Optimization of crystal microstructure in piezoelectric ceramics by multiscale finite element analysis
Introduction
Advanced piezoelectric ceramics, such as perovskite compounds with a tetragonal crystal structure, are used as actuators in various electronic and mechanical devices. As new micro- and nanotechnologies begin to incorporate such actuators, the performance requirements of piezoelectric ceramics will become more demanding. Piezoelectric ceramics are polycrystalline materials consisting of randomly orientated crystals. The non-symmetric crystal structure induces spontaneous polarization in the [0 0 1] direction and produces strongly anisotropic mechanical and electrical behavior on the crystal scale. There is thus substantial scope for improving the macroscopic piezoelectric response through the microscopic design of the crystal orientation and morphology. Highly oriented thin piezoelectric films have been successfully fabricated by epitaxial growth techniques. For example, [0 0 1]-oriented thin film on a (1 0 0)SrRuO3/(1 0 0)SrTiO3 substrate has been fabricated by metalorganic chemical vapor deposition [1], and [1 1 1]-oriented thin film on Si(1 0 0) has been fabricated by radiofrequency magnetron sputtering [2]. These films exhibit superior piezoelectric performance due to control of crystal morphology. However, most of the highly oriented piezoelectric thin films fabricated to date are designed on the basis of single-crystals with uniform orientation. An alternative method for improving the macroscopic piezoelectric response is to optimize the microstructure by considering the heterogeneous orientation of crystals in a polycrystalline aggregate.
In the present study, a method for optimizing the heterogeneous orientation of crystals in polycrystalline piezoelectric ceramics so as to maximize the macroscopic piezoelectric response is proposed based on a multiscale finite element analysis [3], [4], [5], [6]. The microstructural crystal orientations are employed as design parameters, and the homogenized piezoelectric strain constants of the macrostructure – the dominant factors governing piezoelectric actuation – are adopted as the objective function. Using this analysis scheme, computations are performed for barium titanate (BaTiO3) and lead titanate (PbTiO3) as representative examples of piezoelectric ceramics. The mechanism by which the optimized microstructure maximizes the macroscopic piezoelectric response is discussed in terms of the orientational dependence of piezoelectricity.
Section snippets
Multiscale finite element method
Consider a polycrystalline piezoelectric material composed of many non-uniformly oriented crystal grains. The macroscopic polycrystalline electromechanical characteristics are governed by the microscopic crystal morphology, and it can usually be assumed that the overall macroscopic structure is formed locally by the spatial repetition of very small microstructures. In other words, it can be assumed that the material properties are periodic functions of microscopic variables. The coupled field
Orientation dependence of BaTiO3 crystal grains
The characteristics of crystal grains in the microstructure are examined here using the material properties of a BaTiO3 single crystal [9]. The dependence of the piezoelectric strain constants microd333 and microd311 on the orientation of crystals for single-crystal BaTiO3 is shown in Fig. 4. These values were computed by tensor transformation for Euler angles ϕ of 0–180° with θ = 0° and ψ = 45°. The piezoelectric strain constant is defined in the microscopic coordinate system, and the Euler angle ϕ
Orientation dependence of PbTiO3 crystals
Fig. 14 shows the orientation dependence of the piezoelectric strain constants microd333 and microd311 for single-crystal PbTiO3 [11]. The maximum values of these constants, microd333 = 156.73 pC N−1 and microd311 = −25.40 pC N−1, are obtained at a Euler angle ϕ of 0°, corresponding to the [0 0 1] direction under spontaneous polarization. As single-crystal PbTiO3 has smaller crystald131 and crystald223 values than single-crystal BaTiO3, the shearing strain due to crystald131 and crystald223 under an
Conclusion
A scheme for maximizing the macroscopic piezoelectric strain constants macrod333 and macrod311 of polycrystalline piezoelectric ceramics based on a multiscale finite element method was presented. Analysis using this scheme revealed that a piezoelectric strain constant higher than that for single-crystal can be realized in a polycrystalline structure consisting of [1 1 1]-oriented crystals. Two structures achieve this enhanced behavior: an ordered layer structure consisting of 120°-rotated layers,
Acknowledgements
The authors thank Professor Eiji Nakamachi of Doshisha University for helpful discussions and comments. Y.U. was financially supported by a Grant-in-Aid for Young Scientists (B) (No. 17760095) from the Ministry of Education, Culture, Sports, Science and Technology of Japan.
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