Two extreme approximations, namely the Voigt-and Reuss-type approximations, have been used to estimate the e ective electrostrictive coe cients of isotropic or anisotropic (as in the dc electric-® eld-biased piezoelectric mode) relaxor-based ferroelectric ceramics. It is shown that, for a dense ceramic with cubic crystallites, both simple approximations give very similar results and can be used for such estimates. However, for common ceramics containing pores, the Voigt and Reuss approximations yield only extreme upper and lower bounds respectively, and a more appropriate approach is needed.Recently relaxor ferroelectric ceramics from the PbMg 1=3 Nb 2=3 O 3 (PMN)± PbTiO 3 (PT) family have received much attention because of their comparatively large electrostriction and very small hysteresis (Cross 1987, Sundar and Newnham 1992, Zhao et al. 1995, Blue et al. 1997, Zhang and Zhao 1997. Their strong potential for application in electroactive sensor and actuator devices has motivated a large and new research activity in the electrostriction e ectÐ a nonlinearly coupled mechanical± electric e ect existing in all dielectric materials. As most of the experimental research is on electrostrictive ceramics, it is highly desirable to relate the electrostrictive properties to the single-crystal properties and texture of the ceramics. Although several successful approaches have been developed to link the e ective properties with the microstructure of ceramics, resulting in many expressions for calculating the e ective properties (for example Nan (1993) ), there are no theoretical expressions for the electrostriction, owing to the complexity of this nonlinear coupled mechanical± electric e ect.An exact derivation of the electrostrictive properties of a polycrystalline ceramic is apparently not possible (Nan and Weng 2000), as the electrostrictive strains developed in neighbouring crystallites are normally incompatible because of their mutual misorientation. By analogy to the elastic moduli of polycrystals, Devonshire (1951) calculated the electrostrictive coe cients Q i j of an isotropic ceramic by directly averaging the coe cients for randomly oriented cubic crystallites. This was the