This paper presents a single-domain boundary element method (BEM) analysis
of fracture mechanics in 2D anisotropic piezoelectric solids. In this analy
sis, the extended displacement (elastic displacement and electrical potenti
al) and extended traction (elastic traction and electrical displacement) in
tegral equations are collocated on the outside boundary (no-crack boundary)
of the problem and on one side of the crack surface, respectively. The Gre
en's functions for the anisotropic piezoelectric solids in an infinite plan
e, a half plane, and two joined dissimilar half-planes are also derived usi
ng the complex variable function method. The extrapolation of the extended
relative crack displacement is employed to calculate the extended 'stress i
ntensity factors' (SIFs), i.e., K-I, K-II, K-III and K-IV. For a finite cra
ck in an infinite anisotropic piezoelectric solid, the extended SIFs obtain
ed with the current numerical formulation were found to be very close to th
e exact solutions. For a central and inclined crack in a finite and anisotr
opic piezoelectric solid, we found that both the coupled and uncoupled (i.e
., the piezoelectric coefficient e(ijk) = 0) cases predict very similar str
ess intensity factors K-I and K-II when a uniform tension sigma(yy) is appl
ied, and very similar electric displacement intensity factor K-IV when a un
iform electrical displacement D-y is applied. However, the relative crack d
isplacement and electrical potential along the crack surface are quite diff
erent for the coupled and uncoupled cases. Furthermore, for a inclined crac
k within a finite domain, we found that while a uniform sigma(yy) (=1N m(-2
)) induces only a very small electrical displacement intensity factor tin t
he unit of Cm-3/2), a uniform D-y (=1 C m(-2)) can produce very large stres
s intensity factors tin the unit of Nm(-3/2)). (C) 1998 Elsevier Science Lt
d. All rights reserved.