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9.6. The Method of Model Solutions

                 9.6-1. Preliminary Remarks*
               Consider a linear equation, which we briefly write out in the form


                                                L [y(x)] = f(x),                            (1)

               where L is a linear (integral) operator, y(x) is an unknown function, and f(x) is a known function.
                   We first define arbitrarily a test solution

                                                 y 0 = y 0 (x, λ),                          (2)

               which depends on an auxiliary parameter λ (it is assumed that the operator L is independent of λ
               and y 0 /≡ const). By means of Eq. (1) we define the right-hand side that corresponds to the test
               solution (2):
                                              f 0 (x, λ)= L [y 0 (x, λ)].
               Let us multiply Eq. (1), for y = y 0 and f = f 0 , by some function ϕ(λ) and integrate the resulting
               relation with respect to λ over an interval [a, b]. We finally obtain

                                               L [y ϕ (x)] = f ϕ (x),                       (3)

               where
                                       b                          b

                              y ϕ (x)=  y 0 (x, λ)ϕ(λ) dλ,  f ϕ (x)=  f 0 (x, λ)ϕ(λ) dλ.    (4)
                                      a                          a
                   It follows from formulas (3) and (4) that, for the right-hand side f = f ϕ (x), the function y = y ϕ (x)
               is a solution of the original equation (1). Since the choice of the function ϕ(λ) (as well as of the
               integration interval) is arbitrary, the function f ϕ (x) can be arbitrary in principle. Here the main
               problem is how to choose a function ϕ(λ) to obtain a given function f ϕ (x). This problem can be
               solved if we can find a test solution such that the right-hand side of Eq. (1) is the kernel of a known
               inverse integral transform (we denote such a test solution by Y (x, λ) and call it a model solution).


                 9.6-2. Description of the Method
               Indeed, let P be an invertible integral transform that takes each function f(x) to the corresponding
               transform F(λ) by the rule
                                                F(λ)= P{f(x)}.                              (5)

                                             –1
               Assume that the inverse transform P  has the kernel ψ(x, λ) and acts as follows:
                                                                 b

                                 –1
                                                     –1
                               P {F(λ)} = f(x),    P {F(λ)}≡      F(λ)ψ(x, λ) dλ.           (6)
                                                                a
               The limits of integration a and b and the integration path in (6) may well lie in the complex plane.
                   Suppose that we succeeded in finding a model solution Y (x, λ) of the auxiliary problem for
                                                                       –1
               Eq. (1) whose right-hand side is the kernel of the inverse transform P :

                                              L [Y (x, λ)] = ψ(x, λ).                       (7)
              * Before reading this section, it is useful to look over Section 9.5.




                 © 1998 by CRC Press LLC









               © 1998 by CRC Press LLC
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