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Thermodynamic Driving Force In Ferroelectric Crystals With A Rank-2 Laminated Domain Pattern, And A Study Of Enhanced Electrostriction

机译:具有2级层积畴模式的铁电晶体的热力学驱动力以及增强的电致伸缩研究

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The thermodynamic driving force for domain growth in a rank-2 laminated ferroelectric crystal is derived in this article, and we used it, together with a homogenization theory, to study the issue of enhanced electrostrictive actuation recently reported by Burcsu et al. [2004. Large electrostrictive actuation of barium titanate single crystals. J. Mech. Phys. Solids 52, 823-846]. We derived this force from the reduction of Cibbs free energy with respect to the increase of domain concentration. It is shown that both the free energy and the thermodynamic force consist of three parts: the first arises from the difference in M_0 and M_1, the linear electromechanical compliances of the parent and product domains, respectively, at a given level of applied stress and electric field, the second stems from the electromechanical work associated with the change of spontaneous strain and spontaneous polarization during domain switch, and the third from the internal energy due to the distribution of polarizations strain and electric polarization inside the crystal. We prove that the first term is substantially lower than the second one, and the third one is identically zero with compatible domain pattern. The second one is, however, not exactly equal to the commonly written sum of the products of stress with strain, and electric field with polarization during switch, unless both domains have identical moduli in the common global axes. We also show that, with compatible domain patterns and when M_1 = M_0, this driving force is identical to Eshelby's driving force acting on a flat interface due to the jump of energy-momentum tensor. Applications of the theory to a BaTiO_3 crystal subjected to a fixed axial compression and decreasing electric field from the [001] state reveal that the crystal undergoes a three-stage switching process: (i) the 0→90° switch to form a rank-1 laminate, (ii) the 0→180 switch inside the 0° domain to form a laminate I with a concurrent 90° → -90° switch inside the 90° domain to form laminate 11, creating a rank-2-laminated domain pattern, and (iii) finally the 90→180° switch. It is the exchange of stability between the 0, 90° , and 180° domains under compression and electric field that is the origin of the enhanced actuation. We illustrate these intrinsic features by showing the evolution of these domains, and demonstrate how the reported large actuation strain can be attained with a rank-2 laminate.
机译:本文推导了2级叠层铁电晶体中畴生长的热力学驱动力,并将其与均质化理论一起用于研究Burcsu等人最近报道的增强电致伸缩致动的问题。 [2004年。钛酸钡单晶的大电致伸缩致动。 J.机甲物理固体52,823-846]。我们从相对于域浓度增加的Cibbs自由能的减少中得出了这一力。结果表明,自由能和热力学力都由三个部分组成:第一个部分是由于M_0和M_1的差异,在给定的施加应力和电场水平下,母体和产品域的线性机电顺应性场,第二源于与在域切换期间自发应变和自发极化的变化有关的机电功,第三源于由于晶体内部极化应变和极化的分布而产生的内部能量。我们证明第一项远低于第二项,并且第三项在兼容域模式下为零。但是,第二个不完全等于开关过程中应力与应变和电场与极化的乘积的总和,除非两个域在公共全局轴上具有相同的模量。我们还表明,在兼容的畴模式下,当M_1 = M_0时,由于能量动量张量的跳跃,该驱动力与作用在平面界面上的埃舍尔比的驱动力相同。该理论在BaTiO_3晶体上受到固定的轴向压缩并从[001]状态减小电场的应用表明,该晶体经历了三阶段转换过程:(i)0→90°转换以形成阶跃- 1个层压板,(ii)在0°域内进行0→180转换以形成层压板I,同时在90°域内进行90°→-90°转换以形成层压板11,从而形成等级2层压的畴图案,然后(iii)最后是90→180°开关。压缩和电场作用下0、90°和180°域之间的稳定性交换是增强驱动的起源。我们通过显示这些域的演变来说明这些内在特征,并演示如何使用2级层压板实现所报道的大驱动应变。

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