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496    CHAPTER 14  The Fourier Integral and Transforms



                                                             0.8



                                                             0.4


                                                              0
                                                     –4   –2    0   2    4    6    8   10
                                                                           t
                                                            –0.4





                                                     FIGURE 14.7  f (t) = sin(t) for 0 ≤ t < 4, period 4.



                                    To see the idea in action, consider the example of a function f having fundamental period
                                 4, and f (t) = sin(t) for 0 ≤ t < 4. A graph of this function is shown in Figure 14.7. With p = 4
                                 the Fourier coefficients are
                                                      1     4             1     4
                                                  d k =   sin(ξ)e −2πikξ/4  dξ =  sin(ξ)e −πikξ/2  dξ
                                                      4  0                4  0
                                                      cos(4) − 1  1 πk sin(4)
                                                    =          + i
                                                       π k − 4   2 π k − 4
                                                        2 2
                                                                     2 2
                                 for k = 0,±1,±2,···.
                                    Let N be a positive integer and subdivide [0,4] into N subintervals of equal lengths 4/N.
                                 These subintervals are

                                                        4 j 4( j + 1)
                                                          ,         for j = 0,1,··· , N − 1.
                                                        N     n
                                 Select N numbers 4 j/N by choosing the left endpoint of each of these subintervals. These define
                                 an N-point sequence u, where
                                                                         4 j

                                                                u j = sin    .
                                                                         n
                                 The N-point DFT of u is
                                                       N−1                N−1
                                                              4 j                4 j

                                                  U k =   sin     e  −2πijk/4  =  sin  e −πijk/2 .
                                                              N                   N
                                                       j=0                 j=0
                                 Now
                                                                   N−1
                                                           !     1        4 j
                                                            U k =     sin     e −πijk/2
                                                          N      N         N
                                                                   j=0
                                 is a Riemann sum for the integral defining d k .
                                    We now ask: To what extent does (1/N)U k approximate d k ? In this example we have
                                 an explicit expression for d k , so we can explore this question directly. We will evaluate
                                                                           N−1
                                 (1/N)U k using a = 4/N in the DFT of [sin( ja)]  j=0  determined in Example 14.15. This
                                 gives us




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                                   October 14, 2010  16:43  THM/NEIL   Page-496        27410_14_ch14_p465-504
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