1999
DOI: 10.1016/s0020-7683(98)00040-7
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Phenomenological modeling of the non-linear electro-mechanical coupling in ferroelectrics

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Cited by 221 publications
(185 citation statements)
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“…The dielectric behavior is thereby described with the help of a hyperbolic function. Another phenomenological model for ferroelectric materials has been advocated by Kamlah and Tsakmakis [23] which is straightforwardly based on the introduction of reasonable internal variables. The constitutive behavior is governed by appropriate ordinary differential equations capturing the history dependence of the material.…”
Section: Introductionmentioning
confidence: 99%
“…The dielectric behavior is thereby described with the help of a hyperbolic function. Another phenomenological model for ferroelectric materials has been advocated by Kamlah and Tsakmakis [23] which is straightforwardly based on the introduction of reasonable internal variables. The constitutive behavior is governed by appropriate ordinary differential equations capturing the history dependence of the material.…”
Section: Introductionmentioning
confidence: 99%
“…A representative set of state variables is thereby adopted and incorporated into essential expressions and functions such as the free energy. Further constitutive relations and evolution equations are then established by taking fundamental thermodynamic considerations into account; see for instance Lynch and McMeeking (1994), Kamlah and Tsakmakis (1999), Landis (2002) or Schröder and Romanowski (2005). When setting up such phenomenologically motivated theories, one generally has the choice whether to fix material properties or to allow the material properties to change during the deformation process.…”
Section: Introductionmentioning
confidence: 99%
“…In order to simulate the characteristic polarization and mechanical butterfly hysteresis loops for ferroelectric solids, we employ a three-dimensional Preisach model. In detail, we decompose the dielectric displacement and mechanical deformations into a linear reversible and a non-linear irreversible part, see [4]. The irreversible part of the dielectric displacement, which describes the remanent polarization of the material, is approximated with a Preisach operator, see [2,3,[6][7][8].…”
Section: Introductionmentioning
confidence: 99%