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Eigenvalues and eigenspaces of matrices of order 2

Theory used: Characteristic polynomialEigenvalues as roots of the characteristic polynomialTrace, determinant and eigenvaluesEigenspaceComputing an eigenspaceAlgebraic and geometric multiplicity

Go to: Exercise 1Exercise 2Exercise 3

Exercise 1

Determine the eigenvalues and eigenspaces of the matrix

x y -3-2-1123-2-112 O uwV₃ : x − 2y = 0V₋₁ : x + 2y = 0
y=x2y = \dfrac{x}{2}y=−x2y = \dfrac{-x}{2}
The eigenspaces and are the lines through the origin spanned by and by

The characteristic polynomial is obtained by subtracting from the diagonal entries and computing the determinant of order . The polynomial has roots and , and the check with trace and determinant confirms the result, since and . For each eigenvalue one solves the homogeneous system with matrix : the two rows of this matrix are proportional, because its determinant is zero, therefore the system reduces to a single equation. From the equation one gets , and with one finds the generator ; from the equation one gets the generator . The final check confirms that the two vectors are eigenvectors. Both eigenspaces have dimension .

Exercise 2

Determine the eigenvalues and eigenspaces of the matrix

For a matrix of order the characteristic polynomial can be written directly as , therefore trace and determinant are sufficient. The roots of are and . The matrix has its second row equal to the first multiplied by , so the system reduces to the equation , that is, , and the generator with is . In the same way the matrix gives the equation , satisfied by . The checks show that and , therefore and .

Exercise 3

Determine the eigenvalues, the eigenspaces, and the algebraic and geometric multiplicities of the eigenvalues of the matrix

The characteristic polynomial is a perfect square, therefore the matrix has the single eigenvalue , a double root: . The geometric multiplicity is the dimension of the eigenspace, that is, . The matrix is not zero and has opposite rows, so its rank is and . The eigenspace is the line , spanned by ; indeed . In this case , therefore the eigenvectors of all lie on a single line and there is no basis of made of eigenvectors of .

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