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Chapter 11


               Methods for Solving Linear Equations

                                                    b

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



               11.1. Some Definition and Remarks


                 11.1-1. Fredholm Equations and Equations With Weak Singularity of the Second Kind
               Linear integral equations of the second kind with constant limits of integration have the form

                                                   b
                                         y(x)– λ   K(x, t)y(t) dt = f(x),                   (1)
                                                 a
               where y(x) is the unknown function (a ≤ x ≤ b), K(x, t)isthe kernel of the integral equation,
               and f(x) is a given function, which is called the right-hand side of Eq. (1). For convenience
               of analysis, a number λ is traditionally singled out in Eq. (1), which is called the parameter of
               integral equation. The classes of functions and kernels under consideration were defined above in
               Subsections 10.1-1 and 10.1-2. Note that equations of the form (1) with constant limits of integration
               and with Fredholm kernels or kernels with weak singularity are called Fredholm equations of the
               second kind and equations with weak singularity of the second kind, respectively.
                   A number λ is called a characteristic value of the integral equation (1) if there exist nontrivial
               solutions of the corresponding homogeneous equation (with f(x) ≡ 0). The nontrivial solutions
               themselves are called the eigenfunctions of the integral equation corresponding to the characteristic
               value λ.If λ is a characteristic value, the number 1/λ is called an eigenvalue of the integral
               equation (1). A value of the parameter λ is said to be regular if for this value the above homogeneous
               equation has only the trivial solution. Sometimes the characteristic values and the eigenfunctions
               of a Fredholm integral equation are called the characteristic values and the eigenfunctions of the
               kernel K(x, t).
                   The kernel K(x, t) of the integral equation (1) is called a degenerate kernel if it has the form
               K(x, t)= g 1 (x)h 1 (t)+ ··· + g n (x)h n (t), a difference kernel if it depends on the difference of the
               arguments (K(x, t)= K(x–t)), and a symmetric kernel if it satisfies the condition K(x, t)= K(t, x).
                   The transposed integral equation is obtained from (1) by replacing the kernel K(x, t)by K(t, x).

                   Remark 1. The variables t and x may vary in different ranges (e.g., a ≤ t ≤ b and c ≤ x ≤ d).
               To be specific, from now on we assume that c = a and d = b (this can be achieved by the linear
               substitution x = α ¯x + β with the aid of an appropriate choice of the constants α and β).
                   Remark 2. In general, the case in which the limits of integration a and/or b can be infinite is
               not excluded; however, in this case, the validity of the condition that the kernel K(x, t) is square
               integrable on the square S = {a ≤ x ≤ b, a ≤ t ≤ b} is especially significant.




                 © 1998 by CRC Press LLC








               © 1998 by CRC Press LLC
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