Fundamental solutions for horizontally polarized shear (SH) waves propagati
ng in continuous medium with an arbitrarily large random wave number an der
ived herein. These fundamental solutions, or Green's functions, besides bei
ng useful in their own right, also serve as kernel functions for integral e
quation formulations that can be used in the numerical solution of elastic
wave scattering problems of practical importance. Thus, the present work se
rves as an extension of earlier derivations of boundary integral equation s
tatements based on the perturbation approach by removing the assumption of
small fluctuations of key medium properties about their mean values. The me
thodology developed here is based on a series expansion of the fundamental
solutions of the SH wave equation under time harmonic conditions using an o
rthogonal polynomial basis (polynomial chaos) for the randomness. The posit
ion-dependent coefficients of this expansion are subsequently found from th
e resulting vector wave equation, which is uncoupled through use of the eig
ensolution of its system matrix. Finally, some representative cases are sol
ved and the results are contrasted with those obtained by the perturbation
method. At the same time, the accuracy of the solution to the number of ter
ms used in the polynomial expansion is investigated. (C) 1999 Elsevier Scie
nce Ltd. All rights reserved.