Titlebook: Hyperelasticity Primer; Robert M. Hackett Textbook 20161st edition Springer International Publishing Switzerland 2016 1st, 2nd, 3rd, and 4

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书目名称Hyperelasticity Primer影响因子(影响力)




书目名称Hyperelasticity Primer影响因子(影响力)学科排名




书目名称Hyperelasticity Primer网络公开度




书目名称Hyperelasticity Primer网络公开度学科排名




书目名称Hyperelasticity Primer被引频次




书目名称Hyperelasticity Primer被引频次学科排名




书目名称Hyperelasticity Primer年度引用




书目名称Hyperelasticity Primer年度引用学科排名




书目名称Hyperelasticity Primer读者反馈




书目名称Hyperelasticity Primer读者反馈学科排名

整理

packet

议程

妨碍议事

Finite Elasticity,troduction of a strain-energy (or stored-energy) function into elasticity is due to George Green (1793–1841) and elastic solids for which such a function is assumed to exist are said to be Green elastic or hyperelastic. Elasticity without an underlying strain-energy function is called Cauchy elastic

Agnosia

委屈

Polar Decomposition,olar decomposition theorem states that any deformation gradient tensor can be multiplicatively decomposed into the product of an orthogonal tensor, known as the rotation tensor, and a symmetric tensor called the right stretch tensor, or into the product of a symmetric tensor called the left stretch

空中

Strain-Energy Functions,unction of the three invariants of each of the two Cauchy-Green deformation tensors, given in terms of the principal extension ratios, or stretches. A number of different strain-energy formulations exist, having properties and characteristics that make them appropriate for characterizing different h

单独

Stress Measures,ensor, a Lagrangian formulation, is the most significant of the stress measures. The formulation and steps for computing it are presented in terms of the Mooney-Rivlin strain-energy function model. The Cauchy stress tensor, an Eulerian formulation, is obtained directly from the second Piola-Kirchhof

切割

Tangent Moduli, is linear, the stiffness does not change as deformation changes. However, for a hyperelastic model, differentiating the strain-energy function with respect to either the finite strain tensor or one of the two Cauchy-Green deformation tensors yields elastic “constants,” the magnitude of which depend