2.2 - Eigenvectors in three dimensions
A three-by-three matrix has a characteristic cubic, but its eigenvectors still come from linear equations. You will use determinant structure, find vectors for real distinct eigenvalues, and prove consequences of the defining equation for powers and inverses.
The characteristic cubic
Can a changed matrix keep the same eigenvalues? Compare
Only the bottom-left entry changes. An expansion down the third column of never uses that entry, so the characteristic equations will agree. The eigenvectors need not agree.
For three dimensions, is cubic. Equivalently, use , which changes the determinant's sign but not its zeros. The latter produces a monic cubic; below we state the final equation in that form.
Worked example 1: exploiting a sparse column
Question. Find the characteristic equation and eigenvalues of .
Plan. Expand down column 3, then factor the remaining quadratic.
Equating this to zero and multiplying the equation by gives a monic form.
Answer. The characteristic equation is
The eigenvalues are .
Check. The roots add to the diagonal sum , while their product is . Their pair products are , checking the expanded cubic.
Change only the bottom-left entry to . This shows why a nontriangular matrix can still have an efficient determinant expansion.
Worked example 2: a coupling that leaves the roots unchanged
Question. Find the characteristic equation and eigenvalues of .
Plan. Expand down the same column; its two zeros still remove two terms.
The bottom-left entry is outside this minor.
Answer. The characteristic equation is again , with eigenvalues .
Check. Independently expand along row 1:
This has exactly the stated roots.
For a triangular matrix the characteristic determinant is the product of its diagonal factors. For a general matrix, inspect sparse rows and columns first. If a cubic does not factor immediately, test plausible rational roots, divide by the factor found, and solve the remaining quadratic.
Watch out
In three dimensions, has leading term . Multiplying the whole characteristic equation by is valid; changing only some signs is not.
Use the same sparse-column strategy with different numbers.
Real distinct eigenvalues
Once a root is known, a three-dimensional eigenvector comes from , just as in two dimensions. Use all three equations: the first two alone may leave a coordinate unchecked.
The eigenvalue calculations here concern real distinct eigenvalues. For a three-by-three matrix this gives three independent eigendirections. Choose convenient integer components, avoiding the zero vector. Repeated eigenvalues and non-real eigendirections require further theory outside this sequence.
Worked example 3: using the third coordinate equation
Question. Find eigenvectors of for .
Plan. Solve the three homogeneous equations for each eigenvalue, clearing fractions where useful.
For , the equations reduce to and . Take , giving , .
For , they reduce to and . Take , giving , .
For , and force ; is free and must be nonzero.
Answer. Corresponding eigenvectors are
Every nonzero multiple of each is valid.
Check. Multiplication by the original matrix gives , , and , respectively, verifying all coordinates and pairings.
Change only the bottom-right entry from to . The first two coordinate relations stay the same; the final coordinate changes for the first two directions.
Worked example 4: adapting the eigenvectors
Question. Find eigenvalues and corresponding eigenvectors of .
Plan. Use the characteristic factorisation, then recalculate each third-coordinate relation.
The determinant factors as , so the eigenvalues are .
At , and , giving . At , and , giving . At , the first two equations force , so take .
Answer. The three displayed vectors correspond to , respectively, with arbitrary nonzero scalar multiples allowed.
Check. Their original-matrix images are , , and , the required multiples.
Continue this lesson.
You’re previewing NovaLearn without an account. Create a free account to read the rest.
Create free account