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A Large Strain Isotropic Elasticity Model Based on Molecular Dynamics Simulations of a Metallic Glass

机译:基于分子动力学模拟的金属玻璃大应变各向同性弹性模型

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For an isotropic hyperelastic material, the free energy per unit reference volume, ψ, may be expressed in terms of an isotropic function y = [`(y)](E)psi=bar{psi}(mathbf{E}) of the logarithmic elastic strain E=ln V. We have conducted numerical experiments using molecular dynamics simulations of a metallic glass to develop the following simple specialized form of the free energy for circumstances in which one might encounter a large volumetric strain tr E, but the shear strain Ö2|E0|sqrt{2}|mathbf{E}_{0}| (with E 0 the deviatoric part of E) is small but not infinitesimal: Ö2|E0|lessapprox0.05sqrt {2}|mathbf{E}_{0}|lessapprox0.05 numerically explored in this paper, this simple five-constant model provides a very good description of the stress-strain results from our molecular dynamics simulations.
机译:对于各向同性的超弹性材料,单位参考体积的自由能ψ可以表示为y的各向同性函数y = [`(y)](E)psi = bar {psi}(mathbf {E})对数弹性应变E = lnV。我们使用金属玻璃的分子动力学模拟进行了数值实验,以开发出以下简单的特殊形式的自由能,用于可能遇到大体积应变tr E但剪切应变较大的情况。 Ö2| E 0 | sqrt {2} | mathbf {E} _ {0} | (对于E 0 E的偏斜部分)很小,但不是无穷小:Ö2| E 0 | lessapprox0.05sqrt {2} | mathbf {E} _ {0} |在本文中进行了数值探索| lessapprox0.05,这个简单的五常数模型很好地描述了我们的分子动力学模拟所产生的应力应变结果。

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