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Unit 9: Representation of Transformations by Matrices




          use of the action of a linear transformation on this basis. Once this much is achieved by means of  Notes
          the operations in A(V), we can induce operations for the symbols created, making of them an
          algebra. This new object, infused with an algebraic life of its own, can be studied as a mathematical
          entity having an interest by itself. This study is what comprises the subject of matrix theory.
          However  to ignore  the source  of these  matrices,  that  is, to  investigate the  set of  symbol
          independently of what they represent, can be costly. Instead we shall always use the interplay
          between the  abstract,  A(V),  and the concrete, the  matrix algebra, to obtain information  one
          about the other.
          Let V be an n-dimensional vector space over the field F and let W be an m-dimensional vector
          space over F. Let   1  ,...,  n  be an ordered basis for V and  '  1 ,...,  m  an ordered basis for
          W. If T is any linear transformation from  V into W, then T is determined by its action on the
          vectors   . Each of the n vectors T   is uniquely expressible as a linear combination
                  j                    j

                       m
                  T  j   A ij  i                                                   ...(1)
                       i  1

          of the   i the scalars  A ij ,...A being the coordinates of T  j   in the ordered basis  '. Accordingly,
                                mj
          the transformation T is determined by the mn scalars  A  via the formula (1). The  m n matrix A
                                                      ij
                      ,
          defined by  A i j  A ij  is called the matrix of T relative to the pair of ordered basis   and  '.  Our
          immediate  task  is  to  understand  explicitly  how  the  matrix  A  determines  the  linear
          transformation T.

          If   x  1  1  ... x n  n is a vector in V, then


                      n
          T        T    x  j  j
                      j  1

                    n
                      x T
                       j   j
                    j  1

                    n   m
                      x   A
                       j   ij  i
                    j  1  j  1


                    m   n
                          A x j  i .
                           ij
                    i  1  j  1
          If X is the coordinate matrix of   in the ordered basis  , then the computation above shows that
          AX is the coordinate matrix of the vector  T in the ordered basis  ’ , because the scalar
                   n
                    A x  j
                      ij
                  j  1
          is the entry in the ith row of the column matrix AX. Let us also observe that if A is any  m n
          matrix over the field F, then




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