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306              Chapter 5                    Norms, Inner Products, and Orthogonality

                                                                                                n
                                   5.4.17. Construct an example using the standard inner product in    to show
                                           that two vectors x and y can have an angle between them that is close
                                                           T
                                           to π/2 without x y being close to 0. Hint: Consider n to be large,
                                           and use the vector e of all 1’s for one of the vectors.

                                   5.4.18. It was demonstrated in Example 5.4.3 that y is linearly correlated with
                                           x in the sense that y ≈ β 0 e + β 1 x if and only if the standardization
                                           vectors z x and z y are “close” in the sense that they are almost on the
                                                        n
                                           same line in   . Explain why simply measuring  z x − z y    does not
                                                                                                2
                                           always gauge the degree of linear correlation.
                                   5.4.19. Let θ be the angle between two vectors x and y from a real inner-
                                           product space.
                                              (a) Prove that cos θ =1 if and only if y = αx for α> 0.
                                              (b) Prove that cos θ = −1if and only if y = αx for α< 0.
                                           Hint: Use the generalization of Exercise 5.1.9.


                                   5.4.20. With respect to the orthonormal set
                                                                                                !
                                                         1   cos t cos 2t   sin t sin 2t sin 3t
                                                  B =   √   , √ , √     ,..., √ , √   , √   ,... ,
                                                         2π    π     π        π     π     π
                                           determine the Fourier series expansion of the saw-toothed function
                                           defined by f(t)= t for −π< t < π. The periodic extension of this
                                           function is depicted in Figure 5.4.3.

                                                                            π



                                                                   −π               π




                                                                           −π

                                                                     Figure 5.4.3
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