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What are the eigenvalues and eigenvectors of a matrix, and how do we find them?

Find the eigenvalues and eigenvectors of 2x2 and 3x3 matrices using the characteristic equation

A focused answer to the H2 Further Mathematics outcome on eigenvalues and eigenvectors. The eigenvalue equation, the characteristic polynomial, finding eigenvalues from det(A - lambda I) = 0, solving for eigenvectors, and their geometric meaning as invariant directions.

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  1. What this dot point is asking
  2. The answer
  3. Examples in context
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What this dot point is asking

SEAB wants you to find the eigenvalues and eigenvectors of 2×22\times2 and 3×33\times3 matrices. An eigenvalue is a scalar λ\lambda for which the matrix has a non-zero vector that it merely scales; that vector is the eigenvector. You find eigenvalues from the characteristic equation det(AλI)=0\det(\mathbf{A} - \lambda\mathbf{I}) = 0 and then solve a homogeneous system for each eigenvector.

The answer

The eigenvalue equation

A non-zero vector v\mathbf{v} is an eigenvector of A\mathbf{A} with eigenvalue λ\lambda if

Av=λv.\mathbf{A}\mathbf{v} = \lambda\mathbf{v}.

Geometrically, A\mathbf{A} leaves the direction of v\mathbf{v} unchanged (or exactly reversed if λ<0\lambda < 0), stretching it by the factor λ\lambda. Such directions are the invariant directions of the linear map.

The characteristic equation

Rearrange Av=λv\mathbf{A}\mathbf{v} = \lambda\mathbf{v} to (AλI)v=0(\mathbf{A} - \lambda\mathbf{I})\mathbf{v} = \mathbf{0}. For a non-zero v\mathbf{v} to exist, the matrix AλI\mathbf{A} - \lambda\mathbf{I} must be singular, so

det(AλI)=0.\det(\mathbf{A} - \lambda\mathbf{I}) = 0.

This is the characteristic equation, a polynomial in λ\lambda of degree equal to the size of the matrix. Its roots are the eigenvalues.

Finding eigenvectors

For each eigenvalue λ\lambda, substitute back and solve the homogeneous system (AλI)v=0(\mathbf{A} - \lambda\mathbf{I})\mathbf{v} = \mathbf{0}. The system is always singular (by construction), so it has non-trivial solutions forming a line (or plane) of eigenvectors; quote any convenient non-zero representative.

Useful shortcuts

For a triangular matrix the eigenvalues are simply the diagonal entries. Two checks on a full matrix: the sum of the eigenvalues equals the trace (sum of the diagonal), and the product of the eigenvalues equals the determinant. These catch arithmetic slips quickly.

Examples in context

Example 1. Long-run behaviour of a process. In a Markov-type model the eigenvalue λ=1\lambda = 1 and its eigenvector give the steady-state distribution, while eigenvalues with λ<1|\lambda| < 1 govern how fast transient effects decay. Eigenanalysis is how the long-run state is extracted.

Example 2. Principal axes of a transformation. The eigenvectors of a symmetric matrix point along the principal axes along which a stretch is pure (no shear), which is why eigenvectors describe the natural directions of deformation and underlie diagonalisation.

Try this

Q1. Write the equation that defines an eigenvalue and eigenvector of A\mathbf{A}. [1 mark]

  • Cue. Av=λv\mathbf{A}\mathbf{v} = \lambda\mathbf{v} with v0\mathbf{v} \neq \mathbf{0}.

Q2. State the characteristic equation used to find eigenvalues. [1 mark]

  • Cue. det(AλI)=0\det(\mathbf{A} - \lambda\mathbf{I}) = 0.

Q3. The eigenvalues of a 2×22\times2 matrix are 33 and 1-1. State its trace and determinant. [2 marks]

  • Cue. Trace =3+(1)=2= 3 + (-1) = 2; determinant =3×(1)=3= 3 \times (-1) = -3.

Exam-style practice questions

Practice questions written in the style of SEAB exam questions on this dot point, with worked answer explainers. The year tag is the paper they imitate, not the source.

Original6 marksFind the eigenvalues and corresponding eigenvectors of A=(2112)\mathbf{A} = \begin{pmatrix} 2 & 1 \\ 1 & 2 \end{pmatrix}.
Show worked answer →

The characteristic equation is det(AλI)=0\det(\mathbf{A} - \lambda\mathbf{I}) = 0:

det(2λ112λ)=(2λ)21=0.\det\begin{pmatrix} 2 - \lambda & 1 \\ 1 & 2 - \lambda \end{pmatrix} = (2-\lambda)^2 - 1 = 0.

So (2λ)2=1(2-\lambda)^2 = 1, giving 2λ=±12 - \lambda = \pm 1, hence λ=1\lambda = 1 or λ=3\lambda = 3.

For λ=1\lambda = 1: solve (AI)v=0(\mathbf{A} - \mathbf{I})\mathbf{v} = \mathbf{0}, that is (1111)v=0\begin{pmatrix} 1 & 1 \\ 1 & 1 \end{pmatrix}\mathbf{v} = \mathbf{0}, giving v1+v2=0v_1 + v_2 = 0. An eigenvector is (11)\begin{pmatrix} 1 \\ -1 \end{pmatrix}.

For λ=3\lambda = 3: solve (1111)v=0\begin{pmatrix} -1 & 1 \\ 1 & -1 \end{pmatrix}\mathbf{v} = \mathbf{0}, giving v1=v2v_1 = v_2. An eigenvector is (11)\begin{pmatrix} 1 \\ 1 \end{pmatrix}.

Markers reward forming the characteristic equation, solving for both eigenvalues, and a correct (non-zero) eigenvector for each.

Original7 marksFind the eigenvalues of B=(300120211)\mathbf{B} = \begin{pmatrix} 3 & 0 & 0 \\ 1 & 2 & 0 \\ 2 & 1 & 1 \end{pmatrix} and an eigenvector corresponding to the largest eigenvalue.
Show worked answer →

Since B\mathbf{B} is lower triangular, its eigenvalues are the diagonal entries: λ=3,2,1\lambda = 3, 2, 1. (For a triangular matrix det(BλI)\det(\mathbf{B} - \lambda\mathbf{I}) is the product of the diagonal terms (3λ)(2λ)(1λ)(3-\lambda)(2-\lambda)(1-\lambda).)

The largest eigenvalue is λ=3\lambda = 3. Solve (B3I)v=0(\mathbf{B} - 3\mathbf{I})\mathbf{v} = \mathbf{0}:

(000110212)(xyz)=0.\begin{pmatrix} 0 & 0 & 0 \\ 1 & -1 & 0 \\ 2 & 1 & -2 \end{pmatrix}\begin{pmatrix} x \\ y \\ z \end{pmatrix} = \mathbf{0}.

Row 2: xy=0x=yx - y = 0 \Rightarrow x = y. Row 3: 2x+y2z=02x+x2z=0z=32x2x + y - 2z = 0 \Rightarrow 2x + x - 2z = 0 \Rightarrow z = \tfrac{3}{2}x.

Take x=2x = 2: eigenvector (223)\begin{pmatrix} 2 \\ 2 \\ 3 \end{pmatrix}.

Markers reward reading eigenvalues off the diagonal of the triangular matrix, setting up (B3I)v=0(\mathbf{B} - 3\mathbf{I})\mathbf{v} = \mathbf{0}, solving the two independent equations, and a valid eigenvector.

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