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出 处:《力学学报》2008年第4期502-510,共9页Chinese Journal of Theoretical and Applied Mechanics
基 金:国家自然科学基金(10272055)~~
摘 要:建立了欧几里德标架无关性的一般表述与某一参考标架φ下作相对刚体运动的一般曲线坐标、分量表述之间的关系,从而使欧几里德标架无关性的张量表述有相应的分量表述形式.建立这种联系的基础是,参考标架φ~*下描述的运动在参考标架φ中某坐标系下的分量结果,对应于φ下另一相对该坐标系作相同刚体运动的坐标系下描述φ观测的运动的分量结果.通过例子说明了Truesdell和Noll用等价动力过程,关于物质标架无关性原理的陈述,比Svendsen和Bertram及Liu的本构关系在参考标架变换下的形式不变性更合理且方便,尤其是对微分方程形式的本构关系更是如此.The main purpose of the present paper is to obtain the relation between the general expression of Euclidean objectivity and the component expression in the general curvilinear coordinate system with a relative rigid motion under a fixed frame φ of reference, so as to the tensor representation of Euclidean objective quantity has its component form. That is, an objective quantity under the reference frame φ* has its components with respect to the fixed coordinate system of reference frame φ, while the objective quantity under the reference frame φ has its components relative to another coordinate system of φ with the same relative rigid motion as that of φ and φ* to the fixed coordinate system of φ. The two types of components correspond to each other. Moreover, it is exemplified in the present paper that the principle of material frame-indifference with the admissible equivalent dynamic processes of a body by Truesdell and Noll[14] is more convenient than the form-invariance of constitutive equations by Svendsen and Bertram[13] and Liu[4], especially for the rate-form constitutive equations.
关 键 词:欧几里德标架无关性 物质标架无关性 参考标架变换 客观张量 本构关系
分 类 号:O331[理学—一般力学与力学基础]
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