Rank-Nullity Theorem
Let be a linear mapping. The rank of is the dimension of the image, The rank is an invariant of the map.
The dimension of the kernel, is said nullity of a mapping.
Theorem
Under the hypothese: the sum of rank and nullity of a mapping is equal to the dimension of the vector space : Usually is the hardest to calculate and this theorem allows an easy way to compute it as
Proof
If then is injective. If the basis spans the image, the vectors are linearly independent.
Corollaries of Rank-Nullity Theorem
Let be an endomorphism where is a finite-dimensional vector space.
- If is injective then it is also surjective
- if is surjective then it is also injective
Corollary
Let be a linear mapping with and .
- Consider . Follows that the mapping is not injective.
- Consider . Follows that the mapping is not surjective
Eigenvalues and Eigenvectors
Let be an endomorphism where is a vectors space with dimension . Every vector such that with a scalar and is said eigenvector of the endomorphism related to the eigenvalue Eigenvalue and eigenvector are building blocks of reality
Dan terms: = eigenvalue (num of x) = eigenvector (any number) homogeneous = (0,0)
Eigenspace
Let be an endomorphism The set with defined as This is said eigenspace of the endomorphism related to the eigenvalue . The dimension of the eigenspace is said geometric multiplicity of the eigne value and is indicated with
Determining Eigenvalues and Eigenvectors
Let be an endomorphism. Let be the order characteristic polynomial related to the endomorphism. The number of roots of is called algebraic multiplicity.
Introduction to Diagonalization
One variable for each line in a diagonal manner. Not all the mappings/matrices can be diagonalized, Need to have enough linearly independent columns of .
Let be an endomorphism. The matrix is diagonalizable if and only if it has n linearly independent eigenvectors:
- All the eigenvalues are distinct
- The algebraic multiplicity of each eigenvalue coincides with its geometric multiplicity
Symmetric Mappings
If the mapping is characterised by a symmetric matrix, then can prove that;
- The mapping is always diagonalisable
- The transformation matrix can be built to be orthogonal (. Also means the new reference system given by the eigenvectors is also a convenient orthogonal system