Linear transformations are mathematical functions that map vectors between spaces while preserving addition and scalar multiplication. Matrices provide a powerful way to represent these transformations, encoding their effects on basis vectors and allowing for efficient computations.
Matrix representations simplify complex transformations into multiplication operations. By applying the transformation to basis vectors and recording the results as matrix columns, we can easily perform and analyze linear transformations using familiar matrix operations.
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Linear transformations map vectors between vector spaces while preserving vector addition and scalar multiplication
Matrices represent linear transformations by encoding effects on basis vectors of input space
Columns of matrix representation correspond to images of basis vectors under linear transformation
For linear transformation T: R^n → R^m, matrix representation becomes m × n matrix
Matrix representation depends on choice of basis for domain and codomain vector spaces
Standard matrix representations use standard basis vectors for input and output spaces
Process of finding matrix representation involves applying transformation to each basis vector and recording results as matrix columns
Matrix representation process
Apply linear transformation to each basis vector of input space
Express resulting vectors as linear combinations of basis vectors in output space
Coefficients of linear combinations form columns of matrix representation
Ensure number of matrix rows matches output space dimension, columns match input space dimension
Use change of basis formula to convert between different matrix representations for non-standard bases
Verify matrix representation by testing on arbitrary vectors and comparing with direct application of linear transformation
Special cases like rotations, reflections, and scaling have characteristic matrix representations
Derive using geometric intuition or trigonometric formulas
Example: 2D rotation by angle θ has matrix representation [ cos θ − sin θ sin θ cos θ ] \begin{bmatrix} \cos θ & -\sin θ \\ \sin θ & \cos θ \end{bmatrix} [ cos θ sin θ − sin θ cos θ ]
Example: Reflection about y-axis has matrix representation [ − 1 0 0 1 ] \begin{bmatrix} -1 & 0 \\ 0 & 1 \end{bmatrix} [ − 1 0 0 1 ]
Action of linear transformation on vector equates to multiplying matrix representation by vector
For transformation T represented by matrix A and vector v, transformed vector becomes T(v) = Av
Matrix and vector dimensions must be compatible for multiplication
m × n matrix multiplied by n × 1 vector results in m × 1 vector
Matrix multiplication performed row by column, each entry in resulting vector becomes dot product
Order of multiplication matters: vector must be on right side of matrix (post-multiplication)
Composite transformations represented by matrix multiplication of respective matrices
Associative property of matrix multiplication allows efficient computation of multiple transformations
Example: For transformations A, B, C and vector v, (ABC)v = A(B(Cv))
Rank of matrix representation equals dimension of range (image) of linear transformation
Nullity of matrix representation equals dimension of kernel (null space) of linear transformation
Determinant of square matrix representation indicates invertibility of transformation
Non-zero determinant: invertible transformation
Zero determinant: non-invertible transformation
Eigenvalues and eigenvectors of matrix representation provide information about invariant subspaces and scaling factors
Trace of matrix representation remains invariant under similarity transformations and relates to sum of eigenvalues
Singular value decomposition (SVD) of matrix representation reveals principal directions and magnitudes of stretching or compression
Condition number of matrix representation indicates sensitivity of linear transformation to small input changes
Crucial for numerical stability in computations
Example: High condition number suggests transformation amplifies small errors, leading to unstable computations
Matrix multiplication mechanics
Multiply matrix representation by vector to perform linear transformation
Ensure matrix and vector dimensions are compatible
m × n matrix multiplied by n × 1 vector yields m × 1 vector
Perform row-by-column multiplication
Each entry in resulting vector becomes dot product of matrix row and vector
Maintain correct order: matrix on left, vector on right (post-multiplication)
Example: For 2×2 matrix A and 2×1 vector v, A = [ a b c d ] , v = [ x y ] A = \begin{bmatrix} a & b \\ c & d \end{bmatrix}, v = \begin{bmatrix} x \\ y \end{bmatrix} A = [ a c b d ] , v = [ x y ]
Transformed vector: A v = [ a x + b y c x + d y ] Av = \begin{bmatrix} ax + by \\ cx + dy \end{bmatrix} A v = [ a x + b y c x + d y ]
Represent composite transformations through matrix multiplication of individual transformation matrices
Order of multiplication matters: rightmost matrix applies first, leftmost matrix applies last
Associative property enables efficient computation of multiple transformations
Example: For transformations A, B, C applied in order (C first, then B, then A):
Composite transformation matrix: ABC
Applied to vector v: (ABC)v = A(B(Cv))
Use matrix multiplication to combine multiple transformations into a single matrix
Reduces computational complexity when applying to multiple vectors
Rank and nullity
Rank of matrix representation equals dimension of transformation's range (image)
Determines number of linearly independent output vectors
Nullity of matrix representation equals dimension of transformation's kernel (null space)
Represents number of linearly independent vectors mapped to zero vector
Rank-nullity theorem : rank(A) + nullity(A) = number of columns in A
Fundamental relationship between input and output spaces
Example: For a 3×3 matrix with rank 2, nullity must be 1 (2 + 1 = 3)
Determinant and invertibility
Determinant of square matrix representation indicates transformation's invertibility
Non-zero determinant: invertible (one-to-one and onto) transformation
Zero determinant: non-invertible transformation (many-to-one or not onto)
Determinant also represents scaling factor of transformation on volumes
Absolute value of determinant gives factor by which volumes are scaled
Example: Determinant of rotation matrix always equals 1, preserving areas and volumes
Eigenvalues and eigenvectors
Eigenvalues of matrix representation represent scaling factors along specific directions
Eigenvectors correspond to directions unchanged by transformation (except for scaling)
Characteristic equation det(A - λI) = 0 used to find eigenvalues
Eigenvectors found by solving (A - λI)v = 0 for each eigenvalue λ
Example: For scaling matrix [ 2 0 0 3 ] \begin{bmatrix} 2 & 0 \\ 0 & 3 \end{bmatrix} [ 2 0 0 3 ]
Eigenvalues: 2 and 3
Eigenvectors: [1, 0]^T and [0, 1]^T respectively