doc:user:elements:volumes:hyper_dev_potential
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| doc:user:elements:volumes:hyper_dev_potential [2026/07/02 15:25] – [GeneralizedMaxwellHyperPotential] vanhulle | doc:user:elements:volumes:hyper_dev_potential [2026/07/02 15:47] (current) – [EightChainHyperPotential] vanhulle | ||
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| Line 76: | Line 76: | ||
| === Description === | === Description === | ||
| + | The deviatoric part of the isotropic Eight-Chain (or Arruda-Boyce) hyperelastic law writes | ||
| + | $$ | ||
| + | W^e_{EC}\left( \bar{\lambda^*}, | ||
| + | |||
| + | $$ where $N$ is the number of chains per unit volume, $k_B$ is Boltzmann constant, $\theta_0$ is the reference temperature, | ||
| + | $\bar{\lambda^*}$ is the effective distortional stretch and writes | ||
| + | $$ | ||
| + | \bar{\lambda}^*=\sqrt{\frac{\bar{I}_1}{3}}. | ||
| + | $$ | ||
| + | |||
| + | The Cauchy stress writes | ||
| + | $$ | ||
| + | \boldsymbol{\sigma}=\frac{\mu}{J \bar{\lambda}^*}\frac{\mathcal{L}\left(\frac{\bar{\lambda}^*}{\lambda^{lock}}\right)}{\mathcal{L}\left(\frac{1}{\lambda^{lock}}\right)}\text{dev}\left(\bar{\mathbf{B}}\right), | ||
| + | $$ | ||
| + | where the locking stretch $\lambda_{lock}=\sqrt{n}$ and shear modulus | ||
| + | $$ | ||
| + | \mu = \frac{N k_B\theta_0}{3}\lambda^{lock} \mathcal{L}^{-1}\left(\frac{1}{\lambda^{lock}}\right) | ||
| + | $$ | ||
| + | have been introduced to simplify the formulation. | ||
| + | |||
| + | [[https:// | ||
| + | A three-dimensional constitutive model for the large stretch behavior of rubber elastic materials, Journal of the Mechanics and Physics of Solids, Volume 41, Issue 2, 1993, Pages 389-412.]] | ||
| === Parameters === | === Parameters === | ||
| ^ | ^ | ||
| - | | Neo-Hookean coefficient | + | | Shear modulus |
| + | | Locking stretch ($\lambda_{lock}$) | ||
doc/user/elements/volumes/hyper_dev_potential.1782998751.txt.gz · Last modified: by vanhulle
