1993
DOI: 10.1177/1045389x9300400303
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A Macroscopic Phenomenological Formulation for Coupled Electromechanical Effects in Piezoelectricity

Abstract: A phenomenological formulation of polarization reversal of piezoelectric materials s proposed based on the dynamics of domain switching. This formulation provides a method to describe the hysteresis in piezoelectricity as well as in electromagnetics. It is shown that a good approach to describe the nonlinear induced strain-field behavior and electromechanical hysteresis in piezoelectricity is by combining the macroscopic phenomenological aspects with the microscopic naterial properties. A one-dimensional therm… Show more

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Cited by 50 publications
(21 citation statements)
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“…The saturation behavior of the Ising relation has also motivated its use in phenomenological models. Translates of the form P = P s tanh(E ± E c ) were employed by Zhang and Rogers [39], and r(x) = tanh(x) provides a suitable choice for the ridge functions employed in generalized Preisach, or Krasnolselskii-Pokrovskii, characterizations [2,3]. The model presented here differs in that it focuses on an energy formulation for domain processes.…”
Section: Asymptotic Polarization Relation In Absence Of Thermal Activmentioning
confidence: 99%
“…The saturation behavior of the Ising relation has also motivated its use in phenomenological models. Translates of the form P = P s tanh(E ± E c ) were employed by Zhang and Rogers [39], and r(x) = tanh(x) provides a suitable choice for the ridge functions employed in generalized Preisach, or Krasnolselskii-Pokrovskii, characterizations [2,3]. The model presented here differs in that it focuses on an energy formulation for domain processes.…”
Section: Asymptotic Polarization Relation In Absence Of Thermal Activmentioning
confidence: 99%
“…We note that (17) is exactly the Ising relation employed in [108] when quantifying the anhysteretic polarization and is equivalent through first-order terms with the Langevin relations employed in various ferroelectric and ferromagnetic models. Translates of the form P = P s tanh(E ± E c ) were also employed by Zhang and Rogers [123], and ridge functions of the form r(x) = tanh(x) are appropriate for generalized Preisach, or Krasnosel'skiǐ-Pokrovskiǐ characterizations [8,9,60]. The relation resulting from (5) is slightly more complicated due to the piecewise nature of the definition.…”
Section: Asymptotic Polarization Relations In the Absence Of Thermal mentioning
confidence: 99%
“…Furthermore, all the potential sites for the spontaneous polarization in the crystallite are orthogonal, the gradient of the resultant displacement from switching is a diagonal, uji = u1511 , and is equal to the strain tensor, as given by (2). Thus the work done by the external load in switching the polarization from any initial state to any final state is given by,…”
Section: Idealized Single Crystal Modelmentioning
confidence: 98%
“…The electrical displacement produced during switching is given by (2). Furthermore, all the potential sites for the spontaneous polarization in the crystallite are orthogonal, the gradient of the resultant displacement from switching is a diagonal, uji = u1511 , and is equal to the strain tensor, as given by (2).…”
Section: Idealized Single Crystal Modelmentioning
confidence: 99%