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On a variant of the Maxwell and Oldroyd-B models within the context of a thermodynamic basis

机译:在热力学基础上的麦克斯韦和奥德罗伊德-B模型的变体

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In this paper we develop models within a theimodynamic standpoint that are very similar in form to the classical Maxwell and Oldroyd-B models but differ from them in one important aspect, the manner in which they unload instantaneously from the deformed configuration. As long as the response is not instantaneous, the models that are derived cannot be differentiated from the Maxwell and Oldroyd-B models, respectively. The models can be viewed within the context of materials whose natural configuration evolves, the evolution being determined by the maximization. of the rate of entropy production of the material. However, the underpinnings to develop the model are quite different from an earlier development by Rajagopal and Srinivasa [8] in that while the total response of the viscoelastic fluid satisfies the constraint of an incompressible material, the energy storage mechanism associated with the elastic response is allowed to be that for a compressible elastic solid and the dissipative mechanism associated with the viscous response allowed to be that for a compressible fluid, the total deformation however being isochoric. The analysis calls for a careful evaluation of firmly held customs in viscoelasticity wherein it is assumed that it is possible to subject a material to a purely instantaneous elastic response without any dissipation whatsoever. Finally, while the model developed by Rajagopal and Srinivasa [8] arises from the linearization of the non-linear elastic response that they chose and leads to a model wherein the instantaneous elastic response is isochoric, here we develop the model within the context Of a different non-linear elastic response that need not be linearized but the instantaneous elastic response not necessarily being isochoric. (C) 2015 Elsevier Ltd. All rights reserved.
机译:在本文中,我们从热力学角度开发了模型,这些模型的形式与经典的Maxwell和Oldroyd-B模型非常相似,但在一个重要方面与它们有所不同,它们是从变形构造中立即卸载的方式。只要响应不是瞬时的,派生的模型就无法分别与Maxwell和Oldroyd-B模型区分开。可以在自然构型发生变化的材料的上下文中查看模型,该演变由最大化确定。材料的熵产生率。但是,模型开发的基础与Rajagopal和Srinivasa [8]的早期开发有很大不同,因为粘弹性流体的总响应满足不可压缩材料的约束,而与弹性响应相关的能量存储机制是对于可压缩的弹性固体,其允许值是多少,而与粘性响应相关的耗散机理,对于可压缩的流体,其总变形是等容的。该分析要求对粘弹性的牢固习惯进行仔细评估,其中假定可以使材料经受纯瞬时弹性响应而无任何耗散。最后,虽然Rajagopal和Srinivasa [8]开发的模型是由他们选择的非线性弹性响应的线性化产生的,并导致了其中瞬时弹性响应是等速的模型,但在此我们在a的上下文中开发了该模型。不需要线性化的不同非线性弹性响应,但瞬时弹性响应不一定是等容的。 (C)2015 Elsevier Ltd.保留所有权利。

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