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Unit 24: Inner Product and Inner Product Spaces




                                                                                                Notes
                                       =  (  m  1 |  j ) (  m  1 |  j )
                                       = 0.

          Therefore { , . . . ,   } is an orthogonal set consisting of m + 1 non-zero vectors in the subspace
                    1     m+1
          spanned by  , . . . ,   . By theorem 2, it is a basis for this subspace. Thus the vectors  , . . . ,
                     1     m+1                                                  1     n
          may be constructed one after the other in accordance with (9). In particular, when n = 4, we have
                                     =
                                    1   1
                                           ( |  )
                                     =       2  1                                … (10)
                                    2   2      2  1
                                              1
                                           ( |  )    ( |  )
                                     =      3  1      3  2
                                    3   3      2  1      2  2
                                              1         2
                                           ( |  )    ( |  )    ( |  )
                                     =       4  1      4  2      4  3  .         … (11)
                                    4   4      2  1      2  2      2   3
                                              1         2         3
          Corollary: Every finite-dimensional inner product space has an orthonormal basis.
          Proof: Let V be a finite-dimensional inner product space and { , . . . ,  } a basis for V. Apply the
                                                            1     n
          Gram-Schmidt process to construct an orthogonal basis { , . . . ,  }. Then to obtain an orthonormal
                                                       1     n
          basis, simply replace each vector   by   /  .
                                      k    k   k
          One  of the  main advantages  which  orthonormal  bases have  over  arbitrary  bases is  that
          computations involving coordinates are simpler. To indicate in general terms why this is true,
          suppose that V is a finite-dimensional inner product space. Then, as in the last section, we may
          use Equation (5) to associate a matrix G with every ordered basis  = { , . . . ,  } of V. Using this
                                                                   1     n
          matrix
                                    G = ( | )
                                     jk   k  j
          we may compute inner products in terms of coordinates, If  is an orthonormal basis, then G is
          the identity matrix, and for any scalars x  and y
                                           j    k

                                         x     y        x y  .
                                          j  j  k  k     j  j
                                       j      k       j
          Thus in terms of an orthonormal basis, the inner product in  V looks like the standard  inner
          product in F .
                    n
          Although  it is  of  limited  practical use for computations,  it is  interesting  to  note  that  the
          Gram-Schmidt process may also be used to test for linear dependence. For suppose  , …,   are
                                                                              1    n
          linearly dependent vectors in an inner product space V. To exclude a trivial case, assume that
              0. Let m be the largest integer for which   , …,    are independent. Then 1   m < n. Let
           1                                    1     m
            , …,    be the vectors obtained by applying the orthogonalization process to   …,   . Then
           1     m                                                          1    m
          the vector   given by (9) is necessarily 0. For   is in the subspace spanned by   ,  , …,
                    m+1                           m+1                         1  2    n
          and orthogonal to each of these vectors; hence it is 0 by (6). Conversely it  , …,   are different
                                                                      1    n
          from 0 and    = 0, then   ,   , …,   are linearly dependent.
                     m+1        1  2   m+1
                 Example 12: Consider the vectors
                                       = (4, 0, 3)
                                      1



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