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13.7 Filtering of Signals  463



                                                        1                                        1



                                                       0.5
                                                                                                0.5
                                                        0                         –3   –2   –1     0   1     2    3
                                         –3   –2   –1     0    1    2    3                       0

                                                      –0.5
                                                                                               –0.5

                                                       –1
                                                                                                –1

                                         FIGURE 13.24 Tenth partial sum and Cesàro
                                                                                  FIGURE 13.25 Thirtieth partial sum and
                                         sum of f .
                                                                                  Cesàro sum of f .


                                           There are many filters used in signal analysis. Two of the more frequently used ones are the
                                        Hamming and Gauss filters.



                                          The Hamming filter is named for Richard Hamming, who was a senior research scientist
                                          at Bell Labs, and is defined by
                                                                   Z(t) = 0.54 + 0.46cos(πt).
                                          The Gauss filter is sometimes used to filter out background noise and is defined by
                                                                                  2 2
                                                                        Z(t) = e −απ t  ,
                                          with α a positive constant.







                               SECTION 13.7        PROBLEMS


                                                                                  ⎧
                            In each of Problems 1 through 5, graph the function, the  ⎪−1  for −1 ≤ t < −1/2
                                                                                  ⎨
                            fifth partial sum of its Fourier series on the interval, and  3. f (t) = 0  for −1/2 ≤ t < 1/2
                            the fifth Cesàro sum, using the same set of axes. Repeat this  ⎪
                                                                                    1   for 1/2 ≤ t < 1
                                                                                  ⎩
                            process for the tenth and twenty-fifth partial sums. Notice
                            in particular the graphs at points of discontinuity of the

                            function, where the Gibbs phenomenon appears.          0      for −3 ≤ t < 0
                                                                           4. f (t) =
                                                                                   cos(t) for 0 ≤ t < 3

                                     1   for 0 ≤ t < 2
                            1. f (t) =
                                     −1for −2 ≤ t < 0
                                                                                   2 + t  for −1 ≤ t < 0
                                                                           5. f (t) =

                                     t 2  for −2 ≤ t < 1                           7     for 0 ≤ t < 1
                            2. f (t) =
                                     2 + t  for 1 ≤ t < 2
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