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Chapter 3


               Linear Equation of the First Kind

               With Constant Limits of Integration






                 Notation: f = f(x), g = g(x), h = h(x), K = K(x), and M = M(x) are arbitrary functions (these
               may be composite functions of the argument depending on two variables x and t); A, B, C, a, b, c,
               k, α, β, γ, λ, and µ are free parameters; and n is a nonnegative integer.


               3.1. Equations Whose Kernels Contain Power-Law
                      Functions

                 3.1-1. Kernels Linear in the Arguments x and t

                         1
               1.       |x – t| y(t) dt = f(x).
                      0
                     1 . Let us remove the modulus in the integrand:
                      ◦
                                          x              1

                                           (x – t)y(t) dt +  (t – x)y(t) dt = f(x).         (1)
                                         0              x
                     Differentiating (1) with respect to x yields

                                                x         1
                                                y(t) dt –  y(t) dt = f (x).                 (2)

                                                                  x
                                              0         x
                     Differentiating (2) yields the solution
                                                         1

                                                   y(x)= f (x).                             (3)
                                                         2 xx
                     2 . Let us demonstrate that the right-hand side f(x) of the integral equation must satisfy
                      ◦
                                                                                  1

                     certain relations. By setting x = 0 and x = 1 in (1), we obtain two corollaries  ty(t) dt = f(0)
                                                                                 0
                           1
                     and  (1 – t)y(t) dt = f(1), which can be rewritten in the form
                         0
                                         1                  1
                                         ty(t) dt = f(0),   y(t) dt = f(0) + f(1).          (4)
                                       0                  0
               In Section 3.1, we mean that kernels of the integral equations discussed may contain power-law functions or modulus of
               power-law functions.



                 © 1998 by CRC Press LLC









               © 1998 by CRC Press LLC
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