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Thermodynamics-based stability criteria for constitutive equations of isotropic hyperelastic solids

机译:各向同性超弹性固体本构方程的基于热力学的稳定性准则

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A generalized thermodynamic stability criterion for isotropic finite elastic solids is derived using the fundamental balance laws and field equations of continuum mechanics, which is then used to formulate constitutive inequalities for the polynomial form of hyperelastic constitutive equations. Individual thermodynamic constitutive inequalities (called T-C inequalities) are derived for the neo-Hookean, Mooney Rivlin, and three-parameter generalized Rivlin models under three pure homogeneous deformation modes, namely, uniaxial compression, uniaxial tension and shear (simple and pure), and are compared against two commonly used adscititious inequalities, the Baker-Ericksen (B-E) and E-inequalities. The range of stable model constants as defined by the T-C inequalities is represented by a region in an N-dimensional coordinate space (N is the total number of model constants), which is defined as the Region of Stability (ROS). It is shown that the ROS is a function of material deformation and evolves with the limiting strain, shrinking from an initially large region representing the necessary condition of thermodynamic stability to a converged region under infinite limiting strain that is equivalent to the ROS defined by the E-inequalities. By investigating the evolution of the ROS under different deformation modes, the implication of T-C inequalities on the selection of experimental routines and filtering of erroneous test data and model constants is discussed. It is also demonstrated that while the E-inequalities are over-restrictive for hyperelastic materials with small to moderate limiting strains, an observation supported by recent experimental evidence, the B-E inequalities are inaccurate under moderate to large limiting strain conditions. The applicability of the proposed mathematical framework to other hyperelastic strain energy density forms, such as exponential/logarithmic functions, is demonstrated by investigating the thermodynamic stability of the Fung-Demiray model. It is shown that the commonly assumed restriction that the Fung-Demiray model constants must be positive can be relaxed so that some typical material behaviors under small to moderate limiting strains can also be modeled. (C) 2018 Elsevier Ltd. All rights reserved.
机译:利用基本平衡定律和连续介质力学的场方程,得出了各向同性有限弹性固体的广义热力学稳定性判据,然后将其用于为超弹性本构方程多项式形式的本构不等式。在三个纯均质变形模式(即单轴压缩,单轴拉伸和剪切(简单和纯净))下,针对新Hookean模型,Mooney Rivlin模型和三参数广义Rivlin模型推导了各个热力学本构不等式(称为TC不等式)。将Baker-Ericksen(BE)和E不平等这两个常用的吸附性不平等进行比较。由T-C不等式定义的稳定模型常数范围由N维坐标空间中的一个区域(N是模型常数的总数)表示,该区域定义为稳定区域(ROS)。结果表明,ROS是材料变形的函数,并随极限应变而演化,从代表热力学稳定性必要条件的初始大区域收缩到无限极限应变下的收敛区域,该极限区域等效于E定义的ROS。 -不平等。通过研究不同变形模式下ROS的演化,讨论了T-C不等式对实验程序选择以及错误测试数据和模型常数的过滤的影响。还证明了,尽管对于具有小到中等极限应变的超弹性材料,E不等式过于严格,但最近的实验证据支持了这一观察结果,但在中到大极限应变条件下,B-E不等式是不准确的。通过研究Fung-Demiray模型的热力学稳定性,证明了所提出的数学框架对其他超弹性应变能密度形式(例如指数/对数函数)的适用性。结果表明,可以放宽通常假定的Fung-Demiray模型常数必须为正的限制条件,从而也可以对在小到中等极限应变下的一些典型材料行为进行建模。 (C)2018 Elsevier Ltd.保留所有权利。

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