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14.1 The Fourier Integral  467


                                                                     1     1         2sin(ω)
                                                                A ω =     cos(ωξ)dξ =
                                                                     π  −1             πω
                                        and
                                                                        1     1
                                                                   B ω =     sin(ωξ)dξ = 0.
                                                                        π  −1
                                        The Fourier integral of f is
                                                                      ∞

                                                                        2sin(ω)
                                                                              cos(ωx)dω.
                                                                         πω
                                                                     0
                                        Because f is continuous for x  =±1, the integral converges to f (x) for x  =±1. At x = 1the
                                        integral converges to
                                                                1                 1        1
                                                                 ( f (1+) + f (1−)) = (1 + 0) = .
                                                                2                 2        2
                                        Similarly, the integral converges to 1/2at x =−1. This Fourier integral is a faithful representation
                                        of the function except at 1 and −1, where it averages the ends of the jump discontinuities there.
                                           In view of this convergence, we have
                                                                                 ⎧
                                                                                 ⎪1     for −1 < x < 1
                                                         1     ∞  2sin(ω)        ⎨
                                                                     cos(ωx)dω = 1/2    for x =±1
                                                         π  0    ω               ⎪
                                                                                   0    for |x| > 1.
                                                                                 ⎩
                                           There is another expression for the Fourier integral of a function that is sometimes
                                        convenient to use. Insert the coefficients into the Fourier integral:
                                              ∞

                                                [A ω cos(ωx) + B ω sin(ωx)]dω =
                                              0

                                              ∞        ∞                             ∞
                                                   1                              1
                                                         f (ξ)cos(ωξ)dξ cos(ωx) +      f (ξ)sin(ωξ)dξ sin(ωx) dω
                                                   π                              π
                                              0       −∞                            −∞
                                               1     ∞     ∞
                                             =          f (ξ)[cos(ωξ)cos(ωx) + sin(ωξ)sin(ωx)]dξ dω
                                               π  0  −∞
                                               1     ∞     ∞
                                             =          f (ξ)cos(ω(ξ − x))dξ dω.
                                               π  0  −∞
                                        This gives us the equivalent Fourier integral representation
                                                               1     ∞     ∞
                                                                         f (ξ)cos(ω(ξ − x))dξ dω                (14.4)
                                                               π  0   −∞
                                        of f (x) on the real line.



                               SECTION 14.1        PROBLEMS



                            In each of Problems 1 through 10, write the Fourier integral  k  for −10 ≤ x ≤ 10
                                                                           2. f (x) =
                            representation (14.1) of the function and determine what  0  for |x| > 10
                            this integral converges to.
                                                                                   ⎧
                                                                                   ⎪−1for −π ≤ x ≤ 0
                                                                                   ⎨

                                      x  for −π ≤ x ≤ π                    3. f (x) = 1  for 0 < x ≤ π
                             1. f (x) =                                            ⎪
                                                                                   ⎩
                                      0  for |x| >π                                  0   for |x| >π
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                                   October 14, 2010  16:43  THM/NEIL   Page-467        27410_14_ch14_p465-504
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