doc:user:elements:volumes:hyper_materials
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| doc:user:elements:volumes:hyper_materials [2025/02/24 14:40] – [NeoHookeanHyperMaterial] vanhulle | doc:user:elements:volumes:hyper_materials [2026/01/16 15:36] (current) – [VeIsoHyperPk2Material] vanhulle | ||
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| Line 15: | Line 15: | ||
| === Parameters === | === Parameters === | ||
| ^ | ^ | ||
| - | | Density | + | | Density |
| | NeoHookean coefficient ($C_1$) | | NeoHookean coefficient ($C_1$) | ||
| - | | Initial bulk modulus ($k_0$) | + | | Initial bulk modulus ($k_0$) |
| | Material temperature evolution law | '' | | Material temperature evolution law | '' | ||
| - | | Thermal expansion coefficient ($\alpha$) | + | | Thermal expansion coefficient ($\alpha$) |
| - | ===== NeoHookeanHyperMaterial | + | ===== TmNeoHookeanHyperMaterial |
| - | <note important> | + | <note important> |
| === Description === | === Description === | ||
| Neo-Hookean hyperelastic law, using a '' | Neo-Hookean hyperelastic law, using a '' | ||
| Line 30: | Line 30: | ||
| === Parameters === | === Parameters === | ||
| ^ | ^ | ||
| - | | Density | + | | Density |
| | NeoHookean coefficient ($C_1$) | | NeoHookean coefficient ($C_1$) | ||
| - | | Initial bulk modulus ($k_0$) | + | | Initial bulk modulus ($k_0$) |
| - | | Thermal expansion coefficient ($\alpha$) | + | | Thermal expansion coefficient ($\alpha$) |
| | Conductivity | | Conductivity | ||
| | Heat capacity | | Heat capacity | ||
| Line 52: | Line 52: | ||
| === Parameters === | === Parameters === | ||
| - | ^ | + | ^ |
| - | | Density | + | | Density |
| - | | Mooney-Rivlin coefficient ($C_1$) | + | | Mooney-Rivlin coefficient ($C_1$) |
| - | | Mooney-Rivlin coefficient ($C_2$) | + | | Mooney-Rivlin coefficient ($C_2$) |
| - | | Initial bulk modulus ($k_0$) | + | | Initial bulk modulus ($k_0$) |
| + | | Material temperature evolution law | '' | ||
| + | | Thermal expansion coefficient ($\alpha$) | ||
| Line 65: | Line 67: | ||
| </ | </ | ||
| - | ===== HolzapfelGasserOgdenHyperMaterial | + | ===== TmMooneyRivlinHyperMaterial |
| + | <note important> | ||
| === Description === | === Description === | ||
| - | Holzapfel-Gasser-Ogden (invariant-based) anisotropic hyperelastic law, using a '' | ||
| - | (Quasi-)incompressibility is treated by a volumetric/ | + | Mooney-Rivlin hyperelastic law, using a '' |
| - | The strain-energy density function $W$ is expressed as the sum of an **isotropic** (=**matrix**) and **anisotropic** (=**fibers**) contribution: | + | Here, the '' |
| - | $$ | + | |
| - | W\left(\bar{I}_1,\bar{I}_4,J \right) = W_{iso}\left(\bar{I}_1, | + | |
| - | $$ | + | |
| - | + | ||
| - | The **isotropic** contribution takes the form of a **generalized Neo-Hookean** model: | + | |
| - | $$ | + | |
| - | W_{iso}\left(\bar{I}_1, | + | |
| - | $$ | + | |
| - | + | ||
| - | The **anisotropic** contribution to the strain energy density function writes: | + | |
| - | $$ | + | |
| - | W_{ani}\left(\bar{I}_1, | + | |
| - | $$ | + | |
| - | where $k_1$[MPa] and $k_2$[-] are material parameters characterizing all fiber families in the material. $d\in[0, | + | |
| - | + | ||
| - | More information and mathematical derivations, | + | |
| === Parameters === | === Parameters === | ||
| - | ^ | + | ^ |
| - | | Density | + | | Density |
| - | | Mooney-Rivlin coefficient ($C_1$) | + | | Mooney-Rivlin coefficient ($C_1$) |
| - | | Initial bulk modulus | + | | Mooney-Rivlin coefficient |
| - | | HGO parameter $k_1$ |'' | + | | Initial bulk modulus ($k_0$) |
| - | | HGO parameter | + | | Thermal expansion coefficient ($\alpha$) |
| - | | Fiber dissipation $d$ (optional, default=0) | + | | Conductivity |
| - | | Direction of $1^{st}$ fiber family | + | | Heat capacity |
| - | | Direction of $2^{nd}$ fiber family $\mathbf{a}^2$ | + | | Dissipated thermoelastic power fraction |
| - | | Direction of $3^{rd}$ fiber family $\mathbf{a}^3$ | + | | Dissipated (visco)plastic power fraction (Taylor-Quinney factor) |
| ===== NeoHookeanHyperPk2Material ===== | ===== NeoHookeanHyperPk2Material ===== | ||
| Line 114: | Line 100: | ||
| $$ | $$ | ||
| - | The deviatoric potential is computed based on a Cauchy tensor with a unit determinant: | + | The deviatoric potential is computed based on the right Cauchy–Green deformation |
| $$ | $$ | ||
| Line 122: | Line 108: | ||
| === Parameters === | === Parameters === | ||
| - | ^ | + | ^ |
| - | | Density | + | | Density |
| - | | Initial bulk modulus ($k_0$) | + | | Initial bulk modulus ($k_0$) |
| - | | Initial shear modulus ($g_0$) | + | | Initial shear modulus ($g_0$) |
| + | | Material temperature evolution law | '' | ||
| + | | Thermal expansion coefficient ($\alpha$) | ||
| ===== LogarihtmicHyperPk2Material ===== | ===== LogarihtmicHyperPk2Material ===== | ||
| Line 133: | Line 121: | ||
| Logarithmic hyperelastic law, using a '' | Logarithmic hyperelastic law, using a '' | ||
| - | The potential per unit volume is computed based on the average compressibility of the element, ($q$): | + | The potential per unit volume is computed based on the average compressibility of the element, ($\theta$): |
| $$ | $$ | ||
| Line 147: | Line 135: | ||
| === Parameters === | === Parameters === | ||
| - | ^ | + | ^ |
| - | | Density | + | | Density |
| - | | Initial bulk modulus ($k_0$) | + | | Initial bulk modulus ($k_0$) |
| - | | Initial shear modulus ($g_0$) | + | | Initial shear modulus ($g_0$) |
| + | | Material temperature evolution law | '' | ||
| + | | Thermal expansion coefficient ($\alpha$) | ||
| ===== EvpIsoHLogarithmicHyperPk2Material ===== | ===== EvpIsoHLogarithmicHyperPk2Material ===== | ||
| Line 172: | Line 163: | ||
| ^ | ^ | ||
| - | | Density | + | | Density |
| - | | Initial bulk modulus ($k_0$) | + | | Initial bulk modulus ($k_0$) |
| - | | Initial shear modulus ($g_0$) | + | | Initial shear modulus ($g_0$) |
| | Number of the material law which defines the yield stress $\sigma_{yield}$ | '' | | Number of the material law which defines the yield stress $\sigma_{yield}$ | '' | ||
| + | | Material temperature evolution law | '' | ||
| + | | Thermal expansion coefficient ($\alpha$) | ||
| ===== FunctionBasedHyperPk2Material ===== | ===== FunctionBasedHyperPk2Material ===== | ||
| Line 194: | Line 187: | ||
| ^ | ^ | ||
| - | | Density | + | | Density |
| - | | Initial bulk modulus ($k_0$) | + | | Initial bulk modulus ($k_0$) |
| - | | Number of the hyperelastic law | '' | + | | Number of the hyperelastic law | '' |
| + | | Material temperature evolution law | '' | ||
| + | | Thermal expansion coefficient ($\alpha$) | ||
| Line 239: | Line 234: | ||
| ^ | ^ | ||
| - | | Density | + | | Density |
| - | | Initial bulk modulus ($k_0$) | + | | Initial bulk modulus ($k_0$) |
| | Number of the main viscoelastic law | '' | | Number of the main viscoelastic law | '' | ||
| - | | Number | + | | Array of numbers definining |
| - | | Number of the second Maxwell viscoelastic | + | | Material temperature evolution |
| - | | Number of the third Maxwell viscoelastic law (optional) | '' | + | | Thermal expansion coefficient |
doc/user/elements/volumes/hyper_materials.1740404406.txt.gz · Last modified: by vanhulle
