材料生长与变形的连续介质模型:平衡方程与边界条件

本文探讨了生长变形体连续介质模型的平衡理论框架。文中首先证明了广义输运定理，根据这个定理，推导了生长变形体广义平衡方程的一般形式及其生长边界条件，并导出反映生长边界面对平衡影响的生长耦合函数。在此基础上，具体讨论了质量、动量、动量矩以及能量平衡方程，并对其中相伴出现的一些新的物理量进行了评述；此外，还根据非平衡热力学理论的局域平衡假设建立了描述生长变形体热力学过程的熵不等式。这些方程唯象反映了生长变形体在运动、变形与生长过程中各物理量之间的耦合关系与平衡规律。     

两相混合流体的非线性本构理论

本文从连续介质力学的基本原理出发,建立了微极流体与经典流体两相流动的非线性扩散理论。给出了混合流体本构方程的一般形式。对单相流体、单相微极流体及稀悬浮体三种特殊情形,得到了具体形式的二阶非线性本构方程,并同已有的理论进行了比较。     

谈微元体平衡微分方程的教学法

从微梁段、部分截面微梁段、微矩形薄板和3维微元体的平衡问题入手,逐一分析平衡体中的应力与内力的关系,详细讨论这种关系的数学与力学意义并建立相应的平衡方程,考察了方程形式由常微分方程到偏微分方程组的变化,将分析结果列入表格进行对比,指出了微元体和应力状态在图示法上的区别,还总结了``用力的平衡条件可求应力'的前提条件和适用原则。     

类石墨烯二维原子晶体的微态理论模型

基于微态(Micromorphic) 连续介质理论,提出了针对类石墨烯二维原子晶体的新力学模型. 该模型以有限大小的布拉维单胞为基元体,考虑基元粒子的宏观位移和微观变形,依据微态理论基本方程,推导了全局坐标系下模型的主导方程. 然后针对布拉维单胞中含有两个原子的类石墨烯晶体,通过分析单胞中声子振动模式与基元体自由度的关系,获得了微态形式下声子色散关系的久期方程,并根据二维晶体声子色散特性对久期方程进行了简化,进而确定了类石墨烯晶体模型的本构方程. 最后,以石墨烯和单层六方氮化硼为例,利用简化的表达式拟合了它们面内声子色散关系数据,计算了模型材料的常数,石墨烯模型的等效杨氏模量、泊松比分别为1.05 TPa 和0.197,氮化硼分别为0.766 TPa 和0.225,均与已有的实验值相符合.      

爆炸与冲击中的实际物质状态方程

本文综述了爆炸力学计算中涉及的实际介质的状态方程,这些物质结构复杂,其描述方法与金属的状态方程有些不同.用物理力学观点及半经验、半理论方法进行描述.①用普遍的热力学方法导出介质的状态方程表达式,并用实测数据计算了有关的参量;②Grneisen系数值的计算以及它与体积和温度的关系;③多孔介质的优态方程;④从理论上系统地导出了波后卸载方程;⑤探讨了原予统计模型的边界势.      

材料生长与变形的连续介质模型:弹性本构方程

本文着重探讨了生长变形体连续介质理论中的本构模型。首先列出了描述生长变形体能量平衡的微分方程以及熵不等式；以此为基础，通过将密度演化的历史作为独立的本构变量扩展了理性力学的因果性公理与决定性公理，具体而详细地推导了简单材料的生长弹性本构方程，给出了这些本构方程中的相关本构变量之间的约束不等式，得到了“生长变形体的自由能与其密度成反比”的结论，并从热力学上对这一结果进行了定性的解释。最后，文中对几个尚待解决的问题进行了说明，并指出了今后的发展方向。     

一种化学-力学耦合连续介质理论与数值格式

对化学驱动的连续介质化学-力学耦合系统进行研究,从热力学定律和化学势角度出发,推导了等温过程的化学-力学耦合本构关系和控制方程,利用变分方法建立了化学-力学耦合系统的能量泛函,得到化学-力学耦合控制方程的等效积分形式和相应的有限元列式. 结合算例,对连续介质的化学-力学耦合行为进行了数值计算,数值结果反映了化学与力学系统的相互耦合作用,即浓度变化能引起介质的变形,同样力学作用也能引起浓度重分布. 从全新的角度建立了描述连续介质的化学-力学耦合行为的基本理论和数值方法,能够较好地反映一类连续介质的化学-力学耦合行为.      

理论力学研究性教学新探索:刚体运动基点法公式与连续介质速度场分解

基础力学课程体系是现代工程教育的重要基础。理论力学作为力学课程体系的起点，提供了力学基本概念和原理。一方面，以离散体系(质点/刚体)为研究对象的理论力学与以连续体系(介质/变形微元体)为对象的连续介质力学，它们之间既存在密切联系又差异明显；另一方面，源于理论/经典力学的动力系统理论和非线性科学研究对应用力学学科产生了广泛影响。围绕这两个侧面，作者将在《理论力学研究性教学新探索》系列教研论文中阐释它们之间的联系。本篇探讨刚体运动基点法公式和连续介质速度场分解之间的关系，它们分别给出刚体模型和连续介质模型的速度分布规律，前者依赖刚体转动角速度矢量，而后者由速度梯度张量所刻画。本文将说明，两者存在对应理论关系，且刚体基点法公式是连续介质速度场分解的退化形式，即忽略变形效应。     

基于微态方法的耦合韧性损伤的弹塑性本构模型

基于广义连续介质力学提出了一个热力学一致性的耦合微态韧性损伤的弹塑性本构模型。该模型遵循Forest的微态方法,在有限变形中提出引入额外的微态损伤因子及其一阶梯度以考虑材料的内部特征尺度。通过广义虚功原理得到了微态损伤的补充控制方程,对亥姆霍兹自由能进行扩展,得到了新的包含微态损伤变量的损伤能量释放率,在微态损伤的正则化作用下,采用隐式迭代更新局部损伤和应力等状态变量。基于Galerkin加权余量法,推导了以传统位移和微态损伤为基本未知量的有限元列式。利用该数值模型,对DP1000材料的单向拉伸实验和十字形零件的冲压实验进行了应变局部化与材料断裂的有限元分析。结果表明,该微态弹塑性损伤模型可以得到一致的有限元模拟响应曲线并收敛到实验曲线,从而避免发生网格依赖性问题。     

缺陷连续统理论及其在本构方程研究中的应用 Ⅰ.一般概述,运动学和变形几何学

缺陷连续统理论即缺陷场论是当代固体力学的一个重要分支,其主要任务是对物质的弹性和非弹性性质的宏、微观研究之间架起一座桥梁。它也被认为是由固体力学、近代物理和数学之间交互作用而发展起来的一门交缘学科。本文分三部分较系统地介绍了它的主要发展和最近结果。第Ⅰ部分讨论具有位错和旋错连续统的运动学和变形几何学,包括Nye,Kondo,Bilby和Krner等人的早期结果以及我们利用4维物质流形上Cartan结构方程推导出的非线性动力学方程的最近结果。第Ⅱ部分详细介绍了缺陷连续统的规范场理论,主要强调对该连续统动力学方程的发展。第Ⅲ部分研究缺陷场论对构造弹塑性物质本构关系的应用。      

RENEWAL OF BASIC LAWS AND PRINCIPLES FOR POLAR CON-TINUUM THEORIES (Ⅱ)—MICROMORPHIC CONTINUUM THEORY AND COUPLE STRESS THEORY

IntroductionThispaperisadirectcontinuationofRef.[1 ] .InitthecoupledconservationlawofenergypresentedinRef.[2 ]wasextendedandtherathercompletesystemsofbasicbalancelawsandequationsformicropolarcontinuumtheoryhavebeenconstitutedbycombiningtherenewedresultsandthetraditionalconservationlawsofmassandmicroinertiaandtheentropyinequality .Thepurposeofthispaperistorestablishthesystemsofbasicbalancelawsandequationsformicromorphiccontinuumtheoryandcouplestresstheoryviadirecttransitionsandreductionsfromth…     

RENEWAL OF BASIC LAWS AND PRINCIPLES FOR POLAR CON-TINUUM THEORIES (Ⅱ)—MICROMORPHIC CONTINUUM THEORY AND COUPLE STRESS THEORY

The purpose is to reestablish the balance laws of momentum, angular momentum and energy and to derive the corresponding local and nonlocal balance equations for micromorphic continuum mechanics and couple stress theory. The desired results for micromorphic continuum mechanics and couple stress theory are naturally obtained via direct transitions and reductions from the coupled conservation law of energy for micropolar continuum theory, respectively. The basic balance laws and equations for micromorphic continuum mechanics and couple stress theory are constituted by combining these results derived here and the traditional conservation laws and equations of mass and microinertia and the entropy inequality. The incomplete degrees of the former related continuum theories are clarified. Finally, some special cases are conveniently derived. Foundation items: the National Natural Science Foundation of China (10072024); the Research Foundation of Liaoning Education Committee (990111001) Biography: DAI Tian-min (1931≈)     

Material force in micromorphic plasticity

Micromorphic theory envisions a material body as a continuous collection of deformable particles with finite size and inner structure. It is considered as the most successful top-down formulation of a two-level continuum model, in which the deformation is expressed as a sum of macroscopic continuous deformation and internal microscopic deformation of the inner structure. In this work, we revisit the original micromorphic theory and further construct a mathematical theory of micromorphic plasticity with generalized strain-based return mapping algorithm. The concept of material forces, which may also be referred as Eshelbian mechanics, was first derived for micromorphic thermo-visco-elastic solid, and, now in this work, it is extended to the micromorphic plasticity. The balance law of pseudo-momentum is formulated. The detailed expressions of Eshelby stress tensor, pseudo-momentum, and material forces are derived. Following this formulation, the failure mechanisms of micromorphic thermo-visco-elastoplastic materials can be further investigated.     

Micromorphic continuum Part I: Strain and stress tensors and their associated rates

Micropolar and micromorphic solids are continuum mechanics models, which take into account, in some sense, the microstructure of the considered real material. The characteristic property of such continua is that the state functions depend, besides the classical deformation of the macroscopic material body, also upon the deformation of the microcontinuum modeling the microstructure, and its gradient with respect to the space occupied by the material body. While micropolar plasticity theories, including non-linear isotropic and non-linear kinematic hardening, have been formulated, even for non-linear geometry, few works are known yet about the formulation of (finite deformation) micromorphic plasticity. It is the aim of the three papers (Parts I, II, and III) to demonstrate how micromorphic plasticity theories may be formulated in a thermodynamically consistent way.In the present article we start by outlining the framework of the theory. Especially, we confine attention to the theory of Mindlin on continua with microstructure, which is formulated for small deformations. After precising some conceptual aspects concerning the notion of microcontinuum, we work out a finite deformation version of theory, suitable for our aims. It is examined that resulting basic field equations are the same as in the non-linear theory of Eringen, which deals with a different definition of the microcontinuum. Furthermore, geometrical interpretations of strain and curvature tensors are elaborated. This allows to find out associated rates in a natural manner. Dual stress and double stress tensors, as well as associated rates, are then defined on the basis of the stress powers. This way, it is possible to relate strain tensors (respectively, micromorphic curvature tensors) and stress tensors (respectively, double stress tensors), as well as associated rates, independently of the particular constitutive properties.     

Anti-plane problems of piezoelectric material with a micro-void or micro-inclusion based on micromorphic electroelastic theory

The linear theory of micromorphic electroelasticity, which incorporate the coupled electromechanical behavior into the framework of micromorphic continuum theory, is used to solve the anti-plane problems of piezoelectric media with a micro-void or micro-inclusion in this paper. The electromechanical field solutions for a transversely isotropic piezoelectric medium are derived in the context of micromorphic electroelasticity and a generalized characteristic length is introduced to describe the size effect. Anti-plane problems of an infinite piezoelectric medium containing a micro-void or micro-inclusion are analyzed. Numerical results reveal that the mechanical and electric fields predicted by the present model highly depend on the relative size of the micro-void or micro-inclusion with respect to the generalized characteristic length, which is obviously different from the classical prediction.     

Theory of 4D-media with stationary dislocations

In earlier studies, the authors showed that an application of classical methods of mechanics of deformable media to the study of properties of 4D-space-time continuum permit stating consistent models of nonholonomic media mechanics consistent with the first and second laws of thermodynamics. In the present paper, we show that the classical methods of continuum mechanics are also promising when modeling physical processes. It is shown that, just as in the three-dimensional theory of stationary dislocations, there exist dislocations of three types for a generalized 4D-medium. They correspond to the decomposition of the free distortion tensor into a spherical tensor, a deviator tensor, and a pseudotensor of rotations. We interpret several particular models, thus showing that the proposed model describes the spectrum of known physical interactions: electromagnetic, strong, weak, and gravitational. We show that the resolving equations include the Maxwell equations of electrodynamics and the Yukawa equations for strong interactions as subsystems.