Problem 23
Question
Solve the given initial-value problem. $$ \left[\begin{array}{c} \frac{d x_{1}}{d t} \\ \frac{d x_{2}}{d t} \end{array}\right]=\left[\begin{array}{cc} 4 & -7 \\ 2 & -5 \end{array}\right]\left[\begin{array}{l} x_{1}(t) \\ x_{2}(t) \end{array}\right] $$ $$ \text { with } x_{1}(0)=13 \text { and } x_{2}(0)=3 \text { . } $$
Step-by-Step Solution
Verified Answer
The particular solution is \( x_1(t) = 14e^{2t} - e^{-3t} \) and \( x_2(t) = 4e^{2t} - e^{-3t} \).
1Step 1: Write the System of Differential Equations
The given matrix equation can be expanded into a system of linear differential equations: \( \frac{d x_1}{d t} = 4x_1 - 7x_2 \) and \( \frac{d x_2}{d t} = 2x_1 - 5x_2 \).
2Step 2: Find the Eigenvalues of the Coefficient Matrix
The coefficient matrix \( A \) is \( \begin{pmatrix} 4 & -7 \ 2 & -5 \end{pmatrix} \). Find the eigenvalues by solving \( \text{det}(A - \lambda I) = 0 \), where \( I \) is the identity matrix. Compute: \[ \begin{vmatrix} 4-\lambda & -7 \ 2 & -5-\lambda \end{vmatrix} = (4-\lambda)(-5-\lambda) - (-7)(2) \]. This simplifies to \( \lambda^2 + \lambda - 6 = 0 \).
3Step 3: Solve the Characteristic Equation
The characteristic equation \( \lambda^2 + \lambda - 6 = 0 \) can be factored as \( (\lambda - 2)(\lambda + 3) = 0 \). Thus, the eigenvalues are \( \lambda_1 = 2 \) and \( \lambda_2 = -3 \).
4Step 4: Find the Eigenvectors
For \( \lambda_1 = 2 \), solve \( (A - 2I)\mathbf{v_1} = \mathbf{0} \). This yields the augmented matrix: \( \begin{pmatrix} 2 & -7 \ 2 & -7 \end{pmatrix} \rightarrow \mathbf{v_1} = \begin{pmatrix} 7 \ 2 \end{pmatrix} \). For \( \lambda_2 = -3 \), solve \( (A + 3I)\mathbf{v_2} = \mathbf{0} \), giving: \( \begin{pmatrix} 7 & -7 \ 2 & -2 \end{pmatrix} \rightarrow \mathbf{v_2} = \begin{pmatrix} 1 \ 1 \end{pmatrix} \).
5Step 5: Construct the General Solution
The general solution of the system is a linear combination of the eigenvectors with exponential terms: \( \begin{pmatrix} x_1(t) \ x_2(t) \end{pmatrix} = c_1 \begin{pmatrix} 7 \ 2 \end{pmatrix}e^{2t} + c_2 \begin{pmatrix} 1 \ 1 \end{pmatrix}e^{-3t} \).
6Step 6: Apply Initial Conditions
Substitute \( t = 0 \), \( x_1(0) = 13 \), and \( x_2(0) = 3 \) into the general solution to find \( c_1 \) and \( c_2 \). Solve: \[ 7c_1 + c_2 = 13 \] \[ 2c_1 + c_2 = 3 \]. Subtract the second equation from the first to get \( 5c_1 = 10 \), so \( c_1 = 2 \). Substitute \( c_1 = 2 \) back into \( 2c_1 + c_2 = 3 \) to find \( c_2 = -1 \).
7Step 7: Write the Particular Solution
Substitute \( c_1 = 2 \) and \( c_2 = -1 \) into the general solution: \( \begin{pmatrix} x_1(t) \ x_2(t) \end{pmatrix} = 2 \begin{pmatrix} 7 \ 2 \end{pmatrix} e^{2t} - \begin{pmatrix} 1 \ 1 \end{pmatrix} e^{-3t} \).
Key Concepts
Linear Differential EquationsEigenvalues and EigenvectorsMatrix Algebra
Linear Differential Equations
Linear differential equations form a crucial part of calculus and mathematical analysis. They involve derivatives of a function and are called 'linear' because the function and its derivatives appear in a linear form. In an initial-value problem, you not only solve these equations but also find a specific solution that satisfies given starting conditions. For instance, in our problem, we deal with a system of linear differential equations:
- \( \frac{dx_1}{dt} = 4x_1 - 7x_2 \)
- \( \frac{dx_2}{dt} = 2x_1 - 5x_2 \)
Eigenvalues and Eigenvectors
In the context of linear differential equations, eigenvalues and eigenvectors offer powerful tools to simplify the problem. They are related to matrices, particularly when we encounter a system of equations that can be represented in matrix form. Here, the matrix is given by:
Eigenvectors are then found by substituting each eigenvalue back into the matrix equation \( (A - \lambda I)\mathbf{v} = \mathbf{0} \). For \( \lambda_1 = 2 \), the eigenvector is \( \begin{pmatrix} 7 \ 2 \end{pmatrix} \), and for \( \lambda_2 = -3 \), it is \( \begin{pmatrix} 1 \ 1 \end{pmatrix} \).
These eigenvectors form the basis of the solution to the differential equation, as a linear combination of these vectors determines the behavior of the system over time.
- \( A = \begin{pmatrix} 4 & -7 \ 2 & -5 \end{pmatrix} \)
Eigenvectors are then found by substituting each eigenvalue back into the matrix equation \( (A - \lambda I)\mathbf{v} = \mathbf{0} \). For \( \lambda_1 = 2 \), the eigenvector is \( \begin{pmatrix} 7 \ 2 \end{pmatrix} \), and for \( \lambda_2 = -3 \), it is \( \begin{pmatrix} 1 \ 1 \end{pmatrix} \).
These eigenvectors form the basis of the solution to the differential equation, as a linear combination of these vectors determines the behavior of the system over time.
Matrix Algebra
Matrix algebra provides a structured way to handle linear equations, especially when dealing with multiple variables and their relationships. In our exercise, the system of differential equations can be compactly written in matrix form, which allows us to apply matrix operations and concepts like eigenvalues and eigenvectors more efficiently.
The matrix \( A = \begin{pmatrix} 4 & -7 \ 2 & -5 \end{pmatrix} \) captures the coefficients of the variables in the system and directly relates to how the system evolves over time. By representing the system in matrix form, you utilize the power of linear transformations, where the matrix operates on a vector (in this case, the state of the system \( \begin{pmatrix} x_1(t) \ x_2(t) \end{pmatrix} \)) to produce its derivative.
The matrix \( A = \begin{pmatrix} 4 & -7 \ 2 & -5 \end{pmatrix} \) captures the coefficients of the variables in the system and directly relates to how the system evolves over time. By representing the system in matrix form, you utilize the power of linear transformations, where the matrix operates on a vector (in this case, the state of the system \( \begin{pmatrix} x_1(t) \ x_2(t) \end{pmatrix} \)) to produce its derivative.
- This approach streamlines the solving process, helping to leverage linear algebraic methods like finding determinants and eigenvector decomposition to solve the system.
- In practice, it allows for easier computation and clearer insight into the system's behavior, particularly when handling complex systems with many variables.
Other exercises in this chapter
Problem 21
A very simple two-compartment model for gap dynamics in a forest assumes that gaps are created by disturbances (wind, fire, etc.) and that gaps revert to forest
View solution Problem 22
Solve the given initial-value problem. $$ \left[\begin{array}{c} \frac{d x_{1}}{d t} \\ \frac{d x_{2}}{d t} \end{array}\right]=\left[\begin{array}{rr} -1 & 0 \\
View solution Problem 23
Let $$ \begin{array}{l} \frac{d x_{1}}{d t}=x_{1}\left(2-x_{1}\right)-x_{1} x_{2} \\ \frac{d x_{2}}{d t}=x_{1} x_{2}-x_{2} \end{array} $$ (a) Graph the zero iso
View solution Problem 23
23\. Solve $$ \frac{d^{2} x}{d t^{2}}=-4 x $$ with \(x(0)=0\) and \(\frac{d x(0)}{d t}=6\).
View solution