Abstract

In piezoelectricity, the stress equations of motion are coupled to the charge equation of electrostatics by means of the linear piezoelectric constitutive equations which contain the piezoelectric constants that couple the small strain to the electric field. In the case of the more general nonlinear interaction of the electric field with a deformable insulator, the Maxwell electrostatic stress tensor must be included in the description. Furthermore, in the nonlinear case, a rotationally invariant combination of the electric field and the deformation occurs in the constitutive equations in place of the electric field for the same reason that the finite train occurs. The linear electroelastic equations for small dynamic fields, superposed on a static bias obtained from the nonlinear system, are more general than the linear piezoelectric equations in that the linear constitutive equations depend on the small local mechanical rotation, as well as the small strain. Nevertheless, when the biasing stress and ele...

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