Adiabatic Processes and Constraints in Thermoelasticity

K. Rajagopal, A. Srinivasa
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引用次数: 0

Abstract

The aim of this paper is to briefly outline an approach to the thermomechanics of thermoelastic solids based on the notion of multiple natural states and the use of adiabatic processes. We use a statement of the second law attributed to Kelvin for certain special cycles and show that the work done in adiabatic cycles of deformation is non-positive. With these and other assumptions on the nature of thermoelastic solids, we demonstrate the existence of an entropy function and the absolute temperature scale. In this, we closely follow the arguments of Caratheodory (1976). Finally, we briefly address the issues of a class of thermomechanical constraints and show that they naturally lead to considering constraints on adiabatic processes. The principal results are the following: 1. Demonstration of the existence of the absolute temperature and entropy functions based on the consideration of adiabatic processes 2. A one-to-one correspondence between the stress-free states and the entropy, leading to a “decomposition” of the deformation gradient as Fκr = FκnG(η). 3. Physical interpretation of the constraints of the form f(Eκr,η) = 0.
热弹性中的绝热过程和约束
本文的目的是简要概述热弹性固体的热力学方法基于多自然状态的概念和绝热过程的使用。对于某些特殊的循环,我们使用了开尔文第二定律,并证明了在绝热变形循环中所做的功是非正的。利用这些和其他关于热弹性固体性质的假设,我们证明了熵函数和绝对温标的存在。在这方面,我们密切关注Caratheodory(1976)的论点。最后,我们简要地讨论了一类热力约束的问题,并表明它们自然导致考虑绝热过程的约束。主要结果如下:1。考虑绝热过程的绝对温度函数和绝对熵函数存在性的证明无应力状态与熵之间的一对一对应关系,导致变形梯度的“分解”为f - κr = f - κ ng (η)。3.f(Eκr,η) = 0形式约束的物理解释。
本文章由计算机程序翻译,如有差异,请以英文原文为准。
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