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12.4. Singular Integral Equations of the First Kind


                 12.4-1. The Simplest Equation With Cauchy Kernel
               Consider the singular integral equation of the first kind


                                              1     ϕ(τ)
                                                        dτ = f(t),                          (1)
                                              πi  L  τ – t

               where L is a closed contour. Let us construct the solution. In this relation we replace the variable t
                                1 dτ 1
               by τ 1 , multiply by    , integrate along the contour L, and change the order of integration
                                πi τ 1 – t
               according to the Poincar´ e–Bertrand formula (see Subsection 12.2-6). Then we obtain

                              1     f(τ 1 )        1           1         dτ 1
                                        dτ 1 = ϕ(t)+    ϕ(τ) dτ                 .           (2)
                             πi  L  τ 1 – t        πi  L       πi  L  (τ 1 – t)(τ – τ 1 )

               Let us calculate the second integral on the right-hand side of (2):


                                 dτ 1       1       dτ 1      dτ 1     1
                                         =              –           =     (iπ – iπ)=0.
                            (τ 1 – t)(τ – τ 1 )  τ – t  τ 1 – t  τ 1 – τ  τ – t
                          L                      L         L
               Thus,
                                                    1     f(τ)
                                              ϕ(t)=          dτ.                            (3)
                                                    πi  L  τ – t

               The last formula gives the solution of the singular integral equation of the first kind (1) for a closed
               contour L.



                 12.4-2. An Equation With Cauchy Kernel on the Real Axis
               Consider the following singular integral equation of the first kind on the real axis:


                                      1     ∞  ϕ(t)
                                                 dt = f(x),  –∞ < x < ∞.                    (4)
                                      πi     t – x
                                         –∞
               Equation (4) is a special case of the characteristic integral equation on the real axis (see Subsec-
               tion 13.2-4). In the class of functions vanishing at infinity, Eq. (4) has the solution

                                            1     ∞  f(t)
                                     ϕ(x)=             dt,   –∞ < x < ∞.                    (5)
                                            πi    t – x
                                               –∞
                                  –1
               Denoting f(x)= F(x)i , we rewrite Eqs. (4) and (5) in the form

                           1     ∞  ϕ(t)                1     ∞  F(t)
                                      dt = F(x),  ϕ(x)= –          dt.  – ∞ < x < ∞.        (6)
                           π     t – x                  π     t – x
                              –∞                           –∞
               The two formulas (6) are called the Hilbert transform pair (see Subsection 7.6-3).




                 © 1998 by CRC Press LLC








               © 1998 by CRC Press LLC
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