The Influence of the Microstructure on the Properties of Ferroelectric Ceramics

Abstract The domain twinning in ferroelectric ceramics is dependent on grain size. In fine grained ceramic a simple lamellar structure allows two- dimensional stress relief, in coarse grained ceramic a banded lamellar structure takes away homogeneous stress in three dimensions. The different domain configurations and internal stresses lead to different dielectric properties and to different hysteresis curves. Inhomogeneous grains of BaTiO3 with some CdBi2Nb2O9 have a core with a normal domain pattern and a shell without domains at room temperature. Core and shell have different transition temperatures. The macroscopic dielectric constant therefore has very high values in a very broad temperature range. Ceramics which are properly prepared in order to have oriented grains exhibit properties which come near to the properties of single crystals.

[1]  G. Arlt,et al.  Theory of the banded domain structure in coarse-grained ferroelectric ceramics , 1992 .

[2]  J. V. Biggers,et al.  Fabrication and electrical properties of grain oriented Bi4Ti3O12 ceramics , 1981 .

[3]  G. Arlt,et al.  Domain configuration and equilibrium size of domains in BaTiO3 ceramics , 1980 .

[4]  W. Schulze,et al.  Grain-oriented fabrication of bismuth titanate ceramics and its electrical properties , 1989, IEEE Transactions on Ultrasonics, Ferroelectrics and Frequency Control.

[5]  Kyoichi Kinoshita,et al.  Grain‐size effects on dielectric properties in barium titanate ceramics , 1976 .

[6]  H. Hagemann Loss mechanisms and domain stabilisation in doped BaTiO3 , 1978 .

[7]  S. E. Koonce,et al.  Effect of Firing Cycle on Structure and Some Dielectric and Piezoelectric Properties of Barium Titanate Ceramics , 1955 .

[8]  G. Arlt,et al.  Aging of fe-doped pzt ceramics and the domain wall contribution to the dielectric constant , 1986 .

[9]  A. J. Burggraaf,et al.  Grain size effects on the ferroelectric-paraelectric transition, the dielectric constant, and the lattice parameters in lanthana-substituted lead titanate , 1974 .

[10]  Toshio Kimura,et al.  Mechanism of Grain Orientation During Hot-Pressing of Bismuth Titanate , 1989 .

[11]  Shaikh,et al.  Dielectric properties of ultrafine grained BaTiO/sub 3/ , 1989, IEEE Transactions on Ultrasonics, Ferroelectrics and Frequency Control.

[12]  W. Buessem,et al.  Phenomenological Theory of High Permittivity in Fine‐Grained Barium Titanate , 1966 .

[13]  L. E. Cross,et al.  The effect of grain size on the permittivity of BaTiO3 , 1984 .

[14]  T. Kanata,et al.  Grain-size effects on dielectric phase transition of BaTiO3 ceramics , 1987 .

[15]  K. Udayakumar,et al.  Thermodynamic Theory of Single-Crystal Lead Titanate with Consideration of Elastic Boundary Conditions , 1990 .

[16]  M. S. Vukasovich,et al.  Ferroelectrics of Ultrafine Particle Size: II, Grain Growth Inhibition Studies , 1966 .

[17]  G. Arlt,et al.  Force constant and effective mass of 90° domain walls in ferroelectric ceramics , 1991 .

[18]  G. Arlt,et al.  Dielectric properties of fine‐grained barium titanate ceramics , 1985 .

[19]  A. Yamaji,et al.  Preparation, Characterization, and Properties of Dy‐Doped Small‐Grained BaTiO3 Ceramics , 1977 .

[20]  G. Arlt,et al.  90°-domain wall relaxation in tetragonally distorted ferroelectric ceramics , 1987 .

[21]  G. Samara Pressure and Temperature Dependences of the Dielectric Properties of the Perovskites BaTi O 3 and SrTi O 3 , 1966 .

[22]  G. Arlt,et al.  Internal stresses and elastic energy in ferroelectric and ferroelastic ceramics: Calculations by the dislocation method , 1991 .