三种分形和分数阶导数阻尼振动模型的比较研究

标准的整数阶导数方程不能准确描述粘弹性材料的记忆性参考文献[1]和阻尼的分数次幂频率依赖[2],因此分形导数、分数阶导数及正定分数阶导数被用于描述粘弹性介质中的阻尼振动.该文通过分析模型和数值模拟,比较了三种模型描述的振动过程.结果显示,当p小于约O.75或大于约1.9时(p为非整数阶导数的阶数),分形导数模型衰减最快;当P大于约0.75且小于约1.9时,正定分数阶导数模型衰减最快,衰减最慢的分别为分数阶导数模型(p<1)和分形导数模型(p>1).且正定分数阶导数模型衰减快于分数阶导数模型,当p接近2时,两种模型较为相近.     

复杂介质中任意阶频率依赖耗散声波的分数阶导数模型

实验现象表明,声波在复杂介质中传播时,其衰减往往呈现频率的任意次幂律依赖现象.鉴于复杂介质的力学和物理性质的记忆性和长程相关性,频率幂律依赖的声波衰减现象难以用经典的声波方程描述,因为经典的阻尼波方程和近似热黏性波方程只能分别描述与频率无关和频率二次方依赖的声衰减.近年来,带有分数阶导数项的声波方程已被成功用于描述这一声衰减现象.基于课题组对声波衰减分数阶导数建模的研究,对已有的分数阶导数声波方程的研究进展及获得的成果做一个系统的综述,重点讨论这些模型的力学本构、统计力学解释等.简述了软物质中声波传播的时间分数阶导数唯象模型和本构模型,空间分数阶导数唯象模型和本构模型,并深入讨论了各种模型之间的联系与区别:介绍了分数阶导数声波模型在多孔介质中的成功应用,该部分内容涉及了均匀和非均匀多孔介质,刚性固体骨架和可变形固体骨架多孔介质等;通过空间分数阶扩散方程与Levy稳定分布之间的联系,给出了频率幂律依赖指数的变化区间为[0,2]的统计力学解释.最后,讨论了声波传播耗散行为的分数阶导数建模领域仍然存在的问题,并对今后的研究方向进行了探讨和展望.     

分数阶黏弹性Pasternak地基上两端固支Timoshenko梁的动力响应

本文研究了放置在黏弹性Pasternak地基上的Timoshenko梁在移动载荷作用下的动力响应行为．首先,引入分数阶导数,将整数阶标准固体黏弹性地基模型推广为分数阶标准固体黏弹性模型．对于Pasternak地基,考虑压缩层是黏弹性的而剪切层仍是弹性的情况,给出了地基反作用力．然后,求解了Timoshenko梁的自由振动解,获得含黏性耗散信息的复固有频率及振型函数．在此基础上用振型叠加法分析了在移动简谐荷载作用下梁的位移响应．在数值算例中,给出了不同分数阶导数、地基黏性系数以及载荷移动速度下梁的动态响应,讨论了黏弹性地基对梁的动态响应的影响规律．     

Maxwell模型薄板的自由振动

本文利用Ｍａｘｗｅｌ粘弹性模型建立了粘弹性薄板的振动微分方程，给出四边简支粘弹性矩形薄板的固有频率解析解．对粘弹性矩形薄板的振动特性进行了讨论     

一种改进的R-L分数阶导数定义在固体推进剂粘弹性本构模型中的应用

针对Riemann-Liouville分数阶导数定义的不足之处进行了改进,利用改进过的分数阶导数定义,建立了类Kelvin体粘弹性本构模型,并应用于某固体推进剂上,对本构方程中的三个参数进行了求解,与经典的prony级数模型进行比较,采用分数阶导数的类Kelvin体粘弹性本构模型与实验结果能很好地吻合.     

粘弹性地基上含孔隙的石墨烯增强功能梯度板的振动

为分析粘弹性地基上含孔隙的石墨烯增强功能梯度板的自由和强迫振动特性，基于三参数粘弹性地基模型及复合材料薄板理论，建立了粘弹性地基上含孔隙石墨烯增强功能梯度板的运动方程，用伽辽金法求解其固有频率和动力响应，并通过数值算例分析了粘弹性地基参数、孔隙率、孔隙类型及石墨烯纳米片分布模式、含量等因素对自由振动和动力响应的影响．结果表明，固有频率随着孔隙率的增大非单调变化，孔隙率对固有频率的影响随着地基参数、孔隙类型的不同而不同．另外，在三种孔隙类型中，上下表面层含有最少孔隙数量的板的动挠度最小，且其动挠度随着孔隙率的增大而微弱提高．     

文章导读

复杂介质中任意阶频率依赖耗散声波的分数阶导数模型(1265–1280, doi：10.6052/0459-1879-16-186)蔡伟,陈文
　　声波在复杂介质中传播时,其衰减往往表现为频率的幂函数形式.综述了软物质中声波传播的分数阶导数本构模型和唯象模型;讨论了时间和空间分数阶导数黏性耗散声波方程的联系与区别;介绍了频率幂律依赖指数在[0,2]之间变化的统计力学解释;概述了多孔介质中的分数阶导数声波方程。     

上覆分数导数粘弹性场地土地震放大效应

基于一维波动模型和分数导数粘弹性本构关系,分析了在竖直方向上传播的剪切地震波作用下,基岩上分数导数粘弹性模型描述的场地土的横向振动问题,用直接刚度矩阵法求得了场地土的地震放大效应系数,并用数值算例讨论了相关参量对分数导数粘弹性场地土地震放大效应系数的影响。研究结果表明:在简谐剪切地震波作用下,分数导数粘弹性场地土存在共振现象;分数导数的阶数、模型参数和基岩与上覆场地土层底部之间的阻抗比对场地土的地震放大效应系数有较大的影响。     

分数阶导数粘弹性模型的有限元法

在分析分数阶导数三元件模型理论的基础上,把分数阶导数三元件模型引入有限元模型中,推导出具有分数阶导数三元件本构关系的粘弹性结构动力学有限元格式。同时,应用分数阶导数型粘弹性结构动力学方程的数值算法求解了该有限元格式的数值解。并以二维沥青路面结构为例进行了路面动态粘弹性响应分析。算例分析表明,该方法能够正确有效地进行路面动态粘弹性分析。     

粘弹性流体的分数元模型及圆管起动流

分数元模型所描述的非牛顿流体属于复杂粘弹性流体,其应力与应变的分数阶时间导数成正比.本文提出一种用弹簧和油壶连接组成的分形网络结构来比拟分数元模型的应力-应变特性,利用Heaviside运算微积,证明了该分形网络结构对应的粘弹性流体为1/2阶导数的分数元.并证明了构成其他分数阶导数分数元模型需要引入弹簧和油壶的多重分形网络结构.本文还导出了分数元模型的圆管起动流的解析解,研究了分数元模型起动过程振荡特征与该模型导数阶β之间的关系;发现在β≠1的情况下,随时间的进程,圆管内分数元模型的运动最终均将趋于静止,只有β=1的情况是一个例外.     

Investigation of guided waves propagation in orthotropic viscoelastic carbon–epoxy plate by Legendre polynomial method

The effect of viscoelasticity on the guided waves propagation in viscoelastic plate has been investigated according to multi-aspect. To this purpose, an extension of the Legendre polynomial method is proposed to formulate the guided waves equation in orthotropic viscoelastic plate composed of carbon–epoxy. The validity of the proposed Legendre polynomial method is illustrated by comparison with available data. The convergence of the method is discussed through a numerical example. The hysteretic and Kelvin–Voigt viscoelastic models are used to integrate the imaginary part of the complex stiffness matrix associated with the viscoelastic plate in this study. Accordingly, both viscoelastic models do not affect on the dispersion curves results. However, appreciable effects are seen in the attenuation curves. Also, the sensitivity of the guided waves propagation caused by variations of elastic and viscoelastic modulus has been studied in detail. Finally, the advantages of the Legendre polynomial method are described.     

Propagation of flexural waves and localized vibrations in the strip plate with a layer using Hamilton system

Based on the theory of laminated plates and applying the method in Hamiltonian state space, the propagation of flexural waves and vibrations in the strip plate covered with a layer are investigated. The boundaries at the two lateral sides are free of traction. According to the character of solar panel, the existence of all kinds of localized vibration modes and wave propagation modes is analyzed. By using eigenfunction expansion method, the dispersion relations of waveguide modes in the strip plate covered with a layer are derived. Through the numerical examples of solar panel, the existence of all kinds of vibration modes and propagating modes is analyzed. The dispersion curves of the strip plate covered with a layer under different parameters are presented and analyzed. The effects of the properties of the covering layer on the propagation of flexural waves are also examined.     

Viscoelastic shear horizontal wave in graded and layered plates

In this paper, viscoelastic shear horizontal (SH) wave propagation in functionally graded material (FGM) plates and laminated plates are investigated. The controlling differential equation in terms of displacements is deduced based on the Kelvin–Voigt viscoelastic theory. The SH wave characteristics is controlled by two elastic constants and their corresponding viscous coefficients. By the Legendre polynomial series method, the asymptotic solutions are obtained. In order to verify the validity of the method, a homogeneous plate is calculated to make a comparison with available data. Through three different graded plates, the influences of gradient shapes on dispersion and attenuation are discussed. The viscous effects on the displacement and stress shapes are illustrated. The different boundary conditions are analyzed. The influential factors of the viscous effect are analyzed. Finally, two multilayered (two layer and five layer) viscoelastic plates that are composed of the same material volume fraction are calculated to show their differences from the graded plate.     

线性黏弹性球面波的特征线分析

基于ZWT黏弹性本构方程建立了体现高应变率效应的黏弹性球面波的控制方程组,包含5个偏微分方程,解5个未知量v、σr、σθ、εr和εθ。采用特征线法,问题转化为解3族特征线上的5个常微分方程,物理上图像清晰,数学上易于求解。特征线数值分析显示,黏弹性球面波的衰减和弥散效应超过线弹性球面波。球面扩散引起的环向拉应力是导致介质拉伸破坏的主因。进一步还针对强间断黏弹性球面波得出其衰减特性的解析表达式,表明这种更强的衰减特性是几何扩散效应和本构黏性效应两者共同作用的后果。     

Shear wave dispersion and attenuation in periodic systems of alternating solid and viscous fluid layers

The attenuation and dispersion of elastic waves in fluid-saturated rocks due to the viscosity of the pore fluid is investigated using an idealized exactly solvable example of a system of alternating solid and viscous fluid layers. Waves in periodic layered systems at low frequencies are studied using an asymptotic analysis of Rytov’s exact dispersion equations. Since the wavelength of shear waves in fluids (viscous skin depth) is much smaller than the wavelength of shear or compressional waves in solids, the presence of viscous fluid layers necessitates the inclusion of higher terms in the long-wavelength asymptotic expansion. This expansion allows for the derivation of explicit analytical expressions for the attenuation and dispersion of shear waves, with the directions of propagation and of particle motion being in the bedding plane. The attenuation (dispersion) is controlled by the parameter which represents the ratio of Biot’s characteristic frequency to the viscoelastic characteristic frequency. If Biot’s characteristic frequency is small compared with the viscoelastic characteristic frequency, the solution is identical to that derived from an anisotropic version of the Frenkel–Biot theory of poroelasticity. In the opposite case when Biot’s characteristic frequency is greater than the viscoelastic characteristic frequency, the attenuation/dispersion is dominated by the classical viscoelastic absorption due to the shear stiffening effect of the viscous fluid layers. The product of these two characteristic frequencies is equal to the squared resonant frequency of the layered system, times a dimensionless proportionality constant of the order 1. This explains why the visco-elastic and poroelastic mechanisms are usually treated separately in the context of macroscopic (effective medium) theories, as these theories imply that frequency is small compared to the resonant (scattering) frequency of individual pores.     

Stability of a viscoelastic plate in fluid flow

The stability of an infinite viscoelastic plate on an elastic foundation in a viscous incompressible flow is studied. The Navier-Stokes system is linearized for an exponential velocity profile. The problem is reduced by a Fourier-Laplace transform to a system of ordinary differential equations, whose solution is found in the form of convergent series. The roots of the dispersion relation that characterize the stability of the system are found numerically. The effect of the viscosities of the fluid and the plate on the stability of the waves propagating upstream and downstream is studied. The results are compared with available data on the stability of a viscoelastic plate in an ideal fluid flow. __________ Translated from Prikladnaya Mekhanika i Tekhnicheskaya Fizika, Vol. 47, No. 4, pp. 66–74, July–August, 2006.     

Flexural gravity wave motion over poroelastic bed

Using Biot’s consolidation theory, effect of poroelastic bed on flexural gravity wave motion is analyzed in both the cases of single-layer and two-layer fluids. The model for the flexural gravity waves is developed using linear water wave theory and small amplitude structural response in finite water depth. The effects of permeability and shear modulus of poroelastic bed and time period on flexural gravity wave motion are studied by analyzing the dispersion relation, phase speed, plate deflection, interface elevation and pressure distribution along water depth. Various results for surface gravity waves are analyzed as special cases. The study reveals that bed permeability retards the hydrodynamic pressure distribution along the water depth significantly compared to shear modulus whilst, floating plate deflection decreases significantly with change in shear modulus compared to permeability of the poroelastic bed. The present study can be generalized to analyze various wave–structure interaction problems over poroelastic bed.     

Some problems of stability of propagation of non-linear waves in shells and plates

In the present paper equations of modulations taking into account the second order derivatives of amplitude and stability conditions are obtained. The general results are applied to the stability problems of propagation of quasimonochromatic waves in plates, shells, plates in contact with fluid, shells containing fluid, plate in magnetic field, tree-layered plate and viscoelastic plate.     

A dynamic investigation of fiber-reinforced viscoelastic materials

In recent years, several mathematical models have been proposed to describe the quasi-static response of fiber-reinforced materials, consisting of continuous, elastic fibers embedded in a linear viscoelastic matrix. By assuming that geometric dispersion (dispersion resulting from the internal geometry of the material) is small in comparison to viscoelastic dispersion (dispersion resulting from the viscoelastic nature of the material), these proposed constitutive equations can be extended from a quasi-static regime to a dynamic regime. Here, we examine how the extension to the dynamic regime may be accomplished, compare the results with a theoretical model that includes geometric dispersion, and use the results of an experimental program to evaluate the models. In general, the quasi-static constitutive equations predict phase velocities that are larger than that predicted by the model which contains geometric dispersion and attenuation coefficients that are lower; and, the experimental results agree with the theoretical predictions, provided the fibers were spread more or less uniformly over the cross section.