首页> 外文期刊>International journal of non-linear mechanics >A constitutive law for dielectric elastomers subject to high levels of stretch during combined electrostatic and mechanical loading: Elastomer stiffening and deformation dependent dielectric permittivity
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A constitutive law for dielectric elastomers subject to high levels of stretch during combined electrostatic and mechanical loading: Elastomer stiffening and deformation dependent dielectric permittivity

机译:介电弹性体的本构定律在静电和机械载荷共同作用下承受高水平的拉伸:弹性体的硬化和变形取决于介电常数

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We construct a constitutive law for the response of dielectric elastomers subject to high levels of stretch during combined electrostatic and mechanical loading. The constitutive law is based on a statistical mechanics analysis of a freely jointed chain, due to Kuhn and Grun [1-3], that relates the force of extension and polarizability anisotropy of a polymer chain to its fractional extension, rl, through the inverse Langevin function. We utilize a Pade [4] approximant that accurately represents the inverse Langevin function through the entire range of fractional extensions. Thereafter, we cast this machinery into the 8-chain lattice [5,6] and model an elastomer as a heavily interpenetrated network of 8-chain lattices. We assume that the motions of each lattice are affine with the overall deformation of the elastomer. In this fashion, the fractional extension of each chain, rl, is linked to the stretch ratios. With such an approach, we obtain a materially objective free energy density and an expression for the dielectric permittivity of the elastomer that depends on the current state of deformation and the overall stretch level. The elastic free energy density depends on two parameters, the small deformation shear modulus and the chain extensibility limit. We observe that the present model and the well established Arruda and Boyce [5], Gent [7], and neoHookean models are all special cases of the eight chain model of the elastic free energy density presented in this work. The isotropic part of the dielectric permittivity and the electrostrictive coefficient depend on the dilatation. The dielectric permittivity remains isotropic under a pure dilatation, but otherwise becomes anisotropic during deformation. The form of the permittivity resembles that of the deformation dependent permittivity presented by Jimenez and McMeeking [8]. However, in the model presented in this work, the electrostrictive coefficient is not only affected by dilatation but also becomes a function of the current level of deformation through the first invariant of the left Green-Cauchy tensor. We utilize the free energy density of the dielectric elastomer to compute the response of a thin film actuator subject to electrostatic and mechanical loading. In this model, the actuator is allowed to have different levels of in-plane limit stretch, and the through thickness permittivity is allowed to increase or decrease with in-plane extension of the actuator. We establish a parameter space map, extensibility limit versus electrostrictive coefficient of the elastomer, for which our constitutive law is relevant to the behavior of dielectric elastomers. With this approach, we study the actuation, electric charge storage, and stability characteristics of the actuator. From the results of our calculations we clearly identify two types of actuator behavior: actuators that exhibit electromechanical instability (type A), and actuators that do not exhibit this instability (type B). We establish that type A actuators develop hysteresis loops in a similar Manner to those identified by Zhao, Hong and Suo [9] and Jimenez and McMeeking [8], for dielectric elastomers with constant isotropic permittivity that stiffen during straining, in the case of the former, and for dielectric elastomers that do not stiffen but exhibit a through thickness permittivity that increases/decreases with straining, in the case of the latter.
机译:我们构造了本构定律,用于介电弹性体在静电和机械载荷联合作用下承受高水平拉伸的响应。本构律基于对自由连接链的统计力学分析(由于Kuhn和Grun [1-3]),该分析将聚合物链的延伸力和极化率各向异性与聚合物链的分数延伸率r / nl通过Langevin逆函数。我们利用Pade [4]近似值,在整个分数扩展范围内准确表示逆Langevin函数。此后,我们将此机械浇铸成8链格[5,6],并将弹性体建模为8链格的高度互穿网络。我们假设每个晶格的运动都与弹性体的整体变形有关。以这种方式,每个链的分数延伸r / nl与拉伸比相关。通过这种方法,我们获得了材料上客观的自由能密度,以及弹性体的介电常数的表达式,该表达式取决于当前的变形状态和整体拉伸水平。弹性自由能密度取决于两个参数,小的变形剪切模量和链的延伸极限。我们观察到,当前模型以及建立良好的Arruda和Boyce [5],Gent [7]和neoHookean模型都是本工作中提出的弹性自由能密度八链模型的特例。介电常数和电致伸缩系数的各向同性部分取决于膨胀。介电常数在纯膨胀下保持各向同性,但在变形过程中变为各向异性。介电常数的形式类似于Jimenez和McMeeking [8]提出的与变形有关的介电常数。但是,在这项工作中提出的模型中,电致伸缩系数不仅受扩张影响,而且还成为通过左Green-Cauchy张量的第一不变量的当前变形水平的函数。我们利用介电弹性体的自由能密度来计算薄膜致动器在静电和机械载荷作用下的响应。在该模型中,允许执行器具有不同水平的平面内极限拉伸,并且允许贯穿厚度的介电常数随着执行器的平面内延伸而增加或减小。我们建立了一个参数空间图,弹性体的延伸极限与电致伸缩系数,我们的本构定律与介电弹性体的性能有关。通过这种方法,我们研究了致动器的致动,电荷存储和稳定性特征。从我们的计算结果中,我们清楚地确定了两种类型的执行器行为:表现出机电不稳定的执行器(A型)和没有表现出这种不稳定的执行器(B型)。我们确定,对于具有恒定各向同性介电常数的介电弹性体,在应变过程中变硬的情况下,A型执行器会以类似于Zhao,Hong和Suo [9]和Jimenez和McMeeking [8]所确定的方式形成磁滞回线。对于前者,对于介电弹性体,它们不变硬,但表现出贯穿厚度的介电常数,在应变的情况下,该介电弹性体随应变而增加/减小。

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