In this paper, a recently proposed method by E. Pan and F.G. Yuan (Int. J.
Solids Struct., 2000) for the calculation of the elastic bimaterial Green's
functions is extended to the analysis of three-dimensional Green's functio
ns for anisotropic piezoelectric bimaterials. The method is based on the St
roh formalism and two-dimensional Fourier transforms in combination with Mi
ndlin's superposition method. We first derive Green's functions in exact fo
rm in the Fourier transform domain. When inverting the Fourier transform, a
polar coordinate transform is introduced so that the radial integral from
0 to +infinity can be carried out exactly. Therefore, the bimaterial Green'
s functions in the physical domain are derived as a sum of a full-space Gre
en's function and a complementary part. While the full-space Green's functi
on is in an explicit form, as derived recently by E, Pan and F. Tonon (Int.
J. Solids Struct., 37 (2000): 943-958), the complementary part is expresse
d in terms of simple regular line integrals over [0, 2 pi] that are suitabl
e for standard numerical integration. Furthermore, the present bimaterial G
reen's functions can be reduced to the special cases such as half-space, su
rface, interfacial, and full-space Green's functions, Uncoupled solutions f
or the purely elastic and purely electric case can also be simply obtained
by setting the piezoelectric coefficients equal to zero. Numerical examples
for Green's functions are given for both half-space and bimaterial cases w
ith transversely isotropic and anisotropic material properties to verify th
e applicability of the technique. Certain interesting features associated w
ith these Green's functions are observed and discussed, as related to the s
elected material properties. (C) 2000 Elsevier Science Ltd. All rights rese
rved.