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Electromechanical Interactions

The following is a brief qualitative description of the most important dielectric, electromechanical and piezoelectric relationships, including parameter definitions. For detailed mathematical formulas, solid state physics relationships, methods of parameter determination, etc., please consult the appropriate specialist literature (see recommendations on page 38).

Basic electromechanical equations The following relationships apply only to small electrical and mechanical amplitudes, i.e. small-signal values
Only in this region is it possible for polarized piezoelectric ceramics to be described by linear relationships between the mechanical strain (S) or mechanical stress (T) components and the components of the electric field E or the dielectric displacement D. These linear relationships are derived using dielectric, piezoelectric and elasticity “constants”. Because they depend on the anisotropy of the piezoelectric material, these physical quantities can only be defined in terms of tensors which reflect the directionality of the electric field, the mechanical stresses, etc.
In simplified form, the basic relationships between the electrical and elastic properties (for a static or quasistatic application) can be represented as follows



where:

D dielectric displacement
T mechanical stress
E electric field
S mechanical strain
d piezoelectric charge constant
T permittivity (for T = constant)
sE elasticity constant ( E = constant)

The piezoelectric constants relating the electric field E, the dielectric displacement D, the mechanical stress T and the strain S require directionality indexing. Analogous to crystallographic descriptions for piezo-ferroelectric ceramics, the polarization vector is usually set parallel to the z or 3rd axis of a righthanded Cartesian coordinate system.

The directional parameters are given the subscripts 1,2 and 3 corresponding to the directions of x, y and z,respectively. Mechanical shear stresses (couples) about x, y and z, and the corresponding shear strains, are designated with the subscripts 4, 5 and 6, respectively.

Orthogonal system
to describe piezoelectric materials
Orthogonal system to describe
piezoelectric materials