This paper considers general second kind integral equations of the form
phi(s) - integral(R)k(s,t)phi(t) dt = psi(s)
(in operator form phi-K(k)phi = psi), where the functions k and psi are ass
umed known. with psi is an element of Y,the space of bounded continuous fun
ctions on R, and k such that the mapping s --> k(s,.), from R to L-1(R), is
bounded and continuous. The function phi is an element of Y is the solutio
n to be determined. Conditions on a set W subset of BC(R L-1(R)) are obtain
ed such that a generalised Fredholm alternative holds: If Mi satisfies thes
e conditions and I - K-k is injective for all k is an element of W then I -
K-k is also surjective for all k is an element of W and, moreover, the inv
erse operators (I - K-k)(-1) on Y are uniformly bounded for k is an element
of W. The approximation of the kernel in the integral equation by a sequen
ce (k(n)) converging in a weak sense to k is also considered and results on
stability and convergence are obtained. These general theorems are used to
establish results for two special classes of kernels: k(s, t) = kappa(s -
t)z(t) and k(s, t) = kappa(s - t)lambda(s - t, t), where kappa is an elemen
t of L-1(R), z is an element of L-infinity(R), and lambda is an element of
BC((R\{0}) x R). Kernels of both classes arise in problems of time harmonic
wave scattering by unbounded surfaces. The general integral equation resul
ts are here applied to prove the existence of a solution for a boundary int
egral equation formulation of scattering by an infinite rough surface and t
o consider the stability and convergence of approximation of the rough surf
ace problem by a sequence of diffraction grating problems of increasingly l
arge period. (C) 2000 Academic Press.