Math Problem Statement

Given a system of differential equations with a matrix A, find the general solution, identify the correct direction field, and describe the behavior of the solution as time approaches infinity.

Solution

Let's break down and solve each part of the problem provided.

Part (a): Finding the General Solution

Given the system of differential equations: x=(3222)x\mathbf{x}' = \begin{pmatrix} 3 & -2 \\ 2 & -2 \end{pmatrix} \mathbf{x} we are tasked to find the general solution for x(t)\mathbf{x}(t).

  1. Find the eigenvalues of the matrix: A=(3222)A = \begin{pmatrix} 3 & -2 \\ 2 & -2 \end{pmatrix} The characteristic polynomial is given by det(AλI)=0\det(A - \lambda I) = 0: det(3λ222λ)=(3λ)(2λ)(2)(2)=0\det \begin{pmatrix} 3 - \lambda & -2 \\ 2 & -2 - \lambda \end{pmatrix} = (3 - \lambda)(-2 - \lambda) - (-2)(2) = 0 Simplifying, we get the characteristic polynomial: λ2λ6=0\lambda^2 - \lambda - 6 = 0 Solving for λ\lambda, we get the eigenvalues λ1=2\lambda_1 = 2 and λ2=1\lambda_2 = -1.

  2. Find eigenvectors for each eigenvalue:

    • For λ1=2\lambda_1 = 2: (A2I)v=0(1224)v=0(A - 2I)\mathbf{v} = 0 \Rightarrow \begin{pmatrix} 1 & -2 \\ 2 & -4 \end{pmatrix} \mathbf{v} = 0 This yields the eigenvector v1=(21)\mathbf{v}_1 = \begin{pmatrix} 2 \\ 1 \end{pmatrix}.

    • For λ2=1\lambda_2 = -1: (A+I)v=0(4221)v=0(A + I)\mathbf{v} = 0 \Rightarrow \begin{pmatrix} 4 & -2 \\ 2 & -1 \end{pmatrix} \mathbf{v} = 0 This yields the eigenvector v2=(12)\mathbf{v}_2 = \begin{pmatrix} 1 \\ 2 \end{pmatrix}.

  3. Construct the general solution: Using the eigenvalues and eigenvectors, the solution can be written as: x(t)=c1(21)e2t+c2(12)et\mathbf{x}(t) = c_1 \begin{pmatrix} 2 \\ 1 \end{pmatrix} e^{2t} + c_2 \begin{pmatrix} 1 \\ 2 \end{pmatrix} e^{-t} This matches the form provided in the problem.

Part (b): Direction Field

The direction field given (Field 5) is chosen to represent the flow of solutions to this system. The positive eigenvalue λ=2\lambda = 2 suggests exponential growth in one direction, while the negative eigenvalue λ=1\lambda = -1 indicates exponential decay in the orthogonal direction. The field confirms this behavior, showing trajectories moving away from the origin along one direction and spiraling due to the interaction between the eigenvalues.

Part (c): Behavior as tt \to \infty

With c1,c20c_1, c_2 \neq 0, the dominant term as tt \to \infty will be the one with the positive exponent e2te^{2t}. Therefore, the solution will grow unbounded in the direction associated with v1=(21)\mathbf{v}_1 = \begin{pmatrix} 2 \\ 1 \end{pmatrix}, meaning the solution will tend towards infinity as tt \to \infty.

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Follow-up Questions:

  1. How are eigenvalues used to determine the stability of solutions in a differential system?
  2. What impact does each eigenvalue's sign have on the behavior of solutions over time?
  3. How can direction fields help visualize solutions to differential systems?
  4. Why is the direction associated with the positive eigenvalue dominant as tt \to \infty?
  5. Can you describe the behavior of the solution if both eigenvalues were negative?

Tip:

For systems with real eigenvalues, the general behavior of solutions can be quickly understood by observing the sign of the eigenvalues: positive eigenvalues indicate instability (growth), while negative eigenvalues indicate stability (decay).

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Math Problem Analysis

Mathematical Concepts

Linear Algebra
Differential Equations
Eigenvalues and Eigenvectors
System Stability
Direction Fields

Formulas

Characteristic polynomial: det(A - λI) = 0
General solution form: x(t) = c1 * v1 * e^(λ1 * t) + c2 * v2 * e^(λ2 * t)

Theorems

Eigenvalue stability criterion
Solution behavior of linear systems based on eigenvalues

Suitable Grade Level

Undergraduate - Differential Equations Course