doc:user:elements:volumes:iso_hypo_materials
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| Both sides previous revisionPrevious revisionNext revision | Previous revision | ||
| doc:user:elements:volumes:iso_hypo_materials [2025/07/22 11:14] – [EvpIsoHHypoMaterial] papeleux | doc:user:elements:volumes:iso_hypo_materials [2026/06/12 14:43] (current) – [TmContinuousDamageEvpIsoHHypoMaterial] papeleux | ||
|---|---|---|---|
| Line 25: | Line 25: | ||
| | Orthotropic axis | | Orthotropic axis | ||
| | Orthotropic axis | | Orthotropic axis | ||
| - | | Orthotropic axis initialized by mesh construction \\ boolean : True - (def) False \\ override OrthoAxis definition | + | | Orthotropic axis initialized by mesh construction \\ boolean : True - False (def) \\ override OrthoAxis definition |
| ===== TmElastHypoMaterial ===== | ===== TmElastHypoMaterial ===== | ||
| Line 47: | Line 47: | ||
| | Orthotropic axis | '' | | Orthotropic axis | '' | ||
| | Orthotropic axis | '' | | Orthotropic axis | '' | ||
| - | | Orthotropic axis initialized by mesh construction | + | | Orthotropic axis initialized by mesh construction |
| | Thermal expansion | | Thermal expansion | ||
| | Conductivity | | Conductivity | ||
| - | | Heat capacity | + | | Heat Capacity |
| + | | Heat Capacity Type : \\ - ENTHALPY_CONSISTENT (default) necessary \\ for high variation of the Heat capacity (phase change) \\ - POINT_WISE for slow variation of Heat Capacity | '' | ||
| | Dissipated thermoelastic power fraction | | Dissipated thermoelastic power fraction | ||
| | Dissipated (visco)plastic power fraction (Taylor-Quinney factor) | | Dissipated (visco)plastic power fraction (Taylor-Quinney factor) | ||
| Line 201: | Line 202: | ||
| :!: Thermomechanical calculation method : | :!: Thermomechanical calculation method : | ||
| * When the thermal expansion changes, an average value is computed over the time step is estimated to model this thermal expansion properly. | * When the thermal expansion changes, an average value is computed over the time step is estimated to model this thermal expansion properly. | ||
| - | * If the heat capacity changes, | + | * Heat Capacity Type allows to manage varying Heat Capacity : |
| + | * POINT_WISE : compute | ||
| + | * ENTHALPY_CONSISTENT (default) : an average value is computed to estimate properly the energy balance. An equivalent heat capacity can be used to take into account the latent heat (= heat capacity + latent heat). Needed for fast variation of HeatCapacity (ex: solid phase changes). | ||
| ---- | ---- | ||
| Line 216: | Line 219: | ||
| | Conductivity | | Conductivity | ||
| | Heat capacity | | Heat capacity | ||
| + | | Heat capacity type : \\ - ENTHALPY_CONSISTENT (default) necessary \\ for high variation of the Heat capacity (phase change) \\ - POINT_WISE for slow variation of Heat Capacity | ||
| | Dissipated thermoelastic power fraction | | Dissipated thermoelastic power fraction | ||
| | Dissipated (visco)plastic power fraction (Taylor-Quinney factor) | | Dissipated (visco)plastic power fraction (Taylor-Quinney factor) | ||
| Line 239: | Line 243: | ||
| - | === Parameters === | + | === Parameters |
| ^ | ^ | ||
| Line 254: | Line 258: | ||
| | Number of kinematic hardening law 4 | | Number of kinematic hardening law 4 | ||
| | Number of kinematic hardening law 5 | | Number of kinematic hardening law 5 | ||
| + | | Material temperature evolution law | '' | ||
| + | |||
| + | === Parameters (Metafor version > | ||
| + | |||
| + | ^ | ||
| + | | Density | ||
| + | | Young' | ||
| + | | Poisson Ratio | '' | ||
| + | | Material Stiffness | ||
| + | | Thermal expansion | ||
| + | | Number of the material law which defines the yield stress $\sigma_{yield}$ | ||
| + | | Array of numbers defining the kinematic hardening laws ([1, 2, | ||
| | Material temperature evolution law | '' | | Material temperature evolution law | '' | ||
| Line 269: | Line 285: | ||
| :!: Thermomechanical calculation method : | :!: Thermomechanical calculation method : | ||
| * When the thermal expansion changes, an average value is computed over the time step is estimated to model this thermal expansion properly. | * When the thermal expansion changes, an average value is computed over the time step is estimated to model this thermal expansion properly. | ||
| - | * If the heat capacity changes, | + | * Heat Capacity Type allows to manage varying Heat Capacity : |
| + | * POINT_WISE : compute | ||
| + | * ENTHALPY_CONSISTENT (default) : an average value is computed to estimate properly the energy balance. An equivalent heat capacity can be used to take into account the latent heat (= heat capacity + latent heat). Needed for fast variation of HeatCapacity (ex: solid phase changes). | ||
| ---- | ---- | ||
| - | === Parameters === | + | === Parameters |
| ^ | ^ | ||
| Line 293: | Line 311: | ||
| | Dissipated (visco)plastic power fraction (Taylor-Quinney factor) | | Dissipated (visco)plastic power fraction (Taylor-Quinney factor) | ||
| + | |||
| + | === Parameters (Metafor version > | ||
| + | |||
| + | ^ | ||
| + | | Density | '' | ||
| + | | Young' | ||
| + | | Poisson Ratio | '' | ||
| + | | Material Stiffness | ||
| + | | Thermal Expansion | ||
| + | | Number of the material law which defines the yield stress $\sigma_{yield}$ | ||
| + | | Array of numbers defining the kinematic hardening laws ([1, 2, | ||
| + | | Conductivity | ||
| + | | Heat Capacity | ||
| + | | Heat Capacity Type : \\ - ENTHALPY_CONSISTENT (default) necessary \\ for high variation of the Heat capacity (phase change) \\ - POINT_WISE for slow variation of Heat Capacity | '' | ||
| + | | Dissipated thermoelastic power fraction | ||
| + | | Dissipated (visco)plastic power fraction (Taylor-Quinney factor) | ||
| ===== EvpIsoHDamageHypoMaterial ===== | ===== EvpIsoHDamageHypoMaterial ===== | ||
| Line 440: | Line 474: | ||
| :!: Thermomechanical calculation method : | :!: Thermomechanical calculation method : | ||
| * When the thermal expansion changes, an average value is computed over the time step is estimated to model this thermal expansion properly. | * When the thermal expansion changes, an average value is computed over the time step is estimated to model this thermal expansion properly. | ||
| - | * If the heat capacity changes, | + | * Heat Capacity Type allows to manage varying Heat Capacity : |
| + | * POINT_WISE : compute | ||
| + | * ENTHALPY_CONSISTENT (default) : an average value is computed to estimate properly the energy balance. An equivalent heat capacity can be used to take into account the latent heat (= heat capacity + latent heat). Needed for fast variation of HeatCapacity (ex: solid phase changes). | ||
| ---- | ---- | ||
| Line 457: | Line 493: | ||
| | Conductivity | | Conductivity | ||
| | Heat Capacity | | Heat Capacity | ||
| + | | Heat Capacity Type \\ - ENTHALPY_CONSISTENT (default) necessary \\ for high variation of the Heat capacity (phase change) \\ - POINT_WISE for slow variation of Heat Capacity | '' | ||
| | Dissipated thermoelastic power fraction | | Dissipated thermoelastic power fraction | ||
| | Dissipated (visco)plastic power fraction (Taylor-Quinney factor) | | Dissipated (visco)plastic power fraction (Taylor-Quinney factor) | ||
doc/user/elements/volumes/iso_hypo_materials.1753175657.txt.gz · Last modified: by papeleux
