Linear transformations are the mathematical superheroes of vector spaces. They preserve vector addition and scalar multiplication, allowing us to map one space to another while keeping the structure intact. These transformations are the backbone of many applications in physics and engineering.
Matrix representations give us a concrete way to work with linear transformations. By expressing transformations as matrices, we can perform calculations and analyze their properties. This powerful tool connects abstract concepts to practical computations, making linear algebra accessible and applicable.
Linear Transformations
Properties of linear transformations
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2.4 Products of Vectors | University Physics Volume 1 View original
Functions between vector spaces that preserve the vector space structure
Let V and W be vector spaces over the same field F, and let T:V→W be a function
T is a if for all vectors u,v∈V and scalars c∈F:
Satisfies additivity property: T(u+v)=T(u)+T(v)
Satisfies homogeneity property: T(cu)=cT(u)
Preserve vector addition and scalar multiplication operations
Map the zero vector of V to the zero vector of W: T(0V)=0W
The set of all linear transformations from V to W is denoted by L(V,W)
Matrix representation of transformations
Can be represented using matrices
Let V and W be finite-dimensional vector spaces with ordered bases B={v1,…,vn} and C={w1,…,wm}, respectively
For a linear transformation T:V→W, the of T with respect to the bases B and C is the m×n matrix A=[aij], where aij is the i-th coordinate of T(vj) with respect to the basis C
Matrix representation depends on the choice of bases for the domain and codomain
corresponds to the composition of linear transformations
If T:U→V and S:V→W are linear transformations with matrix representations A and B, respectively, then the matrix representation of the composition S∘T:U→W is the product BA
Matrix addition corresponds to the pointwise addition of linear transformations
Scalar multiplication of matrices corresponds to scalar multiplication of linear transformations
Kernel and range of transformations
The (or null space) of a linear transformation T:V→W is the set of all vectors in V that are mapped to the zero vector in W
ker(T)={v∈V:T(v)=0W}
The kernel is a subspace of the domain V
The (or image) of a linear transformation T:V→W is the set of all vectors in W that are the output of T for some input vector in V
range(T)={T(v):v∈V}
The range is a subspace of the codomain W
The nullity of a linear transformation T is the of its kernel: nullity(T)=dim(ker(T))
The of a linear transformation T is the dimension of its range: rank(T)=dim(range(T))
The relates the dimensions of the domain, kernel, and range of a linear transformation
For a linear transformation T:V→W, where V is finite-dimensional: dim(V)=rank(T)+nullity(T)
Invertibility of linear transformations
A linear transformation T:V→W is invertible (or bijective) if it is both injective (one-to-one) and surjective (onto)
Injective: For all u,v∈V, if T(u)=T(v), then u=v
Surjective: For every w∈W, there exists a v∈V such that T(v)=w
If T is invertible, there exists a unique linear transformation T−1:W→V called the inverse of T, such that:
T−1∘T=IV (the identity transformation on V)
T∘T−1=IW (the identity transformation on W)
A linear transformation T:V→W is invertible if and only if its kernel is trivial (contains only the zero vector)
Equivalently, T is invertible if and only if nullity(T)=0
For square matrices (linear transformations from a vector space to itself), a matrix is invertible if and only if its determinant is nonzero
The inverse of a matrix A, denoted by A−1, can be found using various methods