Abstract:The coupling of magnetic and mechanical fields due to the constitutive behavior of a material is commonly denoted as magnetostrictive effect. The latter is only observed with large coupling coefficients in ferromagnetic materials, where coupling is caused by the rotation of the domains as a result of magnetic (Joule effect) or mechanical (Villari effect) loads. However, only a few elements (e.g. Fe, Ni, Co, and Mn) and their compositions exhibit such a behavior. In this article, the constitutive modeling of no… Show more
“…where σij and Di denote the associated variables mechanical stress and electric displacement. In equations (2) and (3) the material properties of a grain have been assumed constant in incremental changes of state and are determined as weighted averages, see for example, Avakian and Ricoeur (2016) or Huber et al (1999),…”
Section: Constitutive Framework Of a Ferroelectric Grainmentioning
Macroscopic properties of ferroelectrics are controlled by processes on the microscale, in particular the switching of crystal unit cells and the movement of domain walls, respectively. Besides these microscopic levels, the grains of a polycrystalline material constitute the mesoscopic scale. Interactions of grains with statistically distributed orientations, as a consequence of mechanical and electrostatic mismatch, give rise to for example, residual stress which in turn affects domain switching. A multiscale modeling thus has to incorporate at least three interacting scales. In this context, the condensed method has recently been elaborated as an efficient tool with low computational cost and effort of implementation. It is extended toward statistical distributions of grain sizes in a representative material volume element and amended with regard to the modeling of domain evolution. Each of the few parameters of the constitutive approach has a unique physical meaning and is adapted to available experimental values of macroscopic quantities of barium titanate taken from various sources.
“…where σij and Di denote the associated variables mechanical stress and electric displacement. In equations (2) and (3) the material properties of a grain have been assumed constant in incremental changes of state and are determined as weighted averages, see for example, Avakian and Ricoeur (2016) or Huber et al (1999),…”
Section: Constitutive Framework Of a Ferroelectric Grainmentioning
Macroscopic properties of ferroelectrics are controlled by processes on the microscale, in particular the switching of crystal unit cells and the movement of domain walls, respectively. Besides these microscopic levels, the grains of a polycrystalline material constitute the mesoscopic scale. Interactions of grains with statistically distributed orientations, as a consequence of mechanical and electrostatic mismatch, give rise to for example, residual stress which in turn affects domain switching. A multiscale modeling thus has to incorporate at least three interacting scales. In this context, the condensed method has recently been elaborated as an efficient tool with low computational cost and effort of implementation. It is extended toward statistical distributions of grain sizes in a representative material volume element and amended with regard to the modeling of domain evolution. Each of the few parameters of the constitutive approach has a unique physical meaning and is adapted to available experimental values of macroscopic quantities of barium titanate taken from various sources.
“…More specifically, Lu et al [35] established a model by using thermodynamic theory combined with the Eshelby's inclusion theory to study the electric, magnetic and ME properties of the nano-structured multiferroic composites. Avakian et al [36,37] applied the physically motivated constitutive models for ferromagnetic and ferroelectric phases and investigated the ME coupling coefficients in multifunctional composite consisting of a ferromagnetic inclusion in a ferroelectric matrix. Xu et al [38] proposed a new probabilistic domain switching function considering the surface FM anisotropy and the interface chargemediated effect and investigated the size-dependent electric tuning magnetization behaviour for the ME laminates at nanoscale.…”
Section: Introductionmentioning
confidence: 99%
“…In order to simultaneously consider the influence of nonlinear characteristics of ferroelectric materials and ferromagnetic materials on the ME effect for ME composites, some studies have been carried out [35][36][37][38]. More specifically, Lu et al [35] established a model by using thermodynamic theory combined with the Eshelby's inclusion theory to study the electric, magnetic and ME properties of the nano-structured multiferroic composites.…”
In this paper, we develop a theoretical principle to calculate the direct and converse magnetoelectric (ME) coupling response of ferromagnetic/ferroelectric composites with 2–2 connectivity. We first present an experimentally based constitutive equation for Terfenol-D, and then build the mechanism of domain switch for the ferroelectric phase. In the latter, the change of Gibbs free energy, thermodynamic driving force and kinetic equations for domain growth are also established. These two sets of constitutive equations are shown to capture the experimental data of Terfenol-D and PZT, respectively, well. For the direct effect under an applied magnetic field, the induced electric field and the overall ME coupling coefficient are determined. For the converse effect under an applied electric field, the induced magnetization and the excited magnetic field are obtained. Both the induced electric filed under direct effect and the excited magnetic field under converse effect are shown to display the hysteretic characteristics, and also in good agreement with experiments. We conclude that the developed theory can both qualitatively and quantitatively reflect the essential features of nonlinear direct and converse ME coupling of the multiferroic composites.
“…To utilize the full potential of GMM, based on this nonlinear and coupled constitutive model, some extended investigations have been carried out and the coupling behavior of Terfenol-D rods was studied (Sun and Zheng, 2006), In addition, the active vibration control of Terfenol-D rods and laminated composite beams was investigated (Zhou et al, 2006; Zhou and Zhou, 2007). The constitutive model for multiferroic composites based on the nonlinear reversible and irreversible ferromagnetic behaviors was established (Avakian and Ricoeur, 2016).…”
The dynamic model and vibration suppression of a rotating cantilever beam under magnetic excitations are investigated in this article. The nonlinear constitutive relation of magnetostrictive materials is presented. The layout of the control system is demonstrated and explained. The kinetic energy, potential energy of the system, and work done by the electromagnetic force are obtained. The dynamic equations of the system are obtained and discretized by the Hamilton principle and Galerkin approach, respectively. Based on the negative feedback control method, the control scheme is implemented by the magnetostrictive layer. The dynamic model and control method are validated by the references. Various parameter values of the magnetic excitations and rotating beam systems are investigated to reveal their effects on the control behaviors of the bending vibration. Results illustrate that the magnetic excitations bring negative stiffness in the system and increase the responses of beam greatly. The magnetostrictive suppression is effective and can be regarded as the damping effect in the dynamic equations. Increasing the control gain, bias magnetic field and width ratio of the magnetostrictive layer to the controlled layer are beneficial to the vibration control. However, enlarging the angular velocity and pre-stress is harmful to the vibration suppression.
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