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Chapter 9


               Methods for Solving Linear Equations

                                                     x
               of the Form y(x)–                      K(x, t)y(t) dt = f(x)
                                                   a




               9.1. Volterra Integral Equations of the Second Kind

                 9.1-1. Preliminary Remarks. Equations for the Resolvent
               In this chapter we present methods for solving Volterra integral equations of the second kind, which
               have the form
                                                  x
                                          y(x)–    K(x, t)y(t) dt = f(x),                   (1)
                                                a
               where y(x) is the unknown function (a ≤ x ≤ b), K(x, t) is the kernel of the integral equation, and
               f(x) is the right-hand side of the integral equation. The function classes to which y(x), f(x), and
               K(x, t) can belong are defined in Subsection 8.1-1. In these function classes, there exists a unique
               solution of the Volterra integral equation of the second kind.
                   Equation (1) is said to be homogeneous if f(x) ≡ 0 and nonhomogeneous otherwise.
                   The kernel K(x, t) is said to be degenerate if it can be represented in the form K(x, t)=
               g 1 (x)h 1 (t)+ ··· + g n (x)h n (t).
                   The kernel K(x, t) of an integral equation is called difference kernel if it depends only on the
               difference of the arguments, K(x, t)= K(x – t).
                   Remark 1. A homogeneous Volterra integral equation of the second kind has only the trivial
               solution.
                   Remark 2. The existence and uniqueness of the solution of a Volterra integral equation of the
               second kind hold for a much wider class of kernels and functions.
                   Remark 3. A Volterra equation of the second kind can be regarded as a Fredholm equation of
               the second kind whose kernel K(x, t) vanishes for t > x (see Chapter 11).
                   Remark 4. The case in which a =–∞ and/or b = ∞ is not excluded, but in this case the square
               integrability of the kernel K(x, t) on the square S = {a ≤ x ≤ b, a ≤ t ≤ b} is especially significant.
                   The solution of Eq. (1) can be presented in the form
                                                        x
                                          y(x)= f(x)+    R(x, t)f(t) dt,                    (2)
                                                      a
               where the resolvent R(x, t) is independent of f(x) and the lower limit of integration a and is
               determined by the kernel of the integral equation alone.
                   The resolvent of the Volterra equation (1) satisfies the following two integral equations:
                                                         x
                                      R(x, t)= K(x, t)+  K(x, s)R(s, t) ds,                 (3)
                                                       t



                 © 1998 by CRC Press LLC









               © 1998 by CRC Press LLC
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