Chapter 7: Problem 17
Find all eigenvalues and eigenvectors of the given matrix. $$ \left(\begin{array}{rr}{-2} & {1} \\ {1} & {-2}\end{array}\right) $$
Short Answer
Expert verified
Matrix A:
$$
\left(\begin{array}{rr}{-2} & {1} \\\ {1} & {-2}\end{array}\right)
$$
Answer: The eigenvalues are λ₁ = -1 and λ₂ = -3. The corresponding eigenvectors are:
For λ₁ = -1:
$$
v₁ = \begin{pmatrix} 1 \\ 1 \end{pmatrix}
$$
For λ₂ = -3:
$$
v₂ = \begin{pmatrix} 1 \\ -1 \end{pmatrix}
$$
Step by step solution
01
Calculate the Characteristic Equation
First, we need to find the determinant of the matrix subtracted by a scalar (associate with the eigenvalue) multiplied by the identity matrix.
Given Matrix A:
$$
\left(\begin{array}{rr}{-2} & {1} \\\ {1} & {-2}\end{array}\right)
$$
Let λ be the scalar (representing the eigenvalue), subtract λ times the identity matrix (I) from A:
$$
A - λI = \left(\begin{array}{rr}{-2-λ} & {1} \\\ {1} & {-2-λ}\end{array}\right)
$$
Now, find the determinant of (A - λI) and equate it to 0 to get the characteristic equation:
$$
|A - λI| = \begin{vmatrix} {-2-λ} & {1} \\\ {1} & {-2-λ} \end{vmatrix} = (-2-λ)(-2-λ) - (1)(1) = 0
$$
02
Solve the Characteristic Equation
Now, we need to solve the quadratic equation derived from the determinant in the previous step to find the eigenvalues:
$$
λ^2 + 4λ + 3 =λ^2 + 3λ + λ + 3 = (λ+1)(λ+3) = 0
$$
The solutions for λ are:
$$
λ_1 = -1 \\
λ_2 = -3
$$
We have found the eigenvalues as -1 and -3.
03
Find the Eigenvectors
Now, for each eigenvalue, we will find the corresponding eigenvectors by solving the linear system:
For λ = -1, substitute λ in the matrix (A - λI):
$$
\left(\begin{array}{rr}{-1} & {1} \\\ {1} & {-1}\end{array}\right) \begin{pmatrix} x_1 \\ x_2 \end{pmatrix} = 0
$$
Notice that the first and second rows are linearly dependent. That means, we only need to solve one of them:
$
- x_1+ x_2 = 0
$
Let \(x_2\) = t, then \(x_1 = \)t. So, we have the eigenvector for λ = -1 as:
$$
v_1 = \begin{pmatrix} 1 \\ 1 \end{pmatrix}
$$
For λ = -3, substitute λ in the matrix A - λI:
$$
\left(\begin{array}{rr}{1} & {1} \\\ {1} & {1}\end{array}\right) \begin{pmatrix} x_1 \\ x_2 \end{pmatrix} = 0
$$
Again, the first and second rows are linearly dependent. Thus, we only need to solve one of them:
$
x_1 + x_2 = 0
$
Let \(x_1\) = t, then \(x_2 = -t\). So, we have the eigenvector for λ = -3 as:
$$
v_2 = \begin{pmatrix} 1 \\ -1 \end{pmatrix}
$$
Now, we have found all the eigenvalues and their corresponding eigenvectors:
Eigenvalue λ₁ = -1:
Eigenvector: $$v₁ = \begin{pmatrix} 1 \\ 1 \end{pmatrix}$$
Eigenvalue λ₂ = -3:
Eigenvector: $$v₂ = \begin{pmatrix} 1 \\ -1 \end{pmatrix}$$
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Key Concepts
These are the key concepts you need to understand to accurately answer the question.
Characteristic Equation
In the realm of linear algebra, the characteristic equation is a crucial concept when dealing with eigenvalues. To determine the eigenvalues of a matrix, we begin by formulating this equation. The key idea is that the characteristic equation emerges from the determinant of a modified version of the original matrix.
The modified matrix is created by subtracting \( \lambda I \), where \( \lambda \) represents the eigenvalue and \( I \) is the identity matrix. This adjustment yields the matrix \( A - \lambda I \).
Once this modified matrix is established, its determinant can be calculated.
In our specific exercise, the characteristic equation derived was\( (\lambda + 1)(\lambda + 3) = 0 \), leading to the eigenvalues \( \lambda_1 = -1 \) and \( \lambda_2 = -3 \). These values are critical because they pave the way for identifying the corresponding eigenvectors.
The modified matrix is created by subtracting \( \lambda I \), where \( \lambda \) represents the eigenvalue and \( I \) is the identity matrix. This adjustment yields the matrix \( A - \lambda I \).
Once this modified matrix is established, its determinant can be calculated.
- The determinant of \( A - \lambda I \) provides us with a polynomial expression in terms of \( \lambda \).
- Setting this polynomial's determinant equal to zero gives us the characteristic equation.
In our specific exercise, the characteristic equation derived was\( (\lambda + 1)(\lambda + 3) = 0 \), leading to the eigenvalues \( \lambda_1 = -1 \) and \( \lambda_2 = -3 \). These values are critical because they pave the way for identifying the corresponding eigenvectors.
Determinant Calculation
Calculating the determinant is a fundamental step in finding the characteristic equation.
Determinants provide a scalar value that indicates various properties of matrices, such as whether they are invertible or not.
When we perform determinant calculation on \( A - \lambda I \), it involves a simple algebraic process for a 2x2 matrix:
Determinants provide a scalar value that indicates various properties of matrices, such as whether they are invertible or not.
When we perform determinant calculation on \( A - \lambda I \), it involves a simple algebraic process for a 2x2 matrix:
- Take the product of the main diagonal elements (\( a_{11} \cdot a_{22} \)).
- Subtract the product of the off-diagonal elements (\( a_{12} \cdot a_{21} \)).
Linear Systems
Linear systems are closely tied to finding eigenvectors once eigenvalues are known.
By substituting each eigenvalue back into the equation\( (A - \lambda I)\mathbf{x} = 0 \), we aim to solve for the eigenvector, \( \mathbf{x} \).
This procedure reveals the vector combinations that remain invariant (aside from scaling) under the transformation represented by the matrix.
Similarly, for \( \lambda = -3 \), solving provided the eigenvector\( \mathbf{v_2} = \begin{pmatrix} 1 \ -1 \end{pmatrix} \).
Understanding linear systems allows one to fully appreciate how both simplicity and interdependencies in matrix rows determine the nature of eigenvectors.
By substituting each eigenvalue back into the equation\( (A - \lambda I)\mathbf{x} = 0 \), we aim to solve for the eigenvector, \( \mathbf{x} \).
This procedure reveals the vector combinations that remain invariant (aside from scaling) under the transformation represented by the matrix.
- The matrix \( A - \lambda I \) will have rows that are linearly dependent.
- This allows the system to have a non-trivial solution, where solutions can be expressed in terms of a free variable, often denoted as \( t \).
Similarly, for \( \lambda = -3 \), solving provided the eigenvector\( \mathbf{v_2} = \begin{pmatrix} 1 \ -1 \end{pmatrix} \).
Understanding linear systems allows one to fully appreciate how both simplicity and interdependencies in matrix rows determine the nature of eigenvectors.