These quantities can have a geometric meaning and are also useful in matrix algebra, the geometric meaning is discussed on this page, it tells us something about the symmetry of a transform.
An eigenvector is a vector whose direction is not changed by the transform, it may be streached, but it still points in the same direction.
Each eigenvector has a corresponding eigenvalue which gives the scaling factor by which the transform scales the eigenvector. So the eigenvector is a vector and the eigenvalue is a scaler.
A given transform may have more than one eigenvector and eigenvalue pair depending on how many dimensions we are working in. For instance:
- If we are working in 2 dimensions there are upto 2 eigenvector and eigenvalue pairs.
- If we are working in 3 dimensions there are upto 3 eigenvector and eigenvalue pairs.
and so on.
As an example, if we have a rotation transform in 3 dimensions, then the eigenvector would be the axis of rotation since this is not altered by the transform and the corresponding eigenvalue would be +1 since the axis is not scaled by the rotation. If we have a rotation in 2 dimensions then the eigenvectors would be ±i where i is √-1 since all vectors in the plane change direction.
Eigenvalues
The eigenvalues of a matrix [M] are the values of
such that:
[M] {v} =
{v}
where {v} = a vector
this gives:
|M -
I| = 0
where I = identity matrix
this gives:

so
(m00-
) (m11-
)
(m22-
) + m01 m12 m20 + m02 m10
m21 - (m00-
) m12 m21 - m01 m10 (m22-
) - m02 (m11-
)
m20 = 0
the values of λ are the eigenvalues of the matrix
Eigenvectors
Associated with each eigenvalue λi is an eigenvector {ui} such that:
[M] {ui} = λi {ui}
where:
- [M] is a matrix
- λi is its eigenvalues (i=1,2,3)
- {ui}is its eigenvectors







