Linear mapping (linear transformation)
A linear mapping is a function between vector spaces that preserves vector addition and scalar multiplication. This article explains definition, properties, matrix form, examples, and applications.
Overview
A linear mapping, also called a linear transformation or linear operator, is a function between two vector spaces that preserves the vector space operations: addition and scalar multiplication. Formally, a function f satisfies f(u+v)=f(u)+f(v) and f(cu)=c f(u) for all vectors u,v and scalars c. Linear mappings are central in mathematics and especially in linear algebra, where they describe structure-preserving correspondences between spaces.
Image gallery
3 ImagesKey properties
Important consequences of linearity include that f(0)=0, f applied to a linear combination equals the same linear combination of images, and the image of a subspace is a subspace. The kernel (null space) and image (range) are fundamental invariants used to classify mappings and compute dimensions.
- Additivity: f(u+v)=f(u)+f(v).
- Homogeneity: f(cu)=c f(u).
- Kernel & image: ker(f) and im(f) measure failure of injectivity and surjectivity.
Matrix representation
Given bases of domain and codomain, every linear mapping can be represented by a matrix. Composition of linear maps corresponds to matrix multiplication; invertible linear maps correspond to invertible matrices. Changing bases applies a similarity or conjugation transform to the matrix representation. See a basic reference: linear maps and matrices.
Examples and applications
Common examples include rotations, reflections, projections, and scaling in Euclidean spaces, all of which are linear maps represented by matrices. Linear mappings model systems in physics, engineering, computer graphics, data analysis, and differential equations. Finite-dimensional examples are often taught alongside computations of rank, determinant, and eigenvalues; infinite-dimensional examples appear in functional analysis.
History and context
The concept evolved as part of 19th-century algebra and geometry, becoming formalized with the development of vector space axioms. Modern treatments place linear mappings at the heart of abstract algebraic structures and categorical perspectives. For more background and rigorous definitions consult general references and introductory texts on vector spaces.
Distinctions and notable facts
Not every function between vector spaces is linear; nonlinear maps like translations are excluded. Linear maps preserve origin and straight lines through origin but need not preserve lengths or angles unless additional structure (inner product) is respected. Computational tools often reduce problems about linear maps to matrix algorithms; further topics include canonical forms and spectral theory. Further reading: advanced topics.
Definition
Let and be
vector spaces over a common ground body
. A mapping
is called a linear mapping if for all
and
the following conditions hold:
is homogeneous:
is additive:
The two conditions above can also be combined:
For this transitions into the condition for homogeneity and for
into that for additivity. Another equivalent condition is the requirement that the graph of the mapping is
a subvector space of the sum of the vector spaces
and
Explanation
A mapping is linear if it is compatible with the vector space structure. That is, linear mappings are compatible with both the underlying addition and scalar multiplication of the domain of definitions and values. Compatibility with addition means that the linear mapping preserves sums. If we
have a sum
with the domain of definition, then
and thus this sum is preserved after the mapping in the range of values:
This implication can be shortened by substituting the premise
into Thus, we obtain the requirement
. Analogously, compatibility can be described by scalar multiplication. This is satisfied if from the relation
with the scalar λ
and
in the domain of definition it follows that also
holds in the domain of values:
After substituting the premise into the conclusion
we obtain the claim
.
· 
Visualization of compatibility with vector addition: each vector given by ,
and
addition triangle is
preserved by the linear mapping Also
,
and
forms an addition triangle and it holds that
.
· 
For mappings that are not compatible with addition, there are vectors ,
and
, so that
,
and
not form an addition triangle because
. Such a mapping is not linear.
· 
Visualization of compatibility with scalar multiplication: any scaling λ preserved by a linear mapping and it holds
.
· 
If a mapping is not compatible with scalar multiplication, then there is a scalar λ and a vector
, such that the scaling λ
not
map to the scaling λ Such a mapping is not linear.
Examples
- For any linear mapping has the form
with
.
- Let
and
. Then, for each
-matrix
using matrix multiplication, we obtain a linear mapping
by
defined. Any linear mapping fromto
can be represented in this way.
- If
an open interval,
the
-vector space of continuously differentiable functions on
and
of
-vector space of continuous functions on
, then the mapping
,
,
which assigns to
each functionits derivative, linear. The same holds for other linear differential operators.
· 
The stretch is a linear mapping. In this mapping, the
component is
stretched by a factor of .
· 
This mapping is additive: it doesn't matter if you first add vectors and then map them, or if you first map the vectors and then add them: .
· 
This mapping is homogeneous: it does not matter whether you first scale a vector and then map it, or whether you first map the vector and then scale it: .
Image and core
Two sets important in considering linear mappings are the image and the kernel of a linear mapping .
- The image
the mapping is the set of image vectors under
, that is, the set of all
with
from
. Therefore, the image set is also
notated by The image is a subvector space of
.
- The kernel
the mapping is the set of vectors from
, which are
mapped by
to the zero vector of It is a subvector space of
. The mapping
is injective exactly if the kernel contains only the zero vector.
Properties
- A linear mapping between the vector spaces
and
maps the zero vector of
to the zero vector of
, because
- A relation between kernel and image of a linear mapping
is described by the homomorphism : The factor space
is isomorphic to the image
.
Linear mappings between finite dimensional vector spaces.
Base
A linear mapping between finite-dimensional vector spaces is uniquely determined by the images of the vectors of a basis. If the vectors form a basis of the vector space
and are
vectors in
, then there exists exactly one linear mapping
, which maps
to
,
on
, ..., b_{n}}
maps to If
is any vector from
, then it can be uniquely represented as a linear combination of the basis vectors:
Here are the coordinates of the vector with respect to the basis
. Its image
is given by
The mapping is injective if and only if the image vectors
the basis are linearly independent. It is surjective if and only if
span the target space
If one assigns to each element a basis of
vector
from
arbitrarily, then one can use the above formula to continue this assignment uniquely to a linear mapping
.
Representing the image vectors with respect to a basis of
leads to the matrix representation of the linear mapping.
Mapping matrix
→ Main article: Mapping matrix
If and are
finite dimensional,
,
, and are bases
of
and
of
given, then any linear mapping
be represented by an
matrix This is obtained as follows: For each basis vector
from
the image vector
represented
as a linear combination of the basis vectors
The ,
,
form the entries of the matrix
:
Thus, in the -th column are the coordinates of
respect to the base
.
Using this matrix, one can calculate the image vector
of each vector
Thus, for the coordinates of with respect to
following holds true
.
This can be expressed using matrix multiplication:
The matrix is called the mapping matrix or representation matrix of
. Other notations for
are
and
.
Dimension formula
→ Main article: Rank set
Image and core are related by the dimension theorem. This states that the dimension of is equal to the sum of the dimensions of the image and the core:
Linear mappings between infinite-dimensional vector spaces.
→ Main article: Linear operator
Especially in functional analysis one considers linear mappings between infinite-dimensional vector spaces. In this context, the linear mappings are usually called linear operators. The considered vector spaces usually carry the additional structure of a normalized complete vector space. Such vector spaces are called Banach spaces. In contrast to the finite dimensional case, it is not sufficient to study linear operators only on one basis. According to the Bairean category theorem, a basis of an infinite-dimensional Banach space has overcountably many elements and the existence of such a basis cannot be justified constructively, that is, only by using the axiom of selection. Therefore, one uses a different notion of bases, such as orthonormal bases or, more generally, Schauder bases. With this, certain operators such as Hilbert-Schmidt operators can be represented with the help of "infinite matrices", in which case infinite linear combinations must also be allowed.
Special linear mappings
Monomorphism
A monomorphism between vector spaces is a linear mapping , which is injective. This is true exactly if the column vectors of the representation matrix are linearly independent.
Epimorphism
An epimorphism between vector spaces is a linear mapping , which is surjective. This is the case exactly if the rank of the representation matrix is equal to the dimension of
Isomorphism
An isomorphism between vector spaces is a linear mapping , which is bijective. This is exactly the case if the representation matrix is regular. The two spaces
and
then called isomorphic.
Endomorphism
An endomorphism between vector spaces is a linear mapping where the spaces and
equal:
. The representation matrix of this mapping is a square matrix.
Automorphism
An automorphism between vector spaces is a bijective linear mapping where the spaces and are
equal. Thus, it is both an isomorphism and an endomorphism. The representation matrix of this mapping is a regular matrix.
Vector space of linear mappings
The set of linear mappings from a
-vector space
to a
-vector space
is a vector space over
, more precisely: a subvector space of the
-vector space of all mappings from
to
. This means that the sum of two linear mappings
and
, component-wise defined by
is again a linear mapping and that the product
of a linear mapping with a scalar λis also a linear mapping again.
If has dimension
and
dimension
and if
a base
and
a base
the mapping is
into the matrix space is an isomorphism. Thus the vector space
has dimension
.
If we consider the set of linear self-mappings of a vector space, i.e. the special case , these form not only a vector space, but with the concatenation of mappings as multiplication, an associative algebra,
denoted briefly by
Generalization
A linear mapping is a special case of an affine mapping.
Replacing the body by a ring in the definition of the linear mapping between vector spaces, we obtain a moduli homomorphism.
Related articles
Author
AlegsaOnline.com Linear mapping (linear transformation) Leandro Alegsa
URL: https://en.alegsaonline.com/art/58264
Sources
- en.wikibooks.org : Linear Algebra/Linear Transformations
- cfsv.synechism.org : "The Calculus of Functions of Several Variables, Linear and Affine Functions"


