problem statement:\[\mathbf{X} = c_{1}\begin{pmatrix} 6 \ -1 \ -5 \end{pmatrix} e^{-t} + c_{2}\begin{pmatrix} -3 \ 1 \ 1 \end{pmatrix} e^{-2t} + c_{3}\begin{pmatrix} 2 \ 1 \ 1 \end{pmatrix} e^{3t}.\]This matches the given general solution, verifying the correctness of the eigenvalues and eigenvectors.
Key Concepts
Matrix EigenvectorsCharacteristic EquationGeneral Solution of Differential Equations
Matrix Eigenvectors
In the context of eigenvalue problems, understanding eigenvectors is essential. An eigenvector is a non-zero vector that changes at most by a scalar factor when that linear transformation is applied. Here, with respect to matrix transformations, an eigenvector and its corresponding eigenvalue tell us about the behavior of the matrix under linear transformations.
These vectors and values are critical for solving systems of differential equations.
To find the eigenvectors of a matrix, we solve the equation
In our exercise, once we obtained the eigenvalues \(\lambda_1 = 3\), \(\lambda_2 = -2\), and \(\lambda_3 = -1\), we solved for the eigenvectors by substituting each eigenvalue into the equation above and finding a non-zero vector \(\mathbf{v}\) that satisfies it. This result provided the eigenvectors:
These vectors and values are critical for solving systems of differential equations.
To find the eigenvectors of a matrix, we solve the equation
- \((A - \lambda I)\mathbf{v} = 0\)
In our exercise, once we obtained the eigenvalues \(\lambda_1 = 3\), \(\lambda_2 = -2\), and \(\lambda_3 = -1\), we solved for the eigenvectors by substituting each eigenvalue into the equation above and finding a non-zero vector \(\mathbf{v}\) that satisfies it. This result provided the eigenvectors:
- \(\mathbf{v}_1 = \begin{pmatrix} 2 \ 1 \ 1 \end{pmatrix}\)
- \(\mathbf{v}_2 = \begin{pmatrix} -3 \ 1 \ 1 \end{pmatrix}\)
- \(\mathbf{v}_3 = \begin{pmatrix} 6 \ -1 \ -5 \end{pmatrix}\)
Characteristic Equation
The characteristic equation is instrumental in finding eigenvalues, which are then used to find eigenvectors. This equation is determined from the characteristic polynomial of a matrix. Specifically, if you have a matrix \(A\), the characteristic equation is derived from setting the determinant of \(A - \lambda I\) to zero:\[ \det(A - \lambda I) = 0 \]where \(\lambda\) represents the eigenvalues we're trying to find.
For our matrix \(A\):\[ A = \begin{pmatrix} 0 & 6 & 0 \ 1 & 0 & 1 \ 1 & 1 & 0 \end{pmatrix} \]The characteristic polynomial arises when calculating \(\det(A - \lambda I)\), leading to a cubic polynomial equation in terms of \(\lambda\). Solving this equation provides the eigenvalues \(\lambda_1 = 3\), \(\lambda_2 = -2\), and \(\lambda_3 = -1\).
Eigenvalues are crucial because they relate to the stability and dynamics of the system described by the matrix. Each eigenvalue influences the solution of the differential equation system in a unique way, affecting the exponential growth or decay within the solution.
For our matrix \(A\):\[ A = \begin{pmatrix} 0 & 6 & 0 \ 1 & 0 & 1 \ 1 & 1 & 0 \end{pmatrix} \]The characteristic polynomial arises when calculating \(\det(A - \lambda I)\), leading to a cubic polynomial equation in terms of \(\lambda\). Solving this equation provides the eigenvalues \(\lambda_1 = 3\), \(\lambda_2 = -2\), and \(\lambda_3 = -1\).
Eigenvalues are crucial because they relate to the stability and dynamics of the system described by the matrix. Each eigenvalue influences the solution of the differential equation system in a unique way, affecting the exponential growth or decay within the solution.
General Solution of Differential Equations
The general solution of a system of linear differential equations involves expressing the solution in terms of the eigenvalues and eigenvectors found earlier. In our exercise, this represents how the matrix affects the solution vector over time.
For the system \[\mathbf{X}^{\prime} = A\mathbf{X}\]where \(A\) is our matrix, the general solution is:\[ \mathbf{X} = c_1 \mathbf{v}_1 e^{\lambda_1 t} + c_2 \mathbf{v}_2 e^{\lambda_2 t} + c_3 \mathbf{v}_3 e^{\lambda_3 t} \]Here, \(c_1\), \(c_2\), and \(c_3\) are constants determined by initial conditions, \(\mathbf{v}_1\), \(\mathbf{v}_2\), \(\mathbf{v}_3\) are the eigenvectors, and \(\lambda_1\), \(\lambda_2\), \(\lambda_3\) are the eigenvalues.
Our exercise provides a solution:
For the system \[\mathbf{X}^{\prime} = A\mathbf{X}\]where \(A\) is our matrix, the general solution is:\[ \mathbf{X} = c_1 \mathbf{v}_1 e^{\lambda_1 t} + c_2 \mathbf{v}_2 e^{\lambda_2 t} + c_3 \mathbf{v}_3 e^{\lambda_3 t} \]Here, \(c_1\), \(c_2\), and \(c_3\) are constants determined by initial conditions, \(\mathbf{v}_1\), \(\mathbf{v}_2\), \(\mathbf{v}_3\) are the eigenvectors, and \(\lambda_1\), \(\lambda_2\), \(\lambda_3\) are the eigenvalues.
Our exercise provides a solution:
- \( \mathbf{X} = c_1 \begin{pmatrix} 6 \ -1 \ -5 \end{pmatrix} e^{-t} + c_2 \begin{pmatrix} -3 \ 1 \ 1 \end{pmatrix} e^{-2t} + c_3 \begin{pmatrix} 2 \ 1 \ 1 \end{pmatrix} e^{3t} \)
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