August 14, 2025
Complete the following warm-up problems to re-familiarize yourself with concepts we’ll be leveraging today.
Example: Consider the matrix \(A = \begin{bmatrix} 7 & 6\\ 6 & -2\end{bmatrix}\). Evaluate the following matrix-vector products.
Look closely at the matrix-vector products and determine if there is anything particularly interesting about two of them.
Multiplying an \(n\times 1\) vector \(\vec{x}\) by an \(m\times n\) matrix transforms the vector from \(\mathbb{R}^n\) to \(\mathbb{R}^m\)
Goals for Today: After today’s discussion, you should be able to
We’ll motivate why we might care about eigenvectors and eigenvalues even before defining them! We’ll use an example to do it.
Example: Consider the matrix \(A = \begin{bmatrix} 7 & 6\\ 6 & -2\end{bmatrix}\) and the vectors \(\vec{v_1} = \begin{bmatrix} 2\\ 1\end{bmatrix}\) and \(\vec{v_2} = \begin{bmatrix} -1\\ 2\end{bmatrix}\) from the warm-up problems.
We’ll motivate why we might care about eigenvectors and eigenvalues even before defining them! We’ll use an example to do it.
Example: Consider the matrix \(A = \begin{bmatrix} 7 & 6\\ 6 & -2\end{bmatrix}\) and the vectors \(\vec{v_1} = \begin{bmatrix} 2\\ 1\end{bmatrix}\) and \(\vec{v_2} = \begin{bmatrix} -1\\ 2\end{bmatrix}\) from the warm-up problems.
Definition (Eigenvector and Eigenvalue): An eigenvector of an \(n\times n\) matrix \(A\) is a non-zero vector \(\vec{x}\in\mathbb{R}^n\) such that \(A\vec{x} = \lambda\vec{x}\) for some scalar \(\lambda\).
Geometrical Note: An eigenvector of the matrix \(A\) is a vector \(\vec{x}\) whose transformed position after left-multiplication by the matrix \(A\) is just a scaling of the vector from its original position.
Strategy: Given a matrix \(A\) and a non-zero vector \(\vec{v}\), the vector is an eigenvector of \(A\) if \(A\vec{x} = \lambda\vec{x}\). That is, the matrix multiplication simply scales the original vector.
Example: Determine whether either of the vectors \(\vec{v} = \begin{bmatrix} 1\\ 0\\ 1\end{bmatrix}\) or \(\vec{u} = \begin{bmatrix} 1\\ 2\\ 3\end{bmatrix}\) is an eigenvector of the matrix \(A = \begin{bmatrix} 4 & 1 & 0\\ 0 & 2 & 0\\ 1 & 0 & 3\end{bmatrix}\). If either is an eigenvector, identify its corresponding eigenvalue.
Solution Path. To answer this, do out the multiplication \(A\vec{v}\) and \(A\vec{u}\). Notice that \(A\vec{v} = 4\vec{v}\), but \(A\vec{u}\) is not simply a scaled copy of \(\vec{u}\). The eigenvalue corresponding to the eigenvector \(\vec{v}\) is \(\lambda = 4\).
This will be the focus of our next discussion, but for now, a preview…
Strategy (Finding Eigenvectors and Eigenvalues): Recall that a scalar \(\lambda\) is an eigenvalue of the matrix \(A\) if there exists a non-trivial (not \(\vec{0}\)) solution to the matrix equation \(A\vec{x} = \lambda \vec{x}\).
Intuition: We haven’t solved equations with unknowns on both sides of an equal sign this semester, so we’ll begin by rewriting the equation
\[\begin{align*} A\vec{x} &= \lambda\vec{x} \end{align*}\]
This will be the focus of our next discussion, but for now, a preview…
Strategy (Finding Eigenvectors and Eigenvalues): Recall that a scalar \(\lambda\) is an eigenvalue of the matrix \(A\) if there exists a non-trivial (not \(\vec{0}\)) solution to the matrix equation \(A\vec{x} = \lambda \vec{x}\).
Intuition: We haven’t solved equations with unknowns on both sides of an equal sign this semester, so we’ll begin by rewriting the equation
\[\begin{align*} A\vec{x} &= \lambda\vec{x}\\ \implies A\vec{x} - \lambda\vec{x} &= \vec{0} \end{align*}\]
This will be the focus of our next discussion, but for now, a preview…
Strategy (Finding Eigenvectors and Eigenvalues): Recall that a scalar \(\lambda\) is an eigenvalue of the matrix \(A\) if there exists a non-trivial (not \(\vec{0}\)) solution to the matrix equation \(A\vec{x} = \lambda \vec{x}\).
Intuition: We haven’t solved equations with unknowns on both sides of an equal sign this semester, so we’ll begin by rewriting the equation
\[\begin{align*} A\vec{x} &= \lambda\vec{x}\\ \implies A\vec{x} - \lambda\vec{x} &= \vec{0}\\ \implies \left(A - \lambda I\right)\vec{x} &= \vec{0} \end{align*}\]
The bottom equation will have a unique solution if \(\left(A - \lambda I\right)\) is invertible.
We’ll have non-trivial solutions if \(\left(A - \lambda I\right)\) is not invertible.
Strategy (Finding Eigenvectors and Eigenvalues): Recall that a scalar \(\lambda\) is an eigenvalue of the matrix \(A\) if there exists a non-trivial (not \(\vec{0}\)) solution to the matrix equation \(A\vec{x} = \lambda \vec{x}\).
Note: The following items follow directly from what we just saw and are worth noting regarding eigenvalues.
Example: Determine whether \(\lambda = 5\) is an eigenvalue for the matrix \(A = \left[\begin{array}{rr} 6 & 8\\ 1 & 13\end{array}\right]\). If it is an eigenvalue, find an eigenvector corresponding to \(\lambda = 5\).
We’ll start by solving the matrix equation \(\left(A - 5I\right)\vec{x} = \vec{0}\).
As usual, we’ll do this by constructing a corresponding augmented matrix and row-reducing.
There is a free variable here, so \(\lambda = 5\) is indeed a eigenvalue for this matrix.
Example: Determine whether \(\lambda = 5\) is an eigenvalue for the matrix \(A = \left[\begin{array}{rr} 6 & 8\\ 1 & 13\end{array}\right]\). If it is an eigenvalue, find an eigenvector corresponding to \(\lambda = 5\).
We’ll start by solving the matrix equation \(\left(A - 5I\right)\vec{x} = \vec{0}\).
As usual, we’ll do this by constructing a corresponding augmented matrix and row-reducing.
(Matrix([
[1, 8, 0],
[0, 0, 0]]), (0,))
There is a free variable here, so \(\lambda = 5\) is indeed a eigenvalue for this matrix.
We can construct a basis for the eigenspace of this matrix corresponding to \(\lambda = 5\) by writing the solutions to the equation we began from, in parameteric vector form. Note that \(\vec{x} = x_2\left[\begin{array}{r} -8\\ 1\end{array}\right]\). Thus, \(\mathscr{B}_{\lambda = 5} = \left\{\left[\begin{array}{r} -8\\ 1\end{array}\right]\right\}\).
Recall (Triangular Matrix): A matrix \(A\) having all entries either above or below its main diagonal as \(0\)’s is called a triangular matrix. If the \(0\)’s are below the main diagonal, \(A\) is called lower triangular while a matrix having all \(0\)’s above the main diagonal is $upper triangular*.
Theorem (Eigenvalues of Triangular Matrices): The eigenvalues of a triangular matrix are the entries along its main diagonal.
Example: The eigenvalues of the matrix \(A = \begin{bmatrix} 6 & 0 & 0 & 0\\ -2 & 0 & 0 & 0\\ -1 & 3 & 1 & 0\\ 2 & 0 & -7 & 5\end{bmatrix}\) are…
Recall (Triangular Matrix): A matrix \(A\) having all entries either above or below its main diagonal as \(0\)’s is called a triangular matrix. If the \(0\)’s are below the main diagonal, \(A\) is called lower triangular while a matrix having all \(0\)’s above the main diagonal is $upper triangular*.
Theorem (Eigenvalues of Triangular Matrices): The eigenvalues of a triangular matrix are the entries along its main diagonal.
Example: The eigenvalues of the matrix \(A = \begin{bmatrix} 6 & 0 & 0 & 0\\ -2 & 0 & 0 & 0\\ -1 & 3 & 1 & 0\\ 2 & 0 & -7 & 5\end{bmatrix}\) are \(\lambda_1 = 6\), \(\lambda_2 = 0\), \(\lambda_3 = 1\), and \(\lambda_4 = 5\).
Theorem: If \(\vec{v_1}, \vec{v_2}, \cdots, \vec{v_r}\) are eigenvectors that correspond to distinct eigenvalues \(\lambda_1, \lambda_2, \cdots, \lambda_r\) of an \(n\times n\) matrix \(A\) then the set \(\left\{\vec{v_1}, \vec{v_2}, \cdots, \vec{v_r}\right\}\) are linearly independent.
\[T\left(c_1\vec{v_1} + c_2\vec{v_2} + \cdots + c_n\vec{v_n}\right) = c_1T\left(\vec{v_1}\right) + c_2T\left(\vec{v_2}\right) + \cdots + c_nT\left(\vec{v_n}\right)\]
This is particularly useful when \(\left\{\vec{v_1}, \vec{v_2}, \cdots, \vec{v_n}\right\}\) form a basis for \(\mathbb{R}^n\).
Even better, if we had a basis consisting of eigenvectors (an eigenbasis), then there is no need for matrix multiplication to be carried out at all.
Additionally, eigenvectors and eigenvalues indicate how much (eigenvalues) and in what directions (eigenvectors) a linear transformation stretches space.
We’ve seen that changing bases from the standard basis to an alternative basis (like an eigenbasis) can be helpful.
If one or more of the eigenvectors (axes in the eigenbasis representation of space) have very small eigenvalues, then…
Example 1: Determine whether \(\lambda = 3\) is an eigenvalue for the matrix \(A = \left[\begin{array}{rr} 5 & 6\\ -2 & 4\end{array}\right]\). If it is an eigenvalue, find a corresponding eigenvector.
Example 2: Determine whether the vector \(\left[\begin{array}{r} -5\\ -4\\ 3\end{array}\right]\) is an eigenvector for the matrix \(A = \left[\begin{array}{rrr} 0 & 5 & -10\\ 0 & 22 & 16\\ 0 & -9 & -2\end{array}\right]\). If so, find the corresponding eigenvalue and at least one other eigenvector corresponding to the same eigenvalue.
Example 3: The matrix \(A = \left[\begin{array}{rr} 8 & 2\\ 6 & 12\end{array}\right]\) has eigenvalues \(\lambda = 6\) and \(\lambda = 14\). Find a basis for each of the corresponding eigenspaces.
Example 4: Find the eigenvalues corresponding to the matrix \(A = \left[\begin{array}{rr} 1 & 0 & 0\\ 2 & 2 & 0\\ 1 & 0 & 5\end{array}\right]\).
\[\Huge{\text{Start Homework 11}}\] \[\Huge{\text{on MyOpenMath}}\]
\(\Huge{\text{Finding}}\)
\(\Huge{\text{Eigenvectors and Eigenvalues}}\)