Page 151 - Handbook Of Integral Equations
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Differentiating (4) with respect to x and taking account of (3), we obtain

                                                  n                        n



                                  y (x)+ σ n y(x)+  A k λ k I k = f (x),  σ n =  A k .      (5)
                                                              x
                                   x
                                                 k=1                       k=1
                     Eliminating the integral I n from (4) and (5), we find that
                                                     n–1




                                y (x)+ σ n – λ n )y(x)+  A k (λ k – λ n )I k = f (x) – λ n f(x).  (6)
                                 x                                     x
                                                     k=1
                     Differentiating (6) with respect to x and eliminating I n–1 from the resulting equation with
                     the aid of (6), we obtain a similar equation whose left-hand side is a second-order linear
                                                                                 n–2
                                                                                     1
                     differential operator (acting on y) with constant coefficients plus the sum  A I k .If we
                                                                                     k
                                                                                 k=1
                     proceed with successively eliminating I n–2 , I n–3 , ... , I 1 with the aid of differentiation and
                     formula (3), then we will finally arrive at an nth-order linear nonhomogeneous ordinary
                     differential equation with constant coefficients.
                        The initial conditions for y(x) can be obtained by setting x = a in the integral equation
                     and all its derivative equations.
                     2 . The solution of the equation can be represented in the form
                      ◦
                                                        n
                                                      x
                                        y(x)= f(x)+        B k e µ k (x–t)  f(t) dt.        (7)
                                                     a
                                                        k=1
                     The unknown constants µ k are the roots of the algebraic equation

                                                   n
                                                      A k

                                                           + 1 = 0,                         (8)
                                                     z – λ k
                                                  k=1
                     which is reduced (by separating the numerator) to the problem of finding the roots of an
                     nth-order characteristic polynomial.
                        After the µ k have been calculated, the coefficients B k can be found from the following
                     linear system of algebraic equations:
                                          n
                                               B k

                                                    +1 = 0,    m =1, ... , n.               (9)
                                             λ m – µ k
                                         k=1
                                                                   ◦
                     Another way of determining the B k is presented in item 3 below.
                        If all the roots µ k of equation (8) are real and different, then the solution of the original
                     integral equation can be calculated by formula (7).
                        To a pair of complex conjugate roots µ k,k+1 = α ± iβ of the characteristic polynomial (8)
                     there corresponds a pair of complex conjugate coefficients B k,k+1 in equation (9). In this case,
                     the corresponding terms B k e µ k (x–t)  + B k+1 e µ k+1 (x–t)  in solution (7) can be written in the form


                     B k e α(x–t)   cos β(x – t) + B k+1 e α(x–t)   sin β(x – t) , where B k and B k+1 are real coefficients.
                      ◦
                     3 .For a = 0, the solution of the original integral equation is given by
                                               x

                                                                         –1
                                  y(x)= f(x) –   R(x – t)f(t) dt,  R(x)= L  R(p) ,         (10)
                                              0

                 © 1998 by CRC Press LLC









               © 1998 by CRC Press LLC
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