Chapter 3: Vector Spaces and Linear Mappings (Part I)
Definition and Fundamental Axioms of Vector Spaces
General Definition: A non-empty set is defined as a vector space over a field if it satisfies specific axioms related to internal and external operations. The elements of the field are referred to as scalars, while the elements of the set are called vectors.
Internal Law Analysis (Addition): The operation "+" represents the internal law. For to be a vector space, must be an abelian group, meaning it must satisfy the following five axioms: * Closure: For all , the sum must also be in . This signifies that is stable or closed under addition. * Associativity: For all , the grouping of elements does not change the result: . * Identity Element: There exists an element such that for all , . By default, any vector space must contain at least this element. This identity element is unique and is called the zero vector of . * Inverse or Symmetric Element: For every , there exists a unique element (written as or ) such that . * Commutativity: For all , the order of addition does not matter: . If all five axioms are met, is an abelian or commutative group.
External Law Analysis (Scalar Multiplication): The operation "." represents the external law. The following axioms must be satisfied: * Closure under Scalar Multiplication: For all and all scalars , the product must be in . * Compatibility with Multiplication in : For all and for all , results are consistent: . * Multiplicative Identity: For all , multiplying by the scalar yields the same vector: .
Axioms for Mixed Operations: These axioms relate both internal (addition) and external (multiplication) laws: * Distributivity over Addition of Scalars: For all and all , the operation follows . * Distributivity over Addition of Vectors: For all and all , the operation follows .
The Vector Space
Definition of : Let be a natural number where . The set consists of all -tuples , also called vectors, represented in the form . In this form, each is called the -th component of the vector.
Standard Operations in : * Addition of Vectors: For all where and , addition is defined component-wise: . * Multiplication by a Scalar: For all and all scalars , multiplication is defined component-wise: .
Properties of : The set is a vector space over the field of real numbers (an -vector space) because it satisfies: * (Associativity). * (Commutativity). * (Zero vector identity). * (Additive inverse). * (Compatibility). * (Scalar distributivity). * (Vector distributivity). * (Scalar unit identity).
Vector Subspaces and Linear Combinations
Definition of a Subspace: Let be a non-empty subset of an -vector space . is called a vector subspace of if for all and for all , the linear combination also belongs to .
Requirement for Subspaces: If is a subspace of , then is itself an -vector space.
Alternative Criteria for Subspaces: A non-empty subset is a subspace of if and only if: 1. For all , the sum . 2. For all and , the product . * This is equivalent to the condition: and .
Trivial and Basic Subspaces: * The set containing only the zero vector, , is always a subspace of . * The intersection of two subspaces and () is always a subspace of . * The union of two subspaces is not necessarily a subspace. It is a subspace if and only if one is contained within the other (either or ).
The Concept of Span: For vectors , the set defined as is the smallest vector space containing these vectors. * A vector belongs to the span if and only if there exist scalars such that . * Geometric Interpretation: If and , . This represents a straight line passing through the origin, collinear with vector .
Sums and Direct Sums of Subspaces
Sum of Two Subspaces: Let and be subspaces of . Their sum is defined as . The sum is a subspace of and is the smallest vector space containing both and .
Direct Sum Definition: Subspaces and are in a direct sum, denoted , if every vector can be uniquely decomposed as , where and . * Uniqueness Condition: If and (where and ), then it must follow that and .
Property of Direct Sums: Subspaces and are in a direct sum if and only if their intersection contains only the zero vector: .
Supplementary Subspaces: Subspaces and are called supplementary in if every vector in the entire space can be uniquely decomposed as a sum of a vector from and a vector from . This is equivalent to saying , which requires: 1. 2.
Linear Independence and Generating Sets
Linearly Independent Set: A set of vectors is linearly independent if the equation implies that all scalars must be zero ().
Linearly Dependent Set: A set is linearly dependent if there exist scalars , not all of which are zero, such that .
Specific Independence Examples: * Single Vector: A set containing one vector is independent iff . It is dependent iff . * Two Vectors: A set containing two vectors is independent iff they are not collinear. In other words, they are dependent iff one is a scalar multiple of the other ().
Generating Set: A set is a generating set of if every vector can be expressed as a linear combination of these vectors ().
Basis and Dimension in Finite Spaces
Finite Dimensional Vector Space: A vector space that possesses a finite generating set.
Basis of a Vector Space: A set is a basis for if it satisfies two conditions: 1. It is linearly independent. 2. It is a generating set of .
Coordinates: If is a basis, then every has a unique set of coordinates such that .
Dimension Definition: The dimension of a finite dimensional vector space is the number of vectors in any basis set. The cardinality (number of elements) is identical for all bases of a given space. * The dimension of the trivial space is .
Fundamental Dimensional Theorems (Theorem 4): In a space with : * Any independent set contains at most vectors. * Any independent set of exactly vectors is automatically a basis. * Any generating set contains at least vectors. * Any generating set of exactly vectors is automatically a basis. * Every generating set contains a basis (can be reduced by removing vectors). * Every independent set can be extended to form a basis (by adding vectors).
Canonical Bases and Rank
Canonical Basis of : Defined by vectors where the is at the -th position. Any vector can be written as . The dimension .
Space of Matrices : The set of all real matrices is a vector space with . * Canonical Basis of Matrices: Consists of matrices that have a at position and zeroes elsewhere.
Subspaces in Finite Spaces (Theorem 5): If is finite dimensional, any subspace is also finite dimensional, and . If , then .
Rank Definition: For a subset , the rank of is the dimension of the subspace generated by , denoted .
Rank Properties (Theorem 6): * (number of vectors). * (dimension of the space). * implies independent subset properties; specifically, iff is independent. * iff is a generating set of .
Grassman's Identity and Supplementary Condition: * Theorem 8: . * Theorem 7: and are supplementary iff AND .
Matrix Representation of Vectors and Rank
Coordinate Representation: For a basis , a vector is represented by the column vector .
Matrix of a Set of Vectors: For a set , the matrix is an matrix where each column is the coordinate vector of in basis .
Rank of a Matrix: Defined as the rank of the set of vectors formed by its columns. A square matrix of size is invertible if and only if .
Gaussian Elimination and Row Echelon Form: * Row Echelon Form Criteria: 1. All-zero rows are at the bottom. 2. The leading entry (pivot) of a non-zero row is to the right of the pivot of the row above it. * Rank Calculation: The rank of a matrix in row echelon form equals the number of non-zero rows. For example, a matrix with 3 non-zero rows in echelon form has a rank of 3. * Elementary Row Operations (used to reach echelon form without changing rank): 1. Permutation of any two rows. 2. Multiplication of a row by a non-zero scalar. 3. Adding a linear combination of other rows to a row.
Change of Basis
Transformation Matrix Definition: Let be the old basis and be the new basis. The matrix is formed by taking the coordinates of the vectors of the new basis expressed in terms of the old basis .
Properties of Transformation Matrices: * is always invertible. * The inverse matrix transforms coordinates from the new basis back to the old basis.
Change of Basis Formula: Let be the coordinates in basis and be the coordinates in basis . The relationship is: and .
Example in : If is the canonical basis and new vectors are , , and , the matrix is:
Example in : Given and . To find coordinates of in , the relationship is determined by inverting the matrix, leading to: