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14.5 The Discrete Fourier Transform  495


                                        We claim that
                                                                            N−1
                                                                          1       2πijk/N
                                                                     u j =     U k e                           (14.18)
                                                                          N
                                                                            k=0
                                        for j = 0,1,··· , N − 1. This is the inversion formula for the N-point DFT, and it is analogous
                                        to inversion formulas for the Fourier transform and for the Fourier cosine and sine transforms,
                                        with a summation replacing an integral.
                                           To verify equation (14.18) it is convenient to put W = e −2πi/N  . Then
                                                                      N
                                                                    W = 1 and W  −1  = e  2πi/N .
                                        Write
                                                             N−1            N−1
                                                           1       2πijk/N  1      − jk
                                                                U k e   =      U k W
                                                           N              N
                                                             k=0             k=0
                                                                            N−1    N−1
                                                                          1
                                                                        =           u r e −2πirk/N  W  − jk
                                                                          N
                                                                             k=0  r=0
                                                                            N−1 N−1
                                                                          1           rk  − jk
                                                                        =         u r W W
                                                                          N
                                                                             k=0 r=0
                                                                            N−1   N−1
                                                                          1
                                                                                      rk
                                                                        =      u r  W W   − jk
                                                                          N
                                                                             r=0  k=0
                                                                            N−1   N−1
                                                                          1
                                                                                         ) .
                                                                        =      u r  (W  r− j k
                                                                          N
                                                                             r=0  k=0
                                        Now, if r  = j then (again using the finite geometric series),
                                                                  N−1              r− j N
                                                                       r− j k  1 − (W  )
                                                                    (W   ) =            = 0
                                                                               1 − W  r− j
                                                                  k=0
                                        because
                                                               ) = e
                                                          (W  r− j N  −2π(r− j)  = 1 and W  r− j  = e 2πi(r− j)/N   = 1.
                                                           ) = 1, so
                                        But if r = j, then (W  r− j k
                                                                        N−1
                                                                             r− j k
                                                                          (W   ) = N.
                                                                        k=0
                                        Therefore, in the last double summation we need only retain the term when r = j in the
                                        summation with respect to r, yielding
                                                                 N−1
                                                                                     N−1
                                                                                N−1
                                                               1              1
                                                                   U k e 2πijk/N  =  u r  (W  r− j k
                                                                                             )
                                                              N               N
                                                                 k=0            r=0  k=0
                                                                              1
                                                                            =   u j N = u j .
                                                                              N
                                        14.5.3  DFT Approximation of Fourier Coefficients
                                        We will now complete the idea suggested at the beginning of this section, approximating Fourier
                                        coefficients by a discrete Fourier transform.




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                                   October 14, 2010  16:43  THM/NEIL   Page-495        27410_14_ch14_p465-504
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