聚合物熔体粘弹性本构方程

概述了聚合物熔体粘弹性本构方程的发展历程，给出了有代表性的线性粘弹性和非线性粘弹性本构方程的各种形式的数学表达式，讨论了它们的特点及应用范围，旨在为聚合物熔体流动数值模拟中本构方程的选择提供帮助。     

低速冲击下短纤维复合材料本构方程研究

借助ZWT非线性粘弹性一维本构关系,导出了常应变率条件下,热固性聚合物不含时间变量和积分项的、简化的、三次多项式型本构方程;采用细观力学方法,将建立在线弹性理论之上的Eshelby等效包容体理论推广应用于非线性弹性问题.在上述工作基础之上,结合应变率影响,提出了低速冲击下随机分布短纤维复合材料的一维率相关本构方程;把方程预测结果与实验结果对比,发现吻合很好,因而初步验证了所提本构方程的可靠性.     

弹性损伤理论的几何-拓扑描述

材料内部微观几何缺陷通常是作为物理非线性问题在本构方程中考虑。针对连续介质弹性损伤理论作几何拓扑,采用非完整标架方法把材料内部微观几何缺陷转化为材料空间的弯曲,并体现在基本几何法则中。首先由连续损伤变量定义拟塑性张量,给出这些基本张量所满足的连续性方程和基本几何法则。由此建立了弹性损伤缺陷与Riemann流形的对应关系,将物理非线性问题转化为物理线性和材料所在空间的弯曲之和。最后讨论了二维情况下,各向同性晶格材料受各向异性损伤的算例。     

基于不可逆内变量热力学的岩石材料粘弹-粘塑性本构方程

岩石材料的粘弹性和粘塑性变形是与时间相关的能量耗散行为。在Rice不可逆内变量热力学框架下,引入两组内变量分别用来描述在粘弹性和粘塑性变形过程中材料的内部结构调整。通过给定比余能的具体形式和内变量的演化方程,推导出内变量粘弹-粘塑性本构方程。粘弹性本构方程具有普遍性,能涵盖Kelvin-Voigt和Poynting-Thomson在内的经典粘弹性模型的本构方程。并指出热力学力与应力呈线性关系是组合元件模型为线性模型的根本原因。粘塑性本构方程能较好地刻画岩石材料在粘塑性变形过程中的硬化现象。对模拟岩石的模型相似材料进行单轴加卸载蠕变试验,将蠕变过程中的粘弹性和粘塑性变形分离并根据试验数据对本构方程的材料参数进行辨识。试验数据和理论曲线对比结果表明该文提出的本构方程能很好地模拟材料的蠕变行为。该类型的本构方程能为岩石工程的长期稳定性的预测、评价以及加固分析提供基础。     

轴向运动粘弹性弦线的横向非线性动力学行为

采用Poincaré映射和分岔图分析轴向运动黏弹性弦线横向振动的非线性动力学行为。考虑由积分型本构关系描述的黏弹性弦线,并计及微小但有限的变形导致的几何非线性,建立了系统的控制方程。应用Galerkin方法将系统控制方程截断,并通过引入辅助变量将截断后的方程转化为便于数值积分的形式。计算了弦线中点Poincaré映射对轴向张力涨落幅值、轴向运动速度、黏弹性系数和黏弹性指数的分岔图。     

刚／粘塑性梁的强迫振动

本文依据粘塑性梁强迫振动的非齐次方程与非线性本构方程,提出采用分离变量的位移方法求解,获得该问题的应力和位移解.     

复合固体推进剂黏弹性微裂纹损伤本构模型

为建立复合固体推进剂的损伤本构模型,在介观尺度上视其为微裂纹损伤,选取微裂纹密度为损伤内变量。在Abdel-Tawab本构方程的基础上,基于微裂纹均匀化理论,推导了损伤映射张量的一般形式。该张量通常具有非完全对称性,其物理意义是将真实应力空间中各向异性材料的多轴加载映射为等效应力空间中各向同性材料的更为复杂的多轴加载。其次,基于黏弹性动态裂纹扩展模型和裂纹扩展阻力曲线的概念,建立了损伤内变量的演化方程。该演化方程仅含4个物理意义明确的细观参数,并且参数的取值规律与宏观应力曲线的变化规律相一致。数值结果表明,建立的模型能够有效反映材料损伤的应变率、温度依赖性及各向异性特征,并且具有一定的蠕变损伤预测能力。     

层状裂隙岩体弹塑性损伤断裂模型与岩质高边坡稳定分析

本文研究了层状裂隙岩体的弹塑性损伤断裂模型。文中按岩体等效柔度张量定义损伤张量,并对层状裂隙岩质高边坡的变形破坏过程建立了损伤演化方程,提出了包含软弱薄层塑性滑移与裂隙损伤扩展耦合性态的本构关系。最后将其应用于某水电站左坝肩高边坡开挖形成过程的稳定性分析中。     

混凝土坝地震动力损伤分析

基于塑性损伤本构理论,将损伤变量作为内变量,在Drucker-Prager本构模型中引入损伤变量,考虑材料损伤引起的材料劲度的退化,基于非关联流动法则计算材料的塑性应变,根据材料的有效塑性应变计算损伤量,考虑到张开裂缝闭合时材料弹性劲度的恢复,推导了考虑塑性损伤的混凝土动态本构关系,并给出了内变量的计算步骤和动力方程的迭代格式。最后利用建立的动态本构模型对Koyna重力坝进行了非线性地震响应时程分析,并给出了关键时刻坝体最大受拉损伤分布,结果表明在坝颈和坝基处出现了较大的损伤,坝颈处的损伤最终形成由下游向上游的开裂破坏,这与该坝的实际震害较为一致。     

纵向振动粘弹性桩的分叉和混沌运动

研究了轴向周期载荷作用下非线性粘弹性嵌岩桩纵向振动的混沌运动。假定桩和土体分别满足Leaderman非线性粘弹性本构关系和线性粘弹性本构关系,得到的运动方程为非线性积分-偏微分方程;利用Galerkin方法将方程简化,并进行了数值计算。数值结果表明纵向振动的非线性粘弹性桩可以通过准周期分叉的方式进入混沌运动。     

A model for anisotropic viscoelastic damage in composites

A model for continuous damage combined with viscoelasticity is proposed. The starting point is the formulation connecting the elastic properties to the tensor of damage variables. A hardening law associated with the damage process is identified from available experimental information and the rate-type constitutive equations are derived. This elastic damage formulation is used to formulate an internal variable approximation to viscoelastic damage in the form of a non-linear Kelvin chain. Elastic and viscoelastic equations are implemented into a finite element procedure. The code is verified by comparison with closed-form solutions in simplified configurations, and validated by fitting results of experimental creep tests.     

Thin shells with finite rotations formulated in biot stresses: Theory and finite element formulation

A bending theory for thin shells undergoing finite rotations is presented, and its associated finite element model is described. The kinematic assumption is based on a shear elastic Reissner-Mindlin theory. The starting point for the derivation of the strain measures are the resultant equilibrium equations and the associated principle of virtual work. Within this formulation the polar decomposition of the shell material deformation gradient leads to symmetric strain measures. The associated work-conjugate stress resultants and stress couples are integrals of the Biot stress tensor. This tensor is invariant with respect to rigid body motions and, therefore, appropriate for the formulation of constitutive equations. Finite rotations are introduced via Eulerian angles. The finite element discretization of arbitrary shells is based on the isoparametric concept formulated with respect to a plane reference configuration. The numerical model is applied to different non-linear plate and shell problems and compared with existing formulations. Due to a consistent linearization, the step size of a load increment is only limited by the local convergence behaviour of Newton's method.     

Nonlocal effect on the free vibration of short nanotubes embedded in an elastic medium

In this paper, the small size effect on the free vibration behavior of finite length nanotubes embedded in an elastic medium is investigated. The problem is formulated based on the three-dimensional (3D) nonlocal elasticity theory. Since the 3D nonlocal constitutive relations in a cylindrical coordinate system are used, in addition to displacement components, the stress tensor components are chosen as degrees of freedom. The surrounding elastic medium is modeled as the Winkler’s elastic foundation. The differential quadrature method as an efficient and accurate numerical tool in conjunction with the series solution is used to discretize the governing equations. Very fast rate of convergence of the method is demonstrated. The effects of the nonlocal parameter together with the other geometrical parameters and also the stiffness parameter of the elastic medium on the natural frequencies are studied.     

Limitations of the constitutive equation of a simple elastic solid

Summary The constitutive equation of a simple, isotropic elastic solid can be arranged in such a form as to give rise to a fundamental identity between Lode's stress parameter and a corresponding deformation parameter. Using the concept of a stress intensity function, it is shown that at initial yield the constitutive equation of a simple, isotropic elastic solid satisfies only the von Mises yield criterion. A general form for the deformation response coefficients is obtained by way of the concept of a deformation intensity function. In general, there are two broad classes of deformation intensity function, defined in terms of whether the deformation intensity function is continuously differentiable or whether it is piece-wise linear and continuous. Use of the fundamental identity between Lode's stress parameter and the corresponding deformation parameter leads to the conclusion that the constitutive equation of the simple, isotropic elastic solid is incompatible with any form of piece-wise linear deformation intensity function. The stretching tensor has been expressed in terms of the co-rotational and convected time derivatives of the left Cauchy-Green deformation tensor and its inverse. This form of the stretching tensor is entered into a particular form of constitutive equation of the rate-type for a simple, isotropic elastic solid. By considering infinitesimal deformations from an arbitrary configuration, the constitutive equation of the rate-type is reduced to a constitutive equation of the incremental-type. In a similar way, an incremental-type constitutive equation is obtained from the constitutive equation of a simple, isotropic elastic solid. Comparison of these two incremental-type constitutive equations leads to the identification of a particular form for the material response coefficients associated with the constitutive equation of a simple elastic solid. Further limitations of the constitutive equation of a simple, isotropic elastic solid are considered in the context of two simple modes of deformation.     

An additive theory for finite elastic–plastic deformations of the micropolar continuous media

In this paper, the method of additive plasticity at finite deformations is generalized to the micropolar continuous media. It is shown that the non-symmetric rate of deformation tensor and gradient of gyration vector could be decomposed into elastic and plastic parts. For the finite elastic deformation, the micropolar hypo-elastic constitutive equations for isotropic micropolar materials are considered. Concerning the additive decomposition and the micropolar hypo-elasticity as the basic tools, an elastic–plastic formulation consisting of an arbitrary number of internal variables and arbitrary form of plastic flow rule is derived. The localization conditions for the micropolar material obeying the developed elastic–plastic constitutive equations are investigated. It is shown that in the proposed formulation, the rate of skew-symmetric part of the stress tensor does not exhibit any jump across the singular surface. As an example, a generalization of the Drucker–Prager yield criterion to the micropolar continuum through a generalized form of the J ₂-flow theory incorporating isotropic and kinematic hardenings is introduced.     

Computation of green’s tensor and wave propagation in the random granular elastic medium

Abstract

A linear differential operator equation involving randomly variable field parameters, characterising the heterogeneous granular elastic medium is considered. The appropriate Green’s tensor is evaluated for the non-deterministic operator equations in the form of Fourier integrals in the frequency space; the exact evaluation is carried out to obtain the 36 components of Green’s tensor. The problem of wave propagation in the random granular elastic medium is then carried out with the help of the associated Green’s tensor. The effect of random variation of parameters on wave propagation in the granular elastic medium is examined. Dispersion equations have been analysed in details.     

A hyperelastic-based large strain elasto-plastic constitutive formulation with combined isotropic-kinematic hardening using the logarithmic stress and strain measures

This paper addresses the formulation of a set of constitutive equations for finite deformation metal plasticity. The combined isotropic-kinematic hardening model of the infinitesimal theory of plasticity is extended to the large strain range on the basis of three main assumptions: (i) the formulation is hyperelastic based, (ii) the stress-strain law preserves the elastic constants of the infinitesimal theory but is written in terms of the Hencky strain tensor and its elastic work conjugate stress tensor, and (iii) the multiplicative decomposition of the deformation gradient is adopted. Since no stress rates are present, the formulation is, of course, numerically objective in the time integration. It is shown that the model gives adequate physical behaviour, and comparison is made with an equivalent constitutive model based on the additive decomposition of the strain tensor.     

Incremental constitutive equation for large strain elasto plasticity

Starting from the standard theory with intermediate configuration for finite deformations of an isotropic elasto-plastic material with isotropic hardening, rate type constitutive equations are obtained. The small elastic strain approximation is then discussed and it is shown that, in this approximation, these equations reduce to Hill's formalism of large strain elasto-plasticity obtained from the classical Prandtl-Reuss relations of infinitesimal plasticity by substituting for the infinitesimal strain rate, stress and stress rate respectively the rate of deformation tensor, the Cauchy stress tensor and the Jaumann stress rate tensor. The limiting case of perfect plasticity is also investigated.     

饱和弹性裂隙介质的混合物理论

本文首先用损伤力学的方法,按孔隙的配置及几何结构,分别定义了含各向异性分布裂隙的固体介质的二阶连续法向裂纹张量和切向裂纹张量。然后,在裂隙内充满流体时,对组分速度、组分偏应力等混合物理论的基本变量进行了各向异性修正。并用混合物理论,建立了饱和裂隙介质中各组分的质量和动量平衡方程。最后,在仅考虑裂纹的单一张开度时,针对线弹性骨架材料,得到了由不可压缩材料构成的各组分的动力学控制方程。     

Compressive failure of microcracked porous brittle solids

Constitutive equations for porous, brittle solids are developed based on the damage mechanics of elastic materials containing cavities and microcracks. For homogeneous deformation modes, microcrack growth from pores causes changes in the average elastic compliance of the material. Failure criteria in terms of bifurcations of the constitutive paths are established by examining the properties of the evolving tangent stiffness tensor. Limit points as well as localized shear band failure modes are addressed. The influence of moderate levels of lateral stresses is studied for biaxial stress states.