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首页> 外文期刊>Latin American Journal of Solids and Structures >Analytical solution for nonlinear dynamic behavior of viscoelastic nano-plates modeled by consistent couple stress theory
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Analytical solution for nonlinear dynamic behavior of viscoelastic nano-plates modeled by consistent couple stress theory

机译:一致耦合应力理论建模的粘弹性纳米板非线性动力学行为的解析解

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This paper analyses the non-stationary free vibration and nonlinear dynamic behavior of the viscoelastic nano-plates. For this purpose, a size-dependent theory is developed in the framework of the consistent couple stress theory for viscoelastic materials. The previously presented modified couple stress theory was based on some consideration making it partially doubtful to apply. This paper uses the recent findings for the mentioned problem and develops it to analyze the nonlinear dynamic behavior of nano-plates with nonlinear viscoelasticity. The material is supposed to follow the Leaderman integral nonlinear constitutive relation. In order to capture the geometrical nonlinearity, the von-Karman strain displacement relation is used. The viscous parts of the size-independent and size-dependent stress tensors are calculated in the framework of the Leaderman integral and the resultant virtual work terms are obtained. The governing equations of motion are derived using the Hamilton principle in the form of the nonlinear second order integro-partial differential equation with coupled terms. These coupled size-dependent viscoelastic equations are solved using the forth-order Runge-kutta and Harmonic balance method after simplifying by the expansion theory. The short-time Fourier transform is performed to examine the system free vibration. In addition, frequency- and force-responses of the nanosystem subjected to distribute harmonic load are presented. The obtained results show that the viscoelastic model-based vibration is non-stationary unlike the elastic model. Moreover, the damping mechanism of the viscoelasticity is amplitude dependent and the contribution of the viscoelastic damping terms at higher forcing conditions becomes noticeable.
机译:本文分析了粘弹性纳米板的非稳态自由振动和非线性动力学行为。为此,在粘弹性材料的一致偶应力理论的框架内发展了尺寸相关理论。先前提出的修改后的偶应力理论是基于某种考虑而使其应用存在部分疑问的。本文利用上述问题的最新发现,并将其发展为分析具有非线性粘弹性的纳米板的非线性动力学行为。该材料应遵循Leaderman积分非线性本构关系。为了捕获几何非线性,使用了von-Karman应变位移关系。在Leaderman积分的框架中,计算了与尺寸无关和与尺寸有关的应力张量的粘性部分,并获得了虚拟工作项。使用汉密尔顿原理,以带有耦合项的非线性二阶积分偏微分方程的形式导出运动的控制方程。通过扩展理论简化后,使用四阶Runge-kutta和Harmonic平衡法求解这些耦合的尺寸相关粘弹性方程。执行短时傅立叶变换以检查系统的自由振动。另外,提出了承受谐波负载的纳米系统的频率响应和力响应。所得结果表明,与弹性模型不同,基于粘弹性模型的振动是非平稳的。而且,粘弹性的阻尼机制是振幅相关的,并且在较高的强迫条件下粘弹性阻尼项的贡献变得明显。

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