The propagation of piezoelectric waves in an anisotropic inhomogeneous linear piezoelectric body is studied. A singular (smooth) surface or discontinuity surface of order r in the displacement and electrical fields is referred to as a weak (piezoelectric) wave if r ≥ 2 and a strong (piezoelectric) wave if r = 0, 1. It is shown that the local propagation condition for weak waves of any given order and for strong waves of order 1 can be expressed in terms of an acoustic tensor, which does not depend on r and coincides with the tensor used for plane progressive waves in the homogeneous case [see A. C. Eringen and G. A. Maugin, Electrodynamics of continua. I, Springer, New York, 1990; MR1031714 (90k:73001)(p. 488)]. For any r ≥ 1 singular hypersurfaces are characteristic for the linear piezoelectric system, whereas for r = 0 singular hypersurfaces may be non-characteristic for such equations. A condition is written which characterizes the strong waves of order 0 that are characteristic. For the latter waves the afore-mentioned acoustic tensor can be used to express the local propagation condition.

On discontinuity waves in linear piezoelectricity

MONTANARO, ADRIANO
2001

Abstract

The propagation of piezoelectric waves in an anisotropic inhomogeneous linear piezoelectric body is studied. A singular (smooth) surface or discontinuity surface of order r in the displacement and electrical fields is referred to as a weak (piezoelectric) wave if r ≥ 2 and a strong (piezoelectric) wave if r = 0, 1. It is shown that the local propagation condition for weak waves of any given order and for strong waves of order 1 can be expressed in terms of an acoustic tensor, which does not depend on r and coincides with the tensor used for plane progressive waves in the homogeneous case [see A. C. Eringen and G. A. Maugin, Electrodynamics of continua. I, Springer, New York, 1990; MR1031714 (90k:73001)(p. 488)]. For any r ≥ 1 singular hypersurfaces are characteristic for the linear piezoelectric system, whereas for r = 0 singular hypersurfaces may be non-characteristic for such equations. A condition is written which characterizes the strong waves of order 0 that are characteristic. For the latter waves the afore-mentioned acoustic tensor can be used to express the local propagation condition.
2001
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Utilizza questo identificativo per citare o creare un link a questo documento: https://hdl.handle.net/11577/1354472
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